diff --git a/.gitignore b/.gitignore index 11e955a8..21f7033f 100644 --- a/.gitignore +++ b/.gitignore @@ -56,3 +56,8 @@ saskit/saskit_* /examples/dll/libsasfit_fuzzysphere.dll /examples/dll/libsasfit.dll /src/fftw/fftw-3.3.7.tar.gz +/src/plugins/magcylshell/include +/src/plugins/magcylshell/include/private.h +/src/plugins/sin2 +/src/plugins/sin2/include/private.h +/src/plugins/sin2/include/sasfit_sin2.h diff --git a/CHANGES.txt b/CHANGES.txt index 48b5f031..732899f5 100644 Binary files a/CHANGES.txt and b/CHANGES.txt differ diff --git a/data/rotational_ellipsoid.sas b/data/rotational_ellipsoid.sas index a2087cb8..2851304d 100644 --- a/data/rotational_ellipsoid.sas +++ b/data/rotational_ellipsoid.sas @@ -113,8 +113,8 @@ set sasfit(export,filename) "" set sasfit(Nth,file,Dlambda) "" set sasfit(Nth,file,DI) "" set sasfit(datatypes) { { Ascii ".*" } { BerSANS "D???????.???" } { SESANS "*.ses"} { ALV5000 "*.ASC"} { All "*" } } -set sasfit(SQ,root_menu) ".analytical.fitpar.sq.lay.wrl.whichsq.menu" set sasfit(FF,root_menu) ".analytical.fitpar.ff.lay.wrl.whichff.menu" +set sasfit(SQ,root_menu) ".analytical.fitpar.sq.lay.wrl.whichsq.menu" set sasfit(Nth,hide) "" set sasfit(print,ipady1) "0" set sasfit(print,file) "sasfit.ps" @@ -311,68 +311,69 @@ set addsasfit(file,lastskip) "" set addsasfit(file,r1) "" set addsasfit(Nth,file,l1) "" set ::ask4dataset_var(simorfit) "simulate" -set ::ask4dataset_var(datasetlabel) {1 2 3 4 5 6} set ::ask4dataset_var(go_on) "1" -set ::ask4dataset_var(N_datasets) "6" -set ::ask4dataset_var(dataset) "6" -set ::GlobalAnalytPar(R_lc) {0.0 0.0 0.0 0.0 0.0 0.0} +set ::ask4dataset_var(datasetlabel) {1 2 3 4 5 6 7 8} +set ::ask4dataset_var(N_datasets) "8" +set ::ask4dataset_var(dataset) "8" +set ::GlobalAnalytPar(R_lc) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(P1) "20.0" -set ::GlobalAnalytPar(wR) "3.29166e+010" +set ::GlobalAnalytPar(wR) "3.17525e+010" set ::GlobalAnalytPar(P2) "50.0" -set ::GlobalAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::GlobalAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar(P3) "4.0" set ::GlobalAnalytPar(sumfp) "0.0" set ::GlobalAnalytPar(P4) "0.2" set ::GlobalAnalytPar() "0.0" set ::GlobalAnalytPar(resolution) "no" -set ::GlobalAnalytPar(SD,param_count) "0" -set ::GlobalAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::GlobalAnalytPar(SD,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::GlobalAnalytPar(SD,param_count) {10 10 10 10 10 10 10 10} +set ::GlobalAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(SD,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} set ::GlobalAnalytPar(P5) "1.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(P6) "0.5" -set ::GlobalAnalytPar(fp) {0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(R_li) {0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(fp) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(R_li) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(alpha) "" -set ::GlobalAnalytPar(calcSDFF) {yes yes yes yes yes yes} -set ::GlobalAnalytPar(SD,typestr) {Delta Delta Delta Delta Delta Delta} +set ::GlobalAnalytPar(calcSDFF) {yes yes yes yes yes yes yes yes} +set ::GlobalAnalytPar(SD,typestr) {Delta Delta Delta Delta Delta Delta Delta Delta} set ::GlobalAnalytPar(P7) "0.0" set ::GlobalAnalytPar(sumR_RG) "0.0" -set ::GlobalAnalytPar(SD,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(SD,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar(par_w) ".obW.tab.analytpar" set ::GlobalAnalytPar(mom_descr) {moments of_analytical_size distrib.} set ::GlobalAnalytPar(sumR_Ac) "0.0" set ::GlobalAnalytPar(covar) "" -set ::GlobalAnalytPar(SD,a) {{1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(SD,a) {{1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::GlobalAnalytPar(sumR_lc) "0.0" set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(SQ,how) {0 0 0 0 0 0} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SQ,how) {0 0 0 0 0 0 0 0} set ::GlobalAnalytPar(mfit) "0" set ::GlobalAnalytPar(Q) "0" set ::GlobalAnalytPar(error) "0" -set ::GlobalAnalytPar(R) "1.62226e+010" +set ::GlobalAnalytPar(R) "1.56815e+010" set ::GlobalAnalytPar(sumR_li) "0.0" -set ::GlobalAnalytPar(SQ,typestr) {None None None None None None} -set ::GlobalAnalytPar(FF,typestr) {38 39 40 41 36 37} -set ::GlobalAnalytPar(reducedchisq) "1.0835e+021" +set ::GlobalAnalytPar(SQ,typestr) {None None None None None None None None} +set ::GlobalAnalytPar(FF,typestr) {37 38 41 42 39 40 43 44} +set ::GlobalAnalytPar(reducedchisq) "1.00822e+021" set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(SQ,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::GlobalAnalytPar(FF,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SQ,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::GlobalAnalytPar(FF,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::GlobalAnalytPar(ndata) "4008" set ::GlobalAnalytPar(par_text_export) {description;value;error;factor;global_param;description;value;error;factor;global_param;description;value;error;factor;global_param scattering contribution;1;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;1;;;;label;1;;;;;;;; -Delta;;;;;ellipsoidal shell 1;;;;;None;;;; -N;1.0;;;;R_principle;30.0;;;P1;;;;; -;;;;;R_equitorial;10.0;;;P2;;;;; +Delta;;;;;ellipsoidal shell;;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; +;;;;;dummy;0.0;;;;;;;; +;;;;;t;4.0;;;P3;;;;; ;;;;;dummy;0.0;;;;;;;; -;;;;;t;5.0;;;P3;;;;; -;;;;;sigma;0.2;;;P4;;;;; ;;;;;eta_core;1.0;;;P5;;;;; ;;;;;eta_shell;0.5;;;P6;;;;; ;;;;;eta_solv;0.0;;;P7;;;;; @@ -380,12 +381,12 @@ N;1.0;;;;R_principle;30.0;;;P1;;;;; scattering contribution;2;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;2;;;;label;;;;;;;;; -Delta;;;;;ellipsoidal shell 1t;;;;;None;;;; -N;1.0;;;;R_principle;30.0;;;P1;;;;; -;;;;;R_equitorial;10.0;;;P2;;;;; +Delta;;;;;ellipsoidal shell (t);;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; ;;;;;dummy;0.0;;;;;;;; -;;;;;t;5.0;;;P3;;;;; -;;;;;sigma;0.2;;;P4;;;;; +;;;;;t;4.0;;;P3;;;;; +;;;;;sigma;0.0;;;;;;;; ;;;;;eta_core;1.0;;;P5;;;;; ;;;;;eta_shell;0.5;;;P6;;;;; ;;;;;eta_solv;0.0;;;P7;;;;; @@ -393,11 +394,11 @@ N;1.0;;;;R_principle;30.0;;;P1;;;;; scattering contribution;3;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;3;;;;label;;;;;;;;; -Delta;;;;;ellipsoidal shell 2;;;;;None;;;; -N;1.0;;;;R_principle;30.0;;;P1;;;;; -;;;;;R_equitorial;10.0;;;P2;;;;; +Delta;;;;;ellipsoidal shell (Rp);;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; ;;;;;dummy;0.0;;;;;;;; -;;;;;t;5.0;;;P3;;;;; +;;;;;t;4.0;;;P3;;;;; ;;;;;sigma;0.2;;;P4;;;;; ;;;;;eta_core;1.0;;;P5;;;;; ;;;;;eta_shell;0.5;;;P6;;;;; @@ -406,11 +407,11 @@ N;1.0;;;;R_principle;30.0;;;P1;;;;; scattering contribution;4;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;4;;;;label;;;;;;;;; -Delta;;;;;ellipsoidal shell 2t;;;;;None;;;; -N;1.0;;;;R_principle;30.0;;;P1;;;;; -;;;;;R_equitorial;10.0;;;P2;;;;; +Delta;;;;;ellipsoidal shell (Rp t);;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; ;;;;;dummy;0.0;;;;;;;; -;;;;;t;5.0;;;P3;;;;; +;;;;;t;4.0;;;P3;;;;; ;;;;;sigma;0.2;;;P4;;;;; ;;;;;eta_core;1.0;;;P5;;;;; ;;;;;eta_shell;0.5;;;P6;;;;; @@ -419,12 +420,12 @@ N;1.0;;;;R_principle;30.0;;;P1;;;;; scattering contribution;5;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;5;;;;label;0;;;;;;;; -Delta;;;;;ellipsoidal shell 0;;;;;None;;;; -N;1.0;;;;R_principle;10.0;;;P1;;;;; -;;;;;R_equitorial;30.0;;;P2;;;;; -;;;;;dummy;0.0;;;;;;;; -;;;;;t;5.0;;;P3;;;;; +Delta;;;;;ellipsoidal shell (Re);;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; ;;;;;dummy;0.0;;;;;;;; +;;;;;t;4.0;;;P3;;;;; +;;;;;sigma;0.0;;;;;;;; ;;;;;eta_core;1.0;;;P5;;;;; ;;;;;eta_shell;0.5;;;P6;;;;; ;;;;;eta_solv;0.0;;;P7;;;;; @@ -432,116 +433,167 @@ N;1.0;;;;R_principle;10.0;;;P1;;;;; scattering contribution;6;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;6;;;;label;;;;;;;;; -Delta;;;;;ellipsoidal shell 0t;;;;;None;;;; -N;1.0;;;;R_principle;20.0;;;P1;;;;; -;;;;;R_equitorial;50.0;;;P2;;;;; +Delta;;;;;ellipsoidal shell (Re t);;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; +;;;;;dummy;0.0;;;;;;;; +;;;;;t;4.0;;;P3;;;;; +;;;;;sigma;0.2;;;P4;;;;; +;;;;;eta_core;1.0;;;P5;;;;; +;;;;;eta_shell;0.5;;;P6;;;;; +;;;;;eta_solv;0.0;;;P7;;;;; +;;;;;;;;;;;;;; +scattering contribution;7;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;7;;;;label;;;;;;;;; +Delta;;;;;ellipsoidal shell (Re Rp);;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; +;;;;;dummy;0.0;;;;;;;; +;;;;;t;4.0;;;P3;;;;; +;;;;;sigma;0.2;;;P4;;;;; +;;;;;eta_core;1.0;;;P5;;;;; +;;;;;eta_shell;0.5;;;P6;;;;; +;;;;;eta_solv;0.0;;;P7;;;;; +;;;;;;;;;;;;;; +scattering contribution;8;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;8;;;;label;;;;;;;;; +Delta;;;;;ellipsoidal shell (Re Rp t);;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; ;;;;;dummy;0.0;;;;;;;; ;;;;;t;4.0;;;P3;;;;; ;;;;;sigma;0.2;;;P4;;;;; ;;;;;eta_core;1.0;;;P5;;;;; ;;;;;eta_shell;0.5;;;P6;;;;; ;;;;;eta_solv;0.0;;;P7;;;;;} -set ::GlobalAnalytPar(ndata) "3006" set ::GlobalAnalytPar(par_x_X) "1.1" -set ::GlobalAnalytPar(mom_text_display) {scattering contribution = 1 calculate = yes - Delta ellipsoidal shell 1 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 2 calculate = yes - Delta ellipsoidal shell 1t - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 3 calculate = yes - Delta ellipsoidal shell 2 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 4 calculate = yes - Delta ellipsoidal shell 2t - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 5 calculate = yes - Delta ellipsoidal shell 0 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 6 calculate = yes - Delta ellipsoidal shell 0t - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - +set ::GlobalAnalytPar(SD,param_count_old) {10 10 10 10 10 10 10 10} +set ::GlobalAnalytPar(mom_text_display) {scattering contribution = 1 calculate = yes + Delta ellipsoidal shell + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 2 calculate = yes + Delta ellipsoidal shell (t) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 3 calculate = yes + Delta ellipsoidal shell (Rp) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 4 calculate = yes + Delta ellipsoidal shell (Rp t) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 5 calculate = yes + Delta ellipsoidal shell (Re) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 6 calculate = yes + Delta ellipsoidal shell (Re t) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 7 calculate = yes + Delta ellipsoidal shell (Re Rp) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 8 calculate = yes + Delta ellipsoidal shell (Re Rp t) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + scattering contribution - of all size distrib. sum N_i = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - sumR_lc = 0.0000e+000 sumlc = 0.0000e+000 - sumR_li = 0.0000e+000 sumli = 0.0000e+000 - sumR_Ac = 0.0000e+000 sumAc = 0.0000e+000 - sumR_VP = 0.0000e+000 sumVP = 0.0000e+000 - sumR_RG = 0.0000e+000 sumRG = 0.0000e+000 - sumfp(Sph.) = 0.0000e+000 } -set ::GlobalAnalytPar(SD,param_count_old) {10 10 10 10 10 10} -set ::GlobalAnalytPar(datalabel) {1 {} {} {} 0 {}} + of all size distrib. sum N_i = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + sumR_lc = 0.0000e+000 sumlc = 0.0000e+000 + sumR_li = 0.0000e+000 sumli = 0.0000e+000 + sumR_Ac = 0.0000e+000 sumAc = 0.0000e+000 + sumR_VP = 0.0000e+000 sumVP = 0.0000e+000 + sumR_RG = 0.0000e+000 sumRG = 0.0000e+000 + sumfp(Sph.) = 0.0000e+000 } +set ::GlobalAnalytPar(datalabel) {1 {} {} {} 0 {} {} {}} set ::GlobalAnalytPar(GraphName) "AnalytPar" set ::GlobalAnalytPar(isGlobal) "1" set ::GlobalAnalytPar(w_MomentsAnalytPar) "" -set ::GlobalAnalytPar(SD,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(SD,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar(mom_text_export) {description;value;description;value scattering contribution;1;calculate;yes -Delta;;ellipsoidal shell 1; +Delta;;ellipsoidal shell; ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -554,7 +606,7 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;2;calculate;yes -Delta;;ellipsoidal shell 1t; +Delta;;ellipsoidal shell (t); ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -567,7 +619,7 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;3;calculate;yes -Delta;;ellipsoidal shell 2; +Delta;;ellipsoidal shell (Rp); ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -580,7 +632,7 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;4;calculate;yes -Delta;;ellipsoidal shell 2t; +Delta;;ellipsoidal shell (Rp t); ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -593,7 +645,7 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;5;calculate;yes -Delta;;ellipsoidal shell 0; +Delta;;ellipsoidal shell (Re); ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -606,7 +658,33 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;6;calculate;yes -Delta;;ellipsoidal shell 0t; +Delta;;ellipsoidal shell (Re t); +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;7;calculate;yes +Delta;;ellipsoidal shell (Re Rp); +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;8;calculate;yes +Delta;;ellipsoidal shell (Re Rp t); ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -631,334 +709,372 @@ sumR_RG;0.0000e+000;sumRG;0.0000e+000 sumfp(Sph.);0.0000e+000;;} set ::GlobalAnalytPar() "0.0" set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(chisq) "3.257e+024" +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(chisq) "4.04094e+024" set ::GlobalAnalytPar(file) "unknown.par" -set ::GlobalAnalytPar(varianceOFfit) "1.0835e+021" +set ::GlobalAnalytPar(varianceOFfit) "1.00822e+021" set ::GlobalAnalytPar(par_descr) {parameters of_analytical_size distrib.} -set ::GlobalAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 1 label = 1 - Delta ellipsoidal shell 1 None - N = 1.0 R_principle = 30.0 P1 - R_equitorial = 10.0 P2 - dummy = 0.0 - t = 5.0 P3 - sigma = 0.2 P4 - eta_core = 1.0 P5 - eta_shell = 0.5 P6 - eta_solv = 0.0 P7 - -scattering contribution = 2 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 2 label - Delta ellipsoidal shell 1t None - N = 1.0 R_principle = 30.0 P1 - R_equitorial = 10.0 P2 - dummy = 0.0 - t = 5.0 P3 - sigma = 0.2 P4 - eta_core = 1.0 P5 - eta_shell = 0.5 P6 - eta_solv = 0.0 P7 - -scattering contribution = 3 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 3 label - Delta ellipsoidal shell 2 None - N = 1.0 R_principle = 30.0 P1 - R_equitorial = 10.0 P2 - dummy = 0.0 - t = 5.0 P3 - sigma = 0.2 P4 - eta_core = 1.0 P5 - eta_shell = 0.5 P6 - eta_solv = 0.0 P7 - -scattering contribution = 4 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 4 label - Delta ellipsoidal shell 2t None - N = 1.0 R_principle = 30.0 P1 - R_equitorial = 10.0 P2 - dummy = 0.0 - t = 5.0 P3 - sigma = 0.2 P4 - eta_core = 1.0 P5 - eta_shell = 0.5 P6 - eta_solv = 0.0 P7 - -scattering contribution = 5 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 5 label = 0 - Delta ellipsoidal shell 0 None - N = 1.0 R_principle = 10.0 P1 - R_equitorial = 30.0 P2 - dummy = 0.0 - t = 5.0 P3 - dummy = 0.0 - eta_core = 1.0 P5 - eta_shell = 0.5 P6 - eta_solv = 0.0 P7 - -scattering contribution = 6 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 6 label - Delta ellipsoidal shell 0t None - N = 1.0 R_principle = 20.0 P1 - R_equitorial = 50.0 P2 - dummy = 0.0 - t = 4.0 P3 - sigma = 0.2 P4 - eta_core = 1.0 P5 - eta_shell = 0.5 P6 - eta_solv = 0.0 P7 } -set ::GlobalAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::GlobalAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::GlobalAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::GlobalAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::GlobalAnalytPar(fitSDFF) {yes yes yes yes yes yes} -set ::GlobalAnalytPar(FF,param_count_old) {8 8 8 8 8 8} -set ::GlobalAnalytPar(SQ,param_count_old) {10 10 10 10 10 10} -set ::GlobalAnalytPar(R_VP) {0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(actual_SD) "6" +set ::GlobalAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 1 label = 1 + Delta ellipsoidal shell None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + dummy = 0.0 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 2 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 2 label + Delta ellipsoidal shell (t) None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + sigma = 0.0 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 3 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 3 label + Delta ellipsoidal shell (Rp) None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + sigma = 0.2 P4 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 4 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 4 label + Delta ellipsoidal shell (Rp t) None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + sigma = 0.2 P4 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 5 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 5 label = 0 + Delta ellipsoidal shell (Re) None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + sigma = 0.0 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 6 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 6 label + Delta ellipsoidal shell (Re t) None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + sigma = 0.2 P4 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 7 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 7 label + Delta ellipsoidal shell (Re Rp) None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + sigma = 0.2 P4 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 8 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 8 label + Delta ellipsoidal shell (Re Rp t) None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + sigma = 0.2 P4 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 } +set ::GlobalAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::GlobalAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::GlobalAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::GlobalAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::GlobalAnalytPar(fitSDFF) {yes yes yes yes yes yes yes yes} +set ::GlobalAnalytPar(SQ,param_count_old) {10 10 10 10 10 10 10 10} +set ::GlobalAnalytPar(FF,param_count_old) {8 0 8 8 8 8 8 8} +set ::GlobalAnalytPar(R_VP) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(actual_SD) "8" set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(SQ,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} -set ::GlobalAnalytPar(FF,common) {{P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 NONE P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SQ,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::GlobalAnalytPar(FF,common) {{P1 P2 NONE P3 NONE P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 NONE P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 NONE P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} set ::GlobalAnalytPar(alambda) "-1" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(fit) "no" -set ::GlobalAnalytPar(max_SD) "6" +set ::GlobalAnalytPar(max_SD) "8" set ::GlobalAnalytPar(common_names) {NONE NEW P1 P2 P3 P4 P5 P6 P7} -set ::GlobalAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::GlobalAnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar(mom_w) ".obW.tab.analytmoments" set ::GlobalAnalytPar(common_i) "7" -set ::GlobalAnalytPar(SQ,param_count) "0" -set ::GlobalAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::GlobalAnalytPar(FF,param_count) "0" -set ::GlobalAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(SQ,param_count) {10 10 10 10 10 10 10 10} +set ::GlobalAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(FF,param_count) {8 8 8 8 8 8 8 8} +set ::GlobalAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(w_AnalytPar) "" -set ::GlobalAnalytPar(SD,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SD,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(sumR_VP) "0.0" -set ::GlobalAnalytPar(FF,l) {{30.0 10.0 0.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {30.0 10.0 0.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {30.0 10.0 0.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {30.0 10.0 0.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 30.0 0.0 5.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(FF,l) {{20.0 50.0 0.0 4.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::GlobalAnalytPar(geometrical/datafile) "yes" -set ::GlobalAnalytPar(substrSDFF) {no no no no no no} +set ::GlobalAnalytPar(substrSDFF) {no no no no no no no no} set ::GlobalAnalytPar(w) "" -set ::GlobalAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::GlobalAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::GlobalAnalytPar(R_RG) {0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::GlobalAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::GlobalAnalytPar(R_RG) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(R_Ac) {0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(old_actual_SD) "6" -set ::GlobalAnalytPar(dataset) {1 2 3 4 5 6} -set ::tmpGlobalAnalytPar(R_lc) {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(wR) "3.65138e+008" +set ::GlobalAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(R_Ac) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(old_actual_SD) "8" +set ::GlobalAnalytPar(dataset) {1 2 3 4 5 6 7 8} +set ::tmpGlobalAnalytPar(R_lc) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(P1) "20.0" -set ::tmpGlobalAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpGlobalAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(wR) "3.29166e+010" set ::tmpGlobalAnalytPar(P2) "50.0" -set ::tmpGlobalAnalytPar(sumfp) "0.0" +set ::tmpGlobalAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar(P3) "4.0" -set ::tmpGlobalAnalytPar(SD,param_count) "0" -set ::tmpGlobalAnalytPar(resolution) "no" -set ::tmpGlobalAnalytPar() "0.0" +set ::tmpGlobalAnalytPar(sumfp) "0.0" set ::tmpGlobalAnalytPar(P4) "0.2" -set ::tmpGlobalAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::tmpGlobalAnalytPar(SD,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::tmpGlobalAnalytPar() "0.0" +set ::tmpGlobalAnalytPar(resolution) "no" +set ::tmpGlobalAnalytPar(SD,param_count) {10 10 10 10 10 10 10 10} +set ::tmpGlobalAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(SD,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} set ::tmpGlobalAnalytPar(P5) "1.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(P6) "0.5" -set ::tmpGlobalAnalytPar(fp) {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(R_li) {0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(fp) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(R_li) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(alpha) "" -set ::tmpGlobalAnalytPar(calcSDFF) {yes yes yes yes yes yes} -set ::tmpGlobalAnalytPar(SD,typestr) {Delta Delta Delta Delta Delta Delta} +set ::tmpGlobalAnalytPar(calcSDFF) {yes yes yes yes yes yes yes yes} +set ::tmpGlobalAnalytPar(SD,typestr) {Delta Delta Delta Delta Delta Delta Delta Delta} set ::tmpGlobalAnalytPar(P7) "0.0" set ::tmpGlobalAnalytPar(sumR_RG) "0.0" -set ::tmpGlobalAnalytPar(SD,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(SD,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar(par_w) ".obW.tab.analytpar" set ::tmpGlobalAnalytPar(mom_descr) {moments of_analytical_size distrib.} set ::tmpGlobalAnalytPar(sumR_Ac) "0.0" set ::tmpGlobalAnalytPar(covar) "" -set ::tmpGlobalAnalytPar(SD,a) {{1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(SD,a) {{1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpGlobalAnalytPar(sumR_lc) "0.0" set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(SQ,how) {0 0 0 0 0 0} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SQ,how) {0 0 0 0 0 0 0 0} set ::tmpGlobalAnalytPar(mfit) "0" set ::tmpGlobalAnalytPar(Q) "0" set ::tmpGlobalAnalytPar(error) "0" -set ::tmpGlobalAnalytPar(R) "2.14227e+008" +set ::tmpGlobalAnalytPar(R) "1.62226e+010" set ::tmpGlobalAnalytPar(sumR_li) "0.0" -set ::tmpGlobalAnalytPar(SQ,typestr) {None None None None None None} -set ::tmpGlobalAnalytPar(FF,typestr) {38 39 40 41 36 37} -set ::tmpGlobalAnalytPar(reducedchisq) "1.33326e+017" +set ::tmpGlobalAnalytPar(SQ,typestr) {None None None None None None None None} +set ::tmpGlobalAnalytPar(FF,typestr) {37 38 41 42 39 40 43 44} +set ::tmpGlobalAnalytPar(reducedchisq) "1.0835e+021" set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(SQ,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::tmpGlobalAnalytPar(FF,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::tmpGlobalAnalytPar(ndata) "2505" +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SQ,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::tmpGlobalAnalytPar(FF,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} set ::tmpGlobalAnalytPar(par_text_export) {description;value;error;factor;global_param;description;value;error;factor;global_param;description;value;error;factor;global_param scattering contribution;1;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;1;;;;label;1;;;;;;;; -Delta;;;;;ellipsoidal shell 1;;;;;None;;;; -N;1.0;;;;R_major;30.0;;;;;;;; -;;;;;R_minor;10;;;;;;;; -;;;;;dummy;0.0;;;;;;;; -;;;;;t;5;;;;;;;; -;;;;;sigma;0.2;;;;;;;; -;;;;;eta_core;1;;;;;;;; -;;;;;eta_shell;0.5;;;;;;;; -;;;;;eta_solv;0.0;;;;;;;; +Delta;;;;;ff_ellipsoidal_shell_1;;;;;None;;;; +N;1.0;;;;;;;;;;;;; ;;;;;;;;;;;;;; scattering contribution;2;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;2;;;;label;;;;;;;;; -Delta;;;;;ellipsoidal shell 1t;;;;;None;;;; -N;1.0;;;;R_major;30.0;;;;;;;; -;;;;;R_minor;10;;;;;;;; -;;;;;dummy;0.0;;;;;;;; -;;;;;t;5;;;;;;;; -;;;;;sigma;0.2;;;;;;;; -;;;;;eta_core;1;;;;;;;; -;;;;;eta_shell;0.5;;;;;;;; -;;;;;eta_solv;0.0;;;;;;;; +Delta;;;;;ff_ellipsoidal_shell_1t;;;;;None;;;; +N;1.0;;;;;;;;;;;;; ;;;;;;;;;;;;;; scattering contribution;3;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;3;;;;label;;;;;;;;; -Delta;;;;;ellipsoidal shell 2;;;;;None;;;; -N;1.0;;;;R_major;30.0;;;;;;;; -;;;;;R_minor;10;;;;;;;; +Delta;;;;;ellipsoidal shell (Re Rp);;;;;None;;;; +N;1.0;;;;R_polar;30.0;;;P1;;;;; +;;;;;R_equatorial;10.0;;;P2;;;;; ;;;;;dummy;0.0;;;;;;;; -;;;;;t;5;;;;;;;; -;;;;;sigma;0.2;;;;;;;; -;;;;;eta_core;1;;;;;;;; -;;;;;eta_shell;0.5;;;;;;;; -;;;;;eta_solv;0.0;;;;;;;; +;;;;;t;5.0;;;P3;;;;; +;;;;;sigma;0.2;;;P4;;;;; +;;;;;eta_core;1.0;;;P5;;;;; +;;;;;eta_shell;0.5;;;P6;;;;; +;;;;;eta_solv;0.0;;;P7;;;;; ;;;;;;;;;;;;;; scattering contribution;4;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;4;;;;label;;;;;;;;; -Delta;;;;;ellipsoidal shell 2t;;;;;None;;;; -N;1.0;;;;R_major;30.0;;;;;;;; -;;;;;R_minor;10;;;;;;;; +Delta;;;;;ellipsoidal shell (Re Rp t);;;;;None;;;; +N;1.0;;;;R_polar;30.0;;;P1;;;;; +;;;;;R_equatorial;10.0;;;P2;;;;; ;;;;;dummy;0.0;;;;;;;; -;;;;;t;5;;;;;;;; -;;;;;sigma;0.2;;;;;;;; -;;;;;eta_core;1;;;;;;;; -;;;;;eta_shell;0.5;;;;;;;; -;;;;;eta_solv;0.0;;;;;;;; +;;;;;t;5.0;;;P3;;;;; +;;;;;sigma;0.2;;;P4;;;;; +;;;;;eta_core;1.0;;;P5;;;;; +;;;;;eta_shell;0.5;;;P6;;;;; +;;;;;eta_solv;0.0;;;P7;;;;; ;;;;;;;;;;;;;; scattering contribution;5;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; dataset;5;;;;label;0;;;;;;;; -Delta;;;;;ellipsoidal shell 2t;;;;;None;;;; -N;1.0;;;;R_major;30.0;;;;;;;; -;;;;;R_minor;10;;;;;;;; +Delta;;;;;ellipsoidal shell;;;;;None;;;; +N;1.0;;;;R_polar;10.0;;;P1;;;;; +;;;;;R_equatorial;30.0;;;P2;;;;; ;;;;;dummy;0.0;;;;;;;; -;;;;;t;5;;;;;;;; -;;;;;sigma;0.0;;;;;;;; -;;;;;eta_core;1;;;;;;;; -;;;;;eta_shell;0.5;;;;;;;; -;;;;;eta_solv;0.0;;;;;;;;} +;;;;;t;5.0;;;P3;;;;; +;;;;;dummy;0.0;;;;;;;; +;;;;;eta_core;1.0;;;P5;;;;; +;;;;;eta_shell;0.5;;;P6;;;;; +;;;;;eta_solv;0.0;;;P7;;;;; +;;;;;;;;;;;;;; +scattering contribution;6;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;6;;;;label;;;;;;;;; +Delta;;;;;ellipsoidal shell (t);;;;;None;;;; +N;1.0;;;;R_polar;20.0;;;P1;;;;; +;;;;;R_equatorial;50.0;;;P2;;;;; +;;;;;dummy;0.0;;;;;;;; +;;;;;t;4.0;;;P3;;;;; +;;;;;sigma;0.2;;;P4;;;;; +;;;;;eta_core;1.0;;;P5;;;;; +;;;;;eta_shell;0.5;;;P6;;;;; +;;;;;eta_solv;0.0;;;P7;;;;;} +set ::tmpGlobalAnalytPar(ndata) "3006" set ::tmpGlobalAnalytPar(par_x_X) "1.1" -set ::tmpGlobalAnalytPar(datalabel) {1 {} {} {} 0 {}} -set ::tmpGlobalAnalytPar(SD,param_count_old) {10 10 10 10 10 10} -set ::tmpGlobalAnalytPar(mom_text_display) {scattering contribution = 1 calculate = yes - Delta ellipsoidal shell 1 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 2 calculate = yes - Delta ellipsoidal shell 1t - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 3 calculate = yes - Delta ellipsoidal shell 2 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 4 calculate = yes - Delta ellipsoidal shell 2t - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - -scattering contribution = 5 calculate = yes - Delta ellipsoidal shell 2t - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - +set ::tmpGlobalAnalytPar(mom_text_display) {scattering contribution = 1 calculate = yes + Delta ff_ellipsoidal_shell_1 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 2 calculate = yes + Delta ff_ellipsoidal_shell_1t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 3 calculate = yes + Delta ellipsoidal shell (Re Rp) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 4 calculate = yes + Delta ellipsoidal shell (Re Rp t) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 5 calculate = yes + Delta ellipsoidal shell + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 6 calculate = yes + Delta ellipsoidal shell (t) + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + scattering contribution - of all size distrib. sum N_i = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - sumR_lc = 0.0000e+000 sumlc = 0.0000e+000 - sumR_li = 0.0000e+000 sumli = 0.0000e+000 - sumR_Ac = 0.0000e+000 sumAc = 0.0000e+000 - sumR_VP = 0.0000e+000 sumVP = 0.0000e+000 - sumR_RG = 0.0000e+000 sumRG = 0.0000e+000 - sumfp(Sph.) = 0.0000e+000 } + of all size distrib. sum N_i = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + sumR_lc = 0.0000e+000 sumlc = 0.0000e+000 + sumR_li = 0.0000e+000 sumli = 0.0000e+000 + sumR_Ac = 0.0000e+000 sumAc = 0.0000e+000 + sumR_VP = 0.0000e+000 sumVP = 0.0000e+000 + sumR_RG = 0.0000e+000 sumRG = 0.0000e+000 + sumfp(Sph.) = 0.0000e+000 } +set ::tmpGlobalAnalytPar(SD,param_count_old) {10 10 10 10 10 10 10 10} +set ::tmpGlobalAnalytPar(datalabel) {1 {} {} {} 0 {} {} {}} set ::tmpGlobalAnalytPar(GraphName) "AnalytPar" -set ::tmpGlobalAnalytPar(SD,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpGlobalAnalytPar(w_MomentsAnalytPar) "" set ::tmpGlobalAnalytPar(isGlobal) "1" +set ::tmpGlobalAnalytPar(w_MomentsAnalytPar) "" +set ::tmpGlobalAnalytPar(SD,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar(mom_text_export) {description;value;description;value scattering contribution;1;calculate;yes -Delta;;ellipsoidal shell 1; +Delta;;ff_ellipsoidal_shell_1; ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -971,7 +1087,7 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;2;calculate;yes -Delta;;ellipsoidal shell 1t; +Delta;;ff_ellipsoidal_shell_1t; ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -984,7 +1100,7 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;3;calculate;yes -Delta;;ellipsoidal shell 2; +Delta;;ellipsoidal shell (Re Rp); ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -997,7 +1113,7 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;4;calculate;yes -Delta;;ellipsoidal shell 2t; +Delta;;ellipsoidal shell (Re Rp t); ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -1010,7 +1126,20 @@ R_RG;0.0000e+000;RG;0.0000e+000 fp;0.0000e+000;; ;;; scattering contribution;5;calculate;yes -Delta;;ellipsoidal shell 2t; +Delta;;ellipsoidal shell; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;6;calculate;yes +Delta;;ellipsoidal shell (t); ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -1034,121 +1163,120 @@ sumR_VP;0.0000e+000;sumVP;0.0000e+000 sumR_RG;0.0000e+000;sumRG;0.0000e+000 sumfp(Sph.);0.0000e+000;;} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar(file) "unknown.par" -set ::tmpGlobalAnalytPar(chisq) "3.33982e+020" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar(varianceOFfit) "1.33326e+017" +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(chisq) "3.257e+024" +set ::tmpGlobalAnalytPar(file) "unknown.par" +set ::tmpGlobalAnalytPar(varianceOFfit) "1.0835e+021" set ::tmpGlobalAnalytPar(par_descr) {parameters of_analytical_size distrib.} -set ::tmpGlobalAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::tmpGlobalAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::tmpGlobalAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 1 label = 1 - Delta ellipsoidal shell 1 None - N = 1.0 R_major = 30.0 - R_minor = 10 - dummy = 0.0 - t = 5 - sigma = 0.2 - eta_core = 1 - eta_shell = 0.5 - eta_solv = 0.0 - -scattering contribution = 2 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 2 label - Delta ellipsoidal shell 1t None - N = 1.0 R_major = 30.0 - R_minor = 10 - dummy = 0.0 - t = 5 - sigma = 0.2 - eta_core = 1 - eta_shell = 0.5 - eta_solv = 0.0 - -scattering contribution = 3 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 3 label - Delta ellipsoidal shell 2 None - N = 1.0 R_major = 30.0 - R_minor = 10 - dummy = 0.0 - t = 5 - sigma = 0.2 - eta_core = 1 - eta_shell = 0.5 - eta_solv = 0.0 - -scattering contribution = 4 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 4 label - Delta ellipsoidal shell 2t None - N = 1.0 R_major = 30.0 - R_minor = 10 - dummy = 0.0 - t = 5 - sigma = 0.2 - eta_core = 1 - eta_shell = 0.5 - eta_solv = 0.0 - -scattering contribution = 5 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 5 label = 0 - Delta ellipsoidal shell 2t None - N = 1.0 R_major = 30.0 - R_minor = 10 - dummy = 0.0 - t = 5 - sigma = 0.0 - eta_core = 1 - eta_shell = 0.5 - eta_solv = 0.0 } -set ::tmpGlobalAnalytPar(fitSDFF) {yes yes yes yes yes yes} -set ::tmpGlobalAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::tmpGlobalAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::tmpGlobalAnalytPar(R_VP) {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(FF,param_count_old) {8 8 8 8 8 8} -set ::tmpGlobalAnalytPar(SQ,param_count_old) {10 10 10 10 10 10} -set ::tmpGlobalAnalytPar(actual_SD) "6" -set ::tmpGlobalAnalytPar(FF,common) {{P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 NONE P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} -set ::tmpGlobalAnalytPar(SQ,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 1 label = 1 + Delta ff_ellipsoidal_shell_1 None + N = 1.0 + +scattering contribution = 2 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 2 label + Delta ff_ellipsoidal_shell_1t None + N = 1.0 + +scattering contribution = 3 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 3 label + Delta ellipsoidal shell (Re Rp) None + N = 1.0 R_polar = 30.0 P1 + R_equatorial = 10.0 P2 + dummy = 0.0 + t = 5.0 P3 + sigma = 0.2 P4 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 4 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 4 label + Delta ellipsoidal shell (Re Rp t) None + N = 1.0 R_polar = 30.0 P1 + R_equatorial = 10.0 P2 + dummy = 0.0 + t = 5.0 P3 + sigma = 0.2 P4 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 5 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 5 label = 0 + Delta ellipsoidal shell None + N = 1.0 R_polar = 10.0 P1 + R_equatorial = 30.0 P2 + dummy = 0.0 + t = 5.0 P3 + dummy = 0.0 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 + +scattering contribution = 6 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 6 label + Delta ellipsoidal shell (t) None + N = 1.0 R_polar = 20.0 P1 + R_equatorial = 50.0 P2 + dummy = 0.0 + t = 4.0 P3 + sigma = 0.2 P4 + eta_core = 1.0 P5 + eta_shell = 0.5 P6 + eta_solv = 0.0 P7 } +set ::tmpGlobalAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpGlobalAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpGlobalAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpGlobalAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpGlobalAnalytPar(fitSDFF) {yes yes yes yes yes yes yes yes} +set ::tmpGlobalAnalytPar(SQ,param_count_old) {10 10 10 10 10 10 10 10} +set ::tmpGlobalAnalytPar(FF,param_count_old) {8 0 8 8 8 8 8 8} +set ::tmpGlobalAnalytPar(R_VP) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(actual_SD) "8" set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SQ,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::tmpGlobalAnalytPar(FF,common) {{P1 P2 NONE P3 NONE P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 NONE P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 NONE P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 NONE P3 P4 P5 P6 P7 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} set ::tmpGlobalAnalytPar(alambda) "-1" +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(fit) "no" -set ::tmpGlobalAnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpGlobalAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(max_SD) "8" set ::tmpGlobalAnalytPar(common_names) {NONE NEW P1 P2 P3 P4 P5 P6 P7} -set ::tmpGlobalAnalytPar(max_SD) "6" +set ::tmpGlobalAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar(mom_w) ".obW.tab.analytmoments" -set ::tmpGlobalAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::tmpGlobalAnalytPar(FF,param_count) "0" -set ::tmpGlobalAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::tmpGlobalAnalytPar(SQ,param_count) "0" set ::tmpGlobalAnalytPar(common_i) "7" -set ::tmpGlobalAnalytPar(SD,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::tmpGlobalAnalytPar(w_AnalytPar) "" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SQ,param_count) {10 10 10 10 10 10 10 10} +set ::tmpGlobalAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(FF,param_count) {8 8 8 8 8 8 8 8} +set ::tmpGlobalAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(FF,l) {{30.0 10.0 0.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {30.0 10.0 0.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {30.0 10.0 0.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {30.0 10.0 0.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 30.0 0.0 5.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(w_AnalytPar) "" +set ::tmpGlobalAnalytPar(SD,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(sumR_VP) "0.0" +set ::tmpGlobalAnalytPar(FF,l) {{20.0 50.0 0.0 4.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {20.0 50.0 0.0 4.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpGlobalAnalytPar(geometrical/datafile) "yes" -set ::tmpGlobalAnalytPar(substrSDFF) {no no no no no no} -set ::tmpGlobalAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpGlobalAnalytPar(substrSDFF) {no no no no no no no no} set ::tmpGlobalAnalytPar(w) "" -set ::tmpGlobalAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::tmpGlobalAnalytPar(R_RG) {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpGlobalAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpGlobalAnalytPar(R_RG) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(R_Ac) {0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(dataset) {1 2 3 4 5 6} -set ::tmpGlobalAnalytPar(old_actual_SD) "6" +set ::tmpGlobalAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(R_Ac) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(old_actual_SD) "8" +set ::tmpGlobalAnalytPar(dataset) {1 2 3 4 5 6 7 8} set ::actualGlobalAnalytPar(SQ,s8,common) "NONE" set ::actualGlobalAnalytPar(P1) "20.0" set ::actualGlobalAnalytPar(SQ,s1,var) "100.0" @@ -1161,46 +1289,46 @@ set ::actualGlobalAnalytPar(sumfp) "0.0" set ::actualGlobalAnalytPar(P4) "0.2" set ::actualGlobalAnalytPar(P5) "1.0" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(fp) "0.0" -set ::actualGlobalAnalytPar(SD,a2,min) "-1e+200" set ::actualGlobalAnalytPar(P6) "0.5" -set ::actualGlobalAnalytPar(FF,l6,var) "1.0" +set ::actualGlobalAnalytPar(SD,a2,min) "-1e+200" +set ::actualGlobalAnalytPar(fp) "0.0" set ::actualGlobalAnalytPar(P7) "0.0" +set ::actualGlobalAnalytPar(FF,l6,var) "1.0" set ::actualGlobalAnalytPar(SD,a10,factor) "1" set ::actualGlobalAnalytPar(SQ,s9,var) "0.0" -set ::actualGlobalAnalytPar(SD,a4,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s4,factor) "1" -set ::actualGlobalAnalytPar(SD,a7,distr) "0" -set ::actualGlobalAnalytPar(SD,a6,factor) "1" +set ::actualGlobalAnalytPar(SD,a4,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s2,min) "-1e+200" -set ::actualGlobalAnalytPar(SQ,s6,common) "NONE" +set ::actualGlobalAnalytPar(SD,a6,factor) "1" +set ::actualGlobalAnalytPar(SD,a7,distr) "0" set ::actualGlobalAnalytPar() "0.0" +set ::actualGlobalAnalytPar(SQ,s6,common) "NONE" set ::actualGlobalAnalytPar(FF,l1,max) "1e+200" -set ::actualGlobalAnalytPar(SD,a8,common) "NONE" -set ::actualGlobalAnalytPar(SQ,s6,active) "0" set ::actualGlobalAnalytPar(SQ,s4,max) "1e+200" +set ::actualGlobalAnalytPar(SQ,s6,active) "0" +set ::actualGlobalAnalytPar(SD,a8,common) "NONE" +set ::actualGlobalAnalytPar(FF,l2,label) {R_equatorial =} set ::actualGlobalAnalytPar(SD,a10,var) "0.0" -set ::actualGlobalAnalytPar(FF,l2,label) {R_minor =} -set ::actualGlobalAnalytPar(SQ,typestr) "None" set ::actualGlobalAnalytPar(FF,l7,min) "-1e+200" +set ::actualGlobalAnalytPar(SQ,typestr) "None" set ::actualGlobalAnalytPar(SD,a8,active) "0" set ::actualGlobalAnalytPar(SD,a4,err) "0.0" set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(SQ,s2,factor) "1" set ::actualGlobalAnalytPar(SQ,s8,limits) "0" -set ::actualGlobalAnalytPar(SD,a10,common) "NONE" set ::actualGlobalAnalytPar(FF,l1,err) "0.0" +set ::actualGlobalAnalytPar(SD,a10,common) "NONE" set ::actualGlobalAnalytPar(SD,a4,factor) "1" -set ::actualGlobalAnalytPar(SD,a6,distr) "0" -set ::actualGlobalAnalytPar(SQ,s4,common) "NONE" set ::actualGlobalAnalytPar(SQ,s4,err) "0.0" +set ::actualGlobalAnalytPar(SQ,s4,common) "NONE" +set ::actualGlobalAnalytPar(SD,a6,distr) "0" set ::actualGlobalAnalytPar(SD,a10,active) "0" -set ::actualGlobalAnalytPar(SD,a6,var) "0.0" set ::actualGlobalAnalytPar(SQ,s4,active) "0" +set ::actualGlobalAnalytPar(SD,a6,var) "0.0" set ::actualGlobalAnalytPar(SD,a6,common) "NONE" -set ::actualGlobalAnalytPar(chisq) "3.33982e+020" +set ::actualGlobalAnalytPar(chisq) "3.257e+024" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(FF,l1,label) {R_major =} +set ::actualGlobalAnalytPar(FF,l1,label) {R_polar =} set ::actualGlobalAnalytPar(SD,a6,active) "0" set ::actualGlobalAnalytPar(FF,l3,var) "0.0" set ::actualGlobalAnalytPar(SQ,s9,distr) "0" @@ -1267,7 +1395,7 @@ set ::actualGlobalAnalytPar(SQ,s10,var) "0.0" set ::actualGlobalAnalytPar(Q) "0" set ::actualGlobalAnalytPar(FF,l3,max) "1e+200" set ::actualGlobalAnalytPar(FF,l5,active) "0" -set ::actualGlobalAnalytPar(R) "2.14227e+008" +set ::actualGlobalAnalytPar(R) "1.62226e+010" set ::actualGlobalAnalytPar(SQ,s6,distr) "0" set ::actualGlobalAnalytPar(SQ,s6,max) "1e+200" set ::actualGlobalAnalytPar(SD,a2,limits) "0" @@ -1322,13 +1450,15 @@ set ::actualGlobalAnalytPar(SQ,s3,err) "0.0" set ::actualGlobalAnalytPar(datalabel,6) "0t" set ::actualGlobalAnalytPar(SQ,s9,active) "0" set ::actualGlobalAnalytPar(SD,a5,label) "" +set ::actualGlobalAnalytPar(datalabel,7) {Re Rp} set ::actualGlobalAnalytPar(SD,a10,min) "-1e+200" +set ::actualGlobalAnalytPar(datalabel,8) {Re Rp t} set ::actualGlobalAnalytPar(SD,a5,var) "0.0" set ::actualGlobalAnalytPar(SQ,s10,max) "1e+200" -set ::actualGlobalAnalytPar(old_actual_SD) "6" +set ::actualGlobalAnalytPar(old_actual_SD) "8" set ::actualGlobalAnalytPar(SQ,s3,distr) "0" set ::actualGlobalAnalytPar(SQ,s10,common) "NONE" -set ::actualGlobalAnalytPar(wR) "3.65138e+008" +set ::actualGlobalAnalytPar(wR) "3.29166e+010" set ::actualGlobalAnalytPar(FF,l8,err) "0.0" set ::actualGlobalAnalytPar(SQ,s5,factor) "1" set ::actualGlobalAnalytPar(FF,l1,limits) "0" @@ -1341,227 +1471,227 @@ set ::actualGlobalAnalytPar(SD,a7,factor) "1" set ::actualGlobalAnalytPar(SQ,s8,label) "" set ::actualGlobalAnalytPar(SQ,s7,common) "NONE" set ::actualGlobalAnalytPar(SQ,s10,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s7,active) "0" -set ::actualGlobalAnalytPar(SD,a6,min) "-1e+200" set ::actualGlobalAnalytPar(SD,a9,common) "NONE" +set ::actualGlobalAnalytPar(SD,a6,min) "-1e+200" +set ::actualGlobalAnalytPar(SQ,s7,active) "0" set ::actualGlobalAnalytPar(SD,a4,label) "" set ::actualGlobalAnalytPar(SD,a9,active) "0" +set ::actualGlobalAnalytPar(datasetlabel) {1 2 3 4 5 6 7 8} set ::actualGlobalAnalytPar(SD,a8,max) "1e+200" -set ::actualGlobalAnalytPar(datasetlabel) {1 2 3 4 5 6} -set ::actualGlobalAnalytPar(SQ,s2,distr) "0" set ::actualGlobalAnalytPar(FF,l3,min) "-1e+200" -set ::actualGlobalAnalytPar(SQ,s3,factor) "1" +set ::actualGlobalAnalytPar(SQ,s2,distr) "0" set ::actualGlobalAnalytPar(SQ,s6,min) "-1e+200" -set ::actualGlobalAnalytPar(error) "0" +set ::actualGlobalAnalytPar(SQ,s3,factor) "1" set ::actualGlobalAnalytPar(SQ,s9,limits) "0" -set ::actualGlobalAnalytPar(FF,typestr) "37" -set ::actualGlobalAnalytPar(FF,l5,max) "1e+200" +set ::actualGlobalAnalytPar(error) "0" set ::actualGlobalAnalytPar(FF,l5,distr) "0" +set ::actualGlobalAnalytPar(FF,l5,max) "1e+200" +set ::actualGlobalAnalytPar(FF,typestr) "44" +set ::actualGlobalAnalytPar(reducedchisq) "1.0835e+021" set ::actualGlobalAnalytPar(SD,a5,factor) "1" -set ::actualGlobalAnalytPar(reducedchisq) "1.33326e+017" -set ::actualGlobalAnalytPar(SQ,s8,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s5,common) "NONE" +set ::actualGlobalAnalytPar(SQ,s8,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s7,label) "" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(SD,a7,common) "NONE" set ::actualGlobalAnalytPar(SQ,s5,active) "0" +set ::actualGlobalAnalytPar(SD,a7,common) "NONE" set ::actualGlobalAnalytPar(SD,a8,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s10,limits) "0" set ::actualGlobalAnalytPar(datalabel) "" -set ::actualGlobalAnalytPar(SD,a7,active) "0" -set ::actualGlobalAnalytPar(SD,a2,var) "0.05" +set ::actualGlobalAnalytPar(SQ,s10,limits) "0" set ::actualGlobalAnalytPar(SD,a3,label) "" -set ::actualGlobalAnalytPar(SQ,s1,distr) "0" +set ::actualGlobalAnalytPar(SD,a2,var) "0.05" +set ::actualGlobalAnalytPar(SD,a7,active) "0" set ::actualGlobalAnalytPar(FF,l5,err) "0.0" +set ::actualGlobalAnalytPar(SQ,s1,distr) "0" set ::actualGlobalAnalytPar(SQ,s1,factor) "1" -set ::actualGlobalAnalytPar(SQ,s8,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s7,limits) "0" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(varianceOFfit) "1.33326e+017" -set ::actualGlobalAnalytPar(SD,a3,factor) "1" -set ::actualGlobalAnalytPar(FF,l4,distr) "0" +set ::actualGlobalAnalytPar(SQ,s7,limits) "0" +set ::actualGlobalAnalytPar(SQ,s8,err) "0.0" +set ::actualGlobalAnalytPar(varianceOFfit) "1.0835e+021" set ::actualGlobalAnalytPar(SQ,s2,var) "0.2" -set ::actualGlobalAnalytPar(SD,a9,limits) "0" +set ::actualGlobalAnalytPar(FF,l4,distr) "0" +set ::actualGlobalAnalytPar(SD,a3,factor) "1" set ::actualGlobalAnalytPar(SQ,s3,common) "NONE" +set ::actualGlobalAnalytPar(SD,a9,limits) "0" set ::actualGlobalAnalytPar(SQ,s6,label) "" -set ::actualGlobalAnalytPar(SD,a5,common) "NONE" set ::actualGlobalAnalytPar(SQ,s3,active) "0" -set ::actualGlobalAnalytPar(SD,a3,min) "-1e+200" +set ::actualGlobalAnalytPar(SD,a5,common) "NONE" set ::actualGlobalAnalytPar(FF,l8,factor) "1" -set ::actualGlobalAnalytPar(actual_SD) "6" +set ::actualGlobalAnalytPar(SD,a3,min) "-1e+200" set ::actualGlobalAnalytPar(FF,l7,var) "0.5" -set ::actualGlobalAnalytPar(SD,a5,active) "0" +set ::actualGlobalAnalytPar(actual_SD) "8" set ::actualGlobalAnalytPar() "0.0" +set ::actualGlobalAnalytPar(SD,a5,active) "0" set ::actualGlobalAnalytPar(SD,a2,label) "" set ::actualGlobalAnalytPar(SD,a5,max) "1e+200" -set ::actualGlobalAnalytPar(SQ,s5,limits) "0" set ::actualGlobalAnalytPar(SQ,s3,min) "-1e+200" -set ::actualGlobalAnalytPar(SD,a1,factor) "1" +set ::actualGlobalAnalytPar(SQ,s5,limits) "0" set ::actualGlobalAnalytPar(FF,l2,max) "1e+200" -set ::actualGlobalAnalytPar(SD,a7,limits) "0" -set ::actualGlobalAnalytPar(FF,l3,distr) "0" +set ::actualGlobalAnalytPar(SD,a1,factor) "1" set ::actualGlobalAnalytPar(SQ,s1,common) "NONE" -set ::actualGlobalAnalytPar(SQ,s5,max) "1e+200" +set ::actualGlobalAnalytPar(FF,l3,distr) "0" +set ::actualGlobalAnalytPar(SD,a7,limits) "0" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(SD,a3,common) "NONE" -set ::actualGlobalAnalytPar(FF,l8,min) "-1e+200" -set ::actualGlobalAnalytPar(SQ,s1,active) "0" +set ::actualGlobalAnalytPar(SQ,s5,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s5,label) "" +set ::actualGlobalAnalytPar(SQ,s1,active) "0" +set ::actualGlobalAnalytPar(FF,l8,min) "-1e+200" +set ::actualGlobalAnalytPar(SD,a3,common) "NONE" set ::actualGlobalAnalytPar(FF,l6,factor) "1" set ::actualGlobalAnalytPar(SD,a5,err) "0.0" set ::actualGlobalAnalytPar(SD,a3,active) "0" set ::actualGlobalAnalytPar(FF,l8,label) {eta_solv =} -set ::actualGlobalAnalytPar(FF,l8,common) "P7" set ::actualGlobalAnalytPar(SD,a1,label) {N =} +set ::actualGlobalAnalytPar(FF,l8,common) "P7" set ::actualGlobalAnalytPar(R_RG) "0.0" -set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l2,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s10,min) "-1e+200" -set ::actualGlobalAnalytPar(SQ,s3,limits) "0" +set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l8,active) "0" +set ::actualGlobalAnalytPar(SQ,s3,limits) "0" +set ::actualGlobalAnalytPar(SQ,s10,min) "-1e+200" set ::actualGlobalAnalytPar(SQ,s5,err) "0.0" -set ::actualGlobalAnalytPar(dataset) "6" +set ::actualGlobalAnalytPar(dataset) "8" set ::actualGlobalAnalytPar(SD,a5,limits) "0" -set ::actualGlobalAnalytPar(SD,a7,var) "0.0" -set ::actualGlobalAnalytPar(R_lc) "0.0" set ::actualGlobalAnalytPar(FF,l2,distr) "0" +set ::actualGlobalAnalytPar(R_lc) "0.0" +set ::actualGlobalAnalytPar(SD,a7,var) "0.0" set ::actualGlobalAnalytPar(SD,a1,common) "NONE" -set ::actualGlobalAnalytPar(FF,l4,factor) "1" set ::actualGlobalAnalytPar(SQ,s4,label) "" +set ::actualGlobalAnalytPar(FF,l4,factor) "1" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(SD,a1,active) "0" set ::actualGlobalAnalytPar(FF,l4,var) "4.0" -set ::actualGlobalAnalytPar(R_li) "0.0" +set ::actualGlobalAnalytPar(SD,a1,active) "0" set ::actualGlobalAnalytPar(SD,typestr) "Delta" -set ::actualGlobalAnalytPar(SQ,s7,var) "0.0" -set ::actualGlobalAnalytPar(sumR_RG) "0.0" -set ::actualGlobalAnalytPar(FF,l6,common) "P5" +set ::actualGlobalAnalytPar(R_li) "0.0" set ::actualGlobalAnalytPar(FF,l7,label) {eta_shell =} +set ::actualGlobalAnalytPar(FF,l6,common) "P5" +set ::actualGlobalAnalytPar(sumR_RG) "0.0" +set ::actualGlobalAnalytPar(SQ,s7,var) "0.0" set ::actualGlobalAnalytPar(SD,a2,max) "1e+200" set ::actualGlobalAnalytPar(plottype) "-1" -set ::actualGlobalAnalytPar(FF,l6,active) "0" set ::actualGlobalAnalytPar(SQ,s1,limits) "0" +set ::actualGlobalAnalytPar(FF,l6,active) "0" set ::actualGlobalAnalytPar(SD,a8,min) "-1e+200" -set ::actualGlobalAnalytPar(SD,a3,limits) "0" -set ::actualGlobalAnalytPar(sumR_lc) "0.0" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(FF,l1,distr) "0" +set ::actualGlobalAnalytPar(sumR_lc) "0.0" +set ::actualGlobalAnalytPar(SD,a3,limits) "0" set ::actualGlobalAnalytPar(SQ,s2,max) "1e+200" -set ::actualGlobalAnalytPar(FF,l2,factor) "1" +set ::actualGlobalAnalytPar(FF,l1,distr) "0" set ::actualGlobalAnalytPar(FF,l5,min) "-1e+200" -set ::actualGlobalAnalytPar(FF,l8,limits) "0" +set ::actualGlobalAnalytPar(FF,l2,factor) "1" set ::actualGlobalAnalytPar(SQ,s3,label) "" -set ::actualGlobalAnalytPar(SD,a2,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s8,min) "-1e+200" +set ::actualGlobalAnalytPar(FF,l8,limits) "0" set ::actualGlobalAnalytPar(sumR_li) "0.0" -set ::actualGlobalAnalytPar(FF,l4,common) "P3" +set ::actualGlobalAnalytPar(SQ,s8,min) "-1e+200" +set ::actualGlobalAnalytPar(SD,a2,err) "0.0" set ::actualGlobalAnalytPar(FF,l7,max) "1e+200" -set ::actualGlobalAnalytPar() "0.0" +set ::actualGlobalAnalytPar(FF,l4,common) "P3" set ::actualGlobalAnalytPar(FF,l6,label) {eta_core =} +set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l4,active) "0" -set ::actualGlobalAnalytPar(SD,param_count_old) "10" set ::actualGlobalAnalytPar(SQ,s2,err) "0.0" +set ::actualGlobalAnalytPar(SD,param_count_old) "10" set ::actualGlobalAnalytPar(SD,a1,limits) "0" set ::actualGlobalAnalytPar(SD,a4,var) "10.0" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(FF,l6,limits) "0" set ::actualGlobalAnalytPar(FF,l7,err) "0.0" +set ::actualGlobalAnalytPar(FF,l6,limits) "0" set ::actualGlobalAnalytPar(SQ,s2,label) "" set ::actualGlobalAnalytPar(FF,l1,var) "20.0" set ::actualGlobalAnalytPar(FF,l2,common) "P2" set ::actualGlobalAnalytPar(SQ,s4,var) "0.0" set ::actualGlobalAnalytPar(FF,l5,label) {sigma =} -set ::actualGlobalAnalytPar(fitSDFF) "yes" set ::actualGlobalAnalytPar(FF,l2,active) "0" -set ::actualGlobalAnalytPar(R_VP) "0.0" +set ::actualGlobalAnalytPar(fitSDFF) "yes" set ::actualGlobalAnalytPar(FF,param_count_old) "8" +set ::actualGlobalAnalytPar(R_VP) "0.0" set ::actualGlobalAnalytPar(SD,a5,min) "-1e+200" -set ::actualGlobalAnalytPar(alambda) "-1" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(max_SD) "6" +set ::actualGlobalAnalytPar(alambda) "-1" set ::actualGlobalAnalytPar(common_names) {NONE NEW P1 P2 P3 P4 P5 P6 P7} +set ::actualGlobalAnalytPar(max_SD) "8" set ::actualGlobalAnalytPar(SD,a7,max) "1e+200" -set ::actualGlobalAnalytPar(SQ,s10,distr) "0" -set ::actualGlobalAnalytPar(SQ,s8,factor) "1" -set ::actualGlobalAnalytPar(FF,l2,min) "-1e+200" set ::actualGlobalAnalytPar(FF,l4,limits) "0" +set ::actualGlobalAnalytPar(FF,l2,min) "-1e+200" +set ::actualGlobalAnalytPar(SQ,s8,factor) "1" +set ::actualGlobalAnalytPar(SQ,s10,distr) "0" set ::actualGlobalAnalytPar(SD,a9,distr) "0" -set ::actualGlobalAnalytPar(SQ,s5,min) "-1e+200" set ::actualGlobalAnalytPar(SQ,s1,label) "" +set ::actualGlobalAnalytPar(SQ,s5,min) "-1e+200" set ::actualGlobalAnalytPar(SQ,param_count) "10" set ::actualGlobalAnalytPar(FF,l4,max) "1e+200" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(SQ,s7,max) "1e+200" -set ::actualGlobalAnalytPar(sumR_VP) "0.0" set ::actualGlobalAnalytPar(FF,l4,label) {t =} +set ::actualGlobalAnalytPar(sumR_VP) "0.0" +set ::actualGlobalAnalytPar(SQ,s7,max) "1e+200" set ::actualGlobalAnalytPar(substrSDFF) "no" set ::actualGlobalAnalytPar(SD,a7,err) "0.0" set ::actualGlobalAnalytPar(SD,a1,var) "1.0" -set ::actualGlobalAnalytPar(SQ,s6,factor) "1" -set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l2,limits) "0" +set ::actualGlobalAnalytPar() "0.0" +set ::actualGlobalAnalytPar(SQ,s6,factor) "1" set ::actualGlobalAnalytPar(FF,l4,err) "0.0" set ::actualGlobalAnalytPar(SD,a8,distr) "0" -set ::actualGlobalAnalytPar(SD,a10,distr) "0" -set ::actualGlobalAnalytPar(SD,a8,factor) "1" set ::actualGlobalAnalytPar(SQ,s7,err) "0.0" +set ::actualGlobalAnalytPar(SD,a8,factor) "1" +set ::actualGlobalAnalytPar(SD,a10,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s8,common) "NONE" -set ::tmpactualGlobalAnalytPar(P1) "10.0" +set ::tmpactualGlobalAnalytPar(P1) "20.0" set ::tmpactualGlobalAnalytPar(SQ,s1,var) "100.0" -set ::tmpactualGlobalAnalytPar(P2) "30.0" +set ::tmpactualGlobalAnalytPar(P2) "50.0" set ::tmpactualGlobalAnalytPar(SD,a9,var) "0.0" set ::tmpactualGlobalAnalytPar(FF,l10,common) "NONE" -set ::tmpactualGlobalAnalytPar(P3) "5.0" +set ::tmpactualGlobalAnalytPar(P3) "4.0" set ::tmpactualGlobalAnalytPar(SQ,s8,active) "0" set ::tmpactualGlobalAnalytPar(sumfp) "0.0" set ::tmpactualGlobalAnalytPar(FF,l3,label) "" set ::tmpactualGlobalAnalytPar(P4) "0.2" -set ::tmpactualGlobalAnalytPar(FF,l10,active) "0" -set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(P5) "1.0" -set ::tmpactualGlobalAnalytPar(fp) "0.0" -set ::tmpactualGlobalAnalytPar(SD,a2,min) "-1e+200" +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l10,active) "0" set ::tmpactualGlobalAnalytPar(P6) "0.5" -set ::tmpactualGlobalAnalytPar(FF,l6,var) "0.2" +set ::tmpactualGlobalAnalytPar(SD,a2,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(fp) "0.0" set ::tmpactualGlobalAnalytPar(P7) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l6,var) "1.0" set ::tmpactualGlobalAnalytPar(SD,a10,factor) "1" set ::tmpactualGlobalAnalytPar(SQ,s9,var) "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s4,factor) "1" set ::tmpactualGlobalAnalytPar(SD,a4,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SD,a7,distr) "0" -set ::tmpactualGlobalAnalytPar(SQ,s2,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s4,factor) "1" set ::tmpactualGlobalAnalytPar(SD,a6,factor) "1" -set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(SQ,s2,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SD,a7,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s6,common) "NONE" +set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(FF,l1,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s4,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s6,active) "0" set ::tmpactualGlobalAnalytPar(SD,a8,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l2,label) {R_minor =} +set ::tmpactualGlobalAnalytPar(SQ,s6,active) "0" +set ::tmpactualGlobalAnalytPar(SQ,s4,max) "1e+200" set ::tmpactualGlobalAnalytPar(SD,a10,var) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l7,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(FF,l2,label) {R_equatorial =} set ::tmpactualGlobalAnalytPar(SQ,typestr) "None" +set ::tmpactualGlobalAnalytPar(FF,l7,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SD,a8,active) "0" set ::tmpactualGlobalAnalytPar(SD,a4,err) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l9,max) "1e+200" set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l9,max) "1e+200" set ::tmpactualGlobalAnalytPar(SQ,s2,factor) "1" set ::tmpactualGlobalAnalytPar(SQ,s8,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l1,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a10,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l10,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l1,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a4,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s4,err) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l10,limits) "0" set ::tmpactualGlobalAnalytPar(SQ,s4,common) "NONE" +set ::tmpactualGlobalAnalytPar(SQ,s4,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a6,distr) "0" set ::tmpactualGlobalAnalytPar(SD,a10,active) "0" set ::tmpactualGlobalAnalytPar(SD,a6,common) "NONE" set ::tmpactualGlobalAnalytPar(SD,a6,var) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s4,active) "0" -set ::tmpactualGlobalAnalytPar(chisq) "3.33982e+020" +set ::tmpactualGlobalAnalytPar(chisq) "3.257e+024" set ::tmpactualGlobalAnalytPar(FF,l9,factor) "1" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l1,label) {R_major =} +set ::tmpactualGlobalAnalytPar(FF,l1,label) {R_polar =} set ::tmpactualGlobalAnalytPar(SD,a6,active) "0" set ::tmpactualGlobalAnalytPar(FF,l9,err) "0.0" set ::tmpactualGlobalAnalytPar(FF,l3,var) "0.0" @@ -1633,7 +1763,7 @@ set ::tmpactualGlobalAnalytPar(Q) "0" set ::tmpactualGlobalAnalytPar(SD,a10,label) "" set ::tmpactualGlobalAnalytPar(FF,l3,max) "1e+200" set ::tmpactualGlobalAnalytPar(FF,l5,active) "0" -set ::tmpactualGlobalAnalytPar(R) "2.14227e+008" +set ::tmpactualGlobalAnalytPar(R) "1.62226e+010" set ::tmpactualGlobalAnalytPar(SQ,s6,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s6,max) "1e+200" set ::tmpactualGlobalAnalytPar(SD,a2,limits) "0" @@ -1670,7 +1800,7 @@ set ::tmpactualGlobalAnalytPar(SQ,s10,factor) "1" set ::tmpactualGlobalAnalytPar(SQ,s3,max) "1e+200" set ::tmpactualGlobalAnalytPar(SQ,s4,distr) "0" set ::tmpactualGlobalAnalytPar(common_i) "7" -set ::tmpactualGlobalAnalytPar(FF,param_count) "10" +set ::tmpactualGlobalAnalytPar(FF,param_count) "8" set ::tmpactualGlobalAnalytPar(FF,l6,min) "-1e+200" set ::tmpactualGlobalAnalytPar(FF,l10,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a3,err) "0.0" @@ -1691,196 +1821,198 @@ set ::tmpactualGlobalAnalytPar(datalabel,5) "0" set ::tmpactualGlobalAnalytPar(SQ,s3,err) "0.0" set ::tmpactualGlobalAnalytPar(datalabel,6) "0t" set ::tmpactualGlobalAnalytPar(SQ,s9,active) "0" +set ::tmpactualGlobalAnalytPar(datalabel,7) {Re Rp} set ::tmpactualGlobalAnalytPar(SD,a10,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SD,a5,label) "" +set ::tmpactualGlobalAnalytPar(datalabel,8) {Re Rp t} set ::tmpactualGlobalAnalytPar(SD,a5,var) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s10,max) "1e+200" -set ::tmpactualGlobalAnalytPar(old_actual_SD) "6" +set ::tmpactualGlobalAnalytPar(old_actual_SD) "8" set ::tmpactualGlobalAnalytPar(SQ,s3,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,l8,err) "0.0" -set ::tmpactualGlobalAnalytPar(wR) "3.65138e+008" set ::tmpactualGlobalAnalytPar(SQ,s10,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l2,var) "30.0" -set ::tmpactualGlobalAnalytPar(FF,l1,limits) "0" +set ::tmpactualGlobalAnalytPar(wR) "3.29166e+010" +set ::tmpactualGlobalAnalytPar(FF,l8,err) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s5,factor) "1" -set ::tmpactualGlobalAnalytPar(SD,param_count) "10" -set ::tmpactualGlobalAnalytPar(SQ,s10,active) "0" +set ::tmpactualGlobalAnalytPar(FF,l1,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l2,var) "50.0" set ::tmpactualGlobalAnalytPar(FF,l6,distr) "0" +set ::tmpactualGlobalAnalytPar(SQ,s10,active) "0" +set ::tmpactualGlobalAnalytPar(SD,param_count) "10" set ::tmpactualGlobalAnalytPar(SQ,s5,var) "0.0" set ::tmpactualGlobalAnalytPar(SD,a7,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s7,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s8,label) "" +set ::tmpactualGlobalAnalytPar(SQ,s7,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s10,err) "0.0" -set ::tmpactualGlobalAnalytPar(SD,a9,common) "NONE" -set ::tmpactualGlobalAnalytPar(SD,a6,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s7,active) "0" +set ::tmpactualGlobalAnalytPar(SD,a6,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SD,a9,common) "NONE" set ::tmpactualGlobalAnalytPar(SD,a4,label) "" set ::tmpactualGlobalAnalytPar(SD,a9,active) "0" -set ::tmpactualGlobalAnalytPar(datasetlabel) {1 2 3 4 5 6} set ::tmpactualGlobalAnalytPar(SD,a8,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s2,distr) "0" +set ::tmpactualGlobalAnalytPar(datasetlabel) {1 2 3 4 5 6 7 8} set ::tmpactualGlobalAnalytPar(FF,l3,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s6,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s2,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s3,factor) "1" -set ::tmpactualGlobalAnalytPar(error) "0" +set ::tmpactualGlobalAnalytPar(SQ,s6,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s9,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l5,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,typestr) "37" +set ::tmpactualGlobalAnalytPar(error) "0" set ::tmpactualGlobalAnalytPar(FF,l5,max) "1e+200" -set ::tmpactualGlobalAnalytPar(reducedchisq) "1.33326e+017" +set ::tmpactualGlobalAnalytPar(FF,typestr) "44" +set ::tmpactualGlobalAnalytPar(FF,l5,distr) "0" set ::tmpactualGlobalAnalytPar(SD,a5,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s5,common) "NONE" +set ::tmpactualGlobalAnalytPar(reducedchisq) "1.0835e+021" set ::tmpactualGlobalAnalytPar(SQ,s8,max) "1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s5,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s7,label) "" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s5,active) "0" set ::tmpactualGlobalAnalytPar(SD,a7,common) "NONE" +set ::tmpactualGlobalAnalytPar(SQ,s5,active) "0" set ::tmpactualGlobalAnalytPar(SD,a8,err) "0.0" -set ::tmpactualGlobalAnalytPar(datalabel) "" set ::tmpactualGlobalAnalytPar(SQ,s10,limits) "0" -set ::tmpactualGlobalAnalytPar(SD,a3,label) "" -set ::tmpactualGlobalAnalytPar(SD,a2,var) "0.05" +set ::tmpactualGlobalAnalytPar(datalabel) "" set ::tmpactualGlobalAnalytPar(SD,a7,active) "0" -set ::tmpactualGlobalAnalytPar(SQ,s1,distr) "0" +set ::tmpactualGlobalAnalytPar(SD,a2,var) "0.05" +set ::tmpactualGlobalAnalytPar(SD,a3,label) "" set ::tmpactualGlobalAnalytPar(FF,l5,err) "0.0" +set ::tmpactualGlobalAnalytPar(SQ,s1,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s1,factor) "1" -set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s7,limits) "0" set ::tmpactualGlobalAnalytPar(SQ,s8,err) "0.0" -set ::tmpactualGlobalAnalytPar(varianceOFfit) "1.33326e+017" -set ::tmpactualGlobalAnalytPar(SQ,s2,var) "0.2" -set ::tmpactualGlobalAnalytPar(FF,l4,distr) "0" +set ::tmpactualGlobalAnalytPar(SQ,s7,limits) "0" +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(varianceOFfit) "1.0835e+021" set ::tmpactualGlobalAnalytPar(SD,a3,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s3,common) "NONE" +set ::tmpactualGlobalAnalytPar(FF,l4,distr) "0" +set ::tmpactualGlobalAnalytPar(SQ,s2,var) "0.2" set ::tmpactualGlobalAnalytPar(SD,a9,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l10,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s3,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s6,label) "" -set ::tmpactualGlobalAnalytPar(SQ,s3,active) "0" +set ::tmpactualGlobalAnalytPar(FF,l10,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SD,a5,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l10,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,l8,factor) "1" +set ::tmpactualGlobalAnalytPar(SQ,s3,active) "0" set ::tmpactualGlobalAnalytPar(SD,a3,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(FF,l8,factor) "1" +set ::tmpactualGlobalAnalytPar(FF,l10,distr) "0" +set ::tmpactualGlobalAnalytPar(actual_SD) "8" set ::tmpactualGlobalAnalytPar(FF,l7,var) "0.5" -set ::tmpactualGlobalAnalytPar(actual_SD) "6" -set ::tmpactualGlobalAnalytPar(FF,l9,label) "" -set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(SD,a5,active) "0" +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l9,label) "" set ::tmpactualGlobalAnalytPar(SD,a2,label) "" set ::tmpactualGlobalAnalytPar(SD,a5,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s3,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s5,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l2,max) "1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s3,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SD,a1,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s1,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l3,distr) "0" +set ::tmpactualGlobalAnalytPar(FF,l2,max) "1e+200" set ::tmpactualGlobalAnalytPar(SD,a7,limits) "0" -set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l3,distr) "0" +set ::tmpactualGlobalAnalytPar(SQ,s1,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s5,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s1,active) "0" -set ::tmpactualGlobalAnalytPar(FF,l8,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s5,label) "" +set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(SD,a3,common) "NONE" +set ::tmpactualGlobalAnalytPar(SQ,s5,label) "" +set ::tmpactualGlobalAnalytPar(FF,l8,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s1,active) "0" set ::tmpactualGlobalAnalytPar(FF,l6,factor) "1" set ::tmpactualGlobalAnalytPar(SD,a5,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a3,active) "0" set ::tmpactualGlobalAnalytPar(FF,l8,label) {eta_solv =} -set ::tmpactualGlobalAnalytPar(FF,l8,common) "P7" set ::tmpactualGlobalAnalytPar(SD,a1,label) {N =} +set ::tmpactualGlobalAnalytPar(FF,l8,common) "P7" set ::tmpactualGlobalAnalytPar(R_RG) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l2,err) "0.0" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l8,active) "0" -set ::tmpactualGlobalAnalytPar(SQ,s3,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l2,err) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s10,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s3,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l8,active) "0" set ::tmpactualGlobalAnalytPar(SQ,s5,err) "0.0" -set ::tmpactualGlobalAnalytPar(dataset) "6" +set ::tmpactualGlobalAnalytPar(dataset) "8" set ::tmpactualGlobalAnalytPar(SD,a5,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l2,distr) "0" -set ::tmpactualGlobalAnalytPar(R_lc) "0.0" set ::tmpactualGlobalAnalytPar(SD,a7,var) "0.0" +set ::tmpactualGlobalAnalytPar(R_lc) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l2,distr) "0" set ::tmpactualGlobalAnalytPar(SD,a1,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l4,factor) "1" set ::tmpactualGlobalAnalytPar(SQ,s4,label) "" +set ::tmpactualGlobalAnalytPar(FF,l4,factor) "1" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l4,var) "5.0" set ::tmpactualGlobalAnalytPar(SD,a1,active) "0" -set ::tmpactualGlobalAnalytPar(SD,typestr) "Delta" +set ::tmpactualGlobalAnalytPar(FF,l4,var) "4.0" set ::tmpactualGlobalAnalytPar(R_li) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l6,common) "P4" -set ::tmpactualGlobalAnalytPar(FF,l7,label) {eta_shell =} -set ::tmpactualGlobalAnalytPar(sumR_RG) "0.0" +set ::tmpactualGlobalAnalytPar(SD,typestr) "Delta" set ::tmpactualGlobalAnalytPar(SQ,s7,var) "0.0" +set ::tmpactualGlobalAnalytPar(sumR_RG) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l7,label) {eta_shell =} +set ::tmpactualGlobalAnalytPar(FF,l6,common) "P5" set ::tmpactualGlobalAnalytPar(SD,a2,max) "1e+200" set ::tmpactualGlobalAnalytPar(plottype) "-1" -set ::tmpactualGlobalAnalytPar(SQ,s1,limits) "0" set ::tmpactualGlobalAnalytPar(FF,l6,active) "0" +set ::tmpactualGlobalAnalytPar(SQ,s1,limits) "0" set ::tmpactualGlobalAnalytPar(SD,a8,min) "-1e+200" -set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(sumR_lc) "0.0" set ::tmpactualGlobalAnalytPar(SD,a3,limits) "0" -set ::tmpactualGlobalAnalytPar(SQ,s2,max) "1e+200" +set ::tmpactualGlobalAnalytPar(sumR_lc) "0.0" +set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(FF,l1,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,l5,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s2,max) "1e+200" set ::tmpactualGlobalAnalytPar(FF,l2,factor) "1" -set ::tmpactualGlobalAnalytPar(FF,l8,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l5,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s3,label) "" -set ::tmpactualGlobalAnalytPar(sumR_li) "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s8,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(FF,l8,limits) "0" set ::tmpactualGlobalAnalytPar(SD,a2,err) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l7,max) "1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s8,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(sumR_li) "0.0" set ::tmpactualGlobalAnalytPar(FF,l4,common) "P3" -set ::tmpactualGlobalAnalytPar(FF,l6,label) {eta_core =} +set ::tmpactualGlobalAnalytPar(FF,l7,max) "1e+200" set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l6,label) {eta_core =} set ::tmpactualGlobalAnalytPar(FF,l4,active) "0" -set ::tmpactualGlobalAnalytPar(SQ,s2,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,param_count_old) "10" +set ::tmpactualGlobalAnalytPar(SQ,s2,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a1,limits) "0" set ::tmpactualGlobalAnalytPar(SD,a4,var) "10.0" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l7,err) "0.0" set ::tmpactualGlobalAnalytPar(FF,l6,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l7,err) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s2,label) "" -set ::tmpactualGlobalAnalytPar(FF,l1,var) "10.0" +set ::tmpactualGlobalAnalytPar(FF,l1,var) "20.0" set ::tmpactualGlobalAnalytPar(FF,l2,common) "P2" set ::tmpactualGlobalAnalytPar(SQ,s4,var) "0.0" set ::tmpactualGlobalAnalytPar(FF,l5,label) {sigma =} -set ::tmpactualGlobalAnalytPar(FF,l2,active) "0" set ::tmpactualGlobalAnalytPar(fitSDFF) "yes" -set ::tmpactualGlobalAnalytPar(FF,param_count_old) "8" +set ::tmpactualGlobalAnalytPar(FF,l2,active) "0" set ::tmpactualGlobalAnalytPar(R_VP) "0.0" +set ::tmpactualGlobalAnalytPar(FF,param_count_old) "8" set ::tmpactualGlobalAnalytPar(SD,a5,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(FF,l9,var) "0.0" -set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(alambda) "-1" +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l9,var) "0.0" +set ::tmpactualGlobalAnalytPar(max_SD) "8" set ::tmpactualGlobalAnalytPar(common_names) {NONE NEW P1 P2 P3 P4 P5 P6 P7} -set ::tmpactualGlobalAnalytPar(max_SD) "6" set ::tmpactualGlobalAnalytPar(SD,a7,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s10,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,l4,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l2,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s8,factor) "1" +set ::tmpactualGlobalAnalytPar(FF,l2,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(FF,l4,limits) "0" +set ::tmpactualGlobalAnalytPar(SQ,s10,distr) "0" set ::tmpactualGlobalAnalytPar(SD,a9,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,l10,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s1,label) "" set ::tmpactualGlobalAnalytPar(SQ,s5,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s1,label) "" +set ::tmpactualGlobalAnalytPar(FF,l10,factor) "1" set ::tmpactualGlobalAnalytPar(SQ,param_count) "10" set ::tmpactualGlobalAnalytPar(FF,l4,max) "1e+200" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l4,label) {t =} -set ::tmpactualGlobalAnalytPar(sumR_VP) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s7,max) "1e+200" +set ::tmpactualGlobalAnalytPar(sumR_VP) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l4,label) {t =} set ::tmpactualGlobalAnalytPar(substrSDFF) "no" set ::tmpactualGlobalAnalytPar(SD,a7,err) "0.0" set ::tmpactualGlobalAnalytPar(FF,l10,label) "" set ::tmpactualGlobalAnalytPar(SD,a1,var) "1.0" -set ::tmpactualGlobalAnalytPar(FF,l2,limits) "0" -set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(SQ,s6,factor) "1" +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l2,limits) "0" set ::tmpactualGlobalAnalytPar(FF,l4,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a8,distr) "0" -set ::tmpactualGlobalAnalytPar(SD,a10,distr) "0" -set ::tmpactualGlobalAnalytPar(SQ,s7,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a8,factor) "1" +set ::tmpactualGlobalAnalytPar(SQ,s7,err) "0.0" +set ::tmpactualGlobalAnalytPar(SD,a10,distr) "0" set ::AnalytPar(R_lc) "26.7406" set ::AnalytPar(wR) "1" set ::AnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} @@ -1888,7 +2020,7 @@ set ::AnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 set ::AnalytPar(sumfp) "0" set ::AnalytPar() "4.46639e-049" set ::AnalytPar(SD,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::AnalytPar(SD,param_count) "10" +set ::AnalytPar(SD,param_count) "0" set ::AnalytPar(resolution) "no" set ::AnalytPar() "6.56021e-019" set ::AnalytPar(fp) "0" @@ -2011,8 +2143,8 @@ set ::AnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+20 set ::AnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} set ::AnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} set ::AnalytPar(fitSDFF) "yes" -set ::AnalytPar(FF,param_count_old) "10" set ::AnalytPar(SQ,param_count_old) "10" +set ::AnalytPar(FF,param_count_old) "8" set ::AnalytPar(R_VP) "1.10583e-010" set ::AnalytPar(actual_SD) "1" set ::AnalytPar() "3.30289e-019" @@ -2025,9 +2157,9 @@ set ::AnalytPar(max_SD) "1" set ::AnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::AnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::AnalytPar(mom_w) ".obW.tab.analytmoments" -set ::AnalytPar(SQ,param_count) "10" +set ::AnalytPar(SQ,param_count) "0" set ::AnalytPar(SQ,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::AnalytPar(FF,param_count) "8" +set ::AnalytPar(FF,param_count) "0" set ::AnalytPar(FF,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::AnalytPar() "6.56021e-019" set ::AnalytPar(w_AnalytPar) "" @@ -2047,17 +2179,17 @@ set ::AnalytPar() "3.30289e-019" set ::AnalytPar(R_Ac) "8.25125e-016" set ::AnalytPar(old_actual_SD) "1" set ::tmpAnalytPar(R_lc) "0.0" -set ::tmpAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar(sumfp) "0.0" -set ::tmpAnalytPar(resolution) "no" -set ::tmpAnalytPar(SD,param_count) "10" -set ::tmpAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpAnalytPar(SD,param_count) "0" +set ::tmpAnalytPar(resolution) "no" set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar(calcSDFF) "yes" -set ::tmpAnalytPar(SD,typestr) "Delta" set ::tmpAnalytPar(fp) "0.0" +set ::tmpAnalytPar(SD,typestr) "Delta" +set ::tmpAnalytPar(calcSDFF) "yes" set ::tmpAnalytPar(alpha) "" set ::tmpAnalytPar(R_li) "0.0" set ::tmpAnalytPar(sumR_RG) "0.0" @@ -2148,7 +2280,7 @@ set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar(file) "unknown.par" set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar(par_descr) {parameters of_analytical_size distrib.} -set ::tmpAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} set ::tmpAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. calculate = yes substract = no fit = yes LogNorm Sphere None @@ -2156,42 +2288,42 @@ set ::tmpAnalytPar(par_text_display) {scattering contribution = 1 approxim s = 0.05 p = 1.0 mu = 10.0 eta = 1.0 } -set ::tmpAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::tmpAnalytPar(fitSDFF) "yes" -set ::tmpAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} set ::tmpAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::tmpAnalytPar(FF,param_count_old) "10" -set ::tmpAnalytPar(SQ,param_count_old) "10" +set ::tmpAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpAnalytPar(fitSDFF) "yes" set ::tmpAnalytPar(R_VP) "0.0" +set ::tmpAnalytPar(SQ,param_count_old) "10" +set ::tmpAnalytPar(FF,param_count_old) "8" set ::tmpAnalytPar(actual_SD) "1" -set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar(alambda) "-1.0" +set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar(fit) "no" -set ::tmpAnalytPar(common_names) "" -set ::tmpAnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar(max_SD) "1" +set ::tmpAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpAnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpAnalytPar(common_names) "" set ::tmpAnalytPar(mom_w) ".obW.tab.analytmoments" -set ::tmpAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::tmpAnalytPar(FF,param_count) "8" +set ::tmpAnalytPar(SQ,param_count) "0" set ::tmpAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::tmpAnalytPar(SQ,param_count) "10" -set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar(w_AnalytPar) "" +set ::tmpAnalytPar(FF,param_count) "0" +set ::tmpAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar(w_AnalytPar) "" +set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar(FF,l) {{30.0 10 0.0 1.0 0.0 1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpAnalytPar(sumR_VP) "0.0" +set ::tmpAnalytPar(FF,l) {{30.0 10 0.0 1.0 0.0 1 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpAnalytPar(geometrical/datafile) "yes" set ::tmpAnalytPar(substrSDFF) "no" -set ::tmpAnalytPar(w) "" set ::tmpAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpAnalytPar(w) "" set ::tmpAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} set ::tmpAnalytPar(R_RG) "0.0" -set ::tmpAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar(R_Ac) "0.0" set ::tmpAnalytPar(old_actual_SD) "1" @@ -2206,43 +2338,43 @@ set ::actualAnalytPar(SD,a2,min) "-1e+200" set ::actualAnalytPar(FF,l6,var) "1" set ::actualAnalytPar(SQ,s9,var) "0.0" set ::actualAnalytPar(SD,a4,max) "1e+200" -set ::actualAnalytPar(SD,a7,distr) "0" set ::actualAnalytPar(SQ,s2,min) "-1e+200" +set ::actualAnalytPar(SD,a7,distr) "0" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l1,max) "1e+200" -set ::actualAnalytPar(SQ,s6,active) "0" set ::actualAnalytPar(SQ,s4,max) "1e+200" -set ::actualAnalytPar(FF,l2,label) {R_equitorial =} +set ::actualAnalytPar(SQ,s6,active) "0" set ::actualAnalytPar(SD,a10,var) "0.0" -set ::actualAnalytPar(SQ,typestr) "None" +set ::actualAnalytPar(FF,l2,label) {R_equitorial =} set ::actualAnalytPar(FF,l7,min) "-1e+200" +set ::actualAnalytPar(SQ,typestr) "None" set ::actualAnalytPar(SD,a8,active) "0" set ::actualAnalytPar(SD,a4,err) "0.0" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(SQ,s8,limits) "0" set ::actualAnalytPar(FF,l1,err) "0.0" -set ::actualAnalytPar(SD,a6,distr) "0" set ::actualAnalytPar(SQ,s4,err) "0.0" +set ::actualAnalytPar(SD,a6,distr) "0" set ::actualAnalytPar(SD,a10,active) "0" -set ::actualAnalytPar(SQ,s4,active) "0" set ::actualAnalytPar(SD,a6,var) "0.0" +set ::actualAnalytPar(SQ,s4,active) "0" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l1,label) {R_principle =} set ::actualAnalytPar(SD,a6,active) "0" set ::actualAnalytPar(FF,l3,var) "0.0" -set ::actualAnalytPar(SQ,s9,distr) "0" set ::actualAnalytPar(SQ,s6,var) "0.0" -set ::actualAnalytPar(SQ,s6,limits) "0" +set ::actualAnalytPar(SQ,s9,distr) "0" set ::actualAnalytPar(SD,a1,max) "1e+200" +set ::actualAnalytPar(SQ,s6,limits) "0" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(SD,a8,limits) "0" -set ::actualAnalytPar(SD,a5,distr) "0" set ::actualAnalytPar(SD,a7,min) "-1e+200" +set ::actualAnalytPar(SD,a5,distr) "0" set ::actualAnalytPar(SQ,s2,active) "0" set ::actualAnalytPar(SQ,s1,max) "1e+200" set ::actualAnalytPar(SD,a9,max) "1e+200" -set ::actualAnalytPar(FF,l4,min) "-1e+200" set ::actualAnalytPar(SD,a4,active) "0" +set ::actualAnalytPar(FF,l4,min) "-1e+200" set ::actualAnalytPar(SQ,s7,min) "-1e+200" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(w_AnalytPar) "" @@ -2391,87 +2523,87 @@ set ::actualAnalytPar(SD,a3,active) "0" set ::actualAnalytPar(FF,l8,label) {eta_solv =} set ::actualAnalytPar(SD,a1,label) {N =} set ::actualAnalytPar(R_RG) "0.0" -set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l2,err) "0.0" -set ::actualAnalytPar(SQ,s10,min) "-1e+200" -set ::actualAnalytPar(SQ,s3,limits) "0" +set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l8,active) "0" +set ::actualAnalytPar(SQ,s3,limits) "0" +set ::actualAnalytPar(SQ,s10,min) "-1e+200" set ::actualAnalytPar(SQ,s5,err) "0.0" set ::actualAnalytPar(SD,a5,limits) "0" -set ::actualAnalytPar(R_lc) "0.0" -set ::actualAnalytPar(FF,l2,distr) "0" set ::actualAnalytPar(SD,a7,var) "0.0" +set ::actualAnalytPar(FF,l2,distr) "0" +set ::actualAnalytPar(R_lc) "0.0" set ::actualAnalytPar(SQ,s4,label) "" set ::actualAnalytPar() "0.0" -set ::actualAnalytPar(FF,l4,var) "1.0" set ::actualAnalytPar(SD,a1,active) "0" -set ::actualAnalytPar(SD,typestr) "Delta" +set ::actualAnalytPar(FF,l4,var) "1.0" set ::actualAnalytPar(R_li) "0.0" -set ::actualAnalytPar(FF,l7,label) {eta_shell =} -set ::actualAnalytPar(SQ,s7,var) "0.0" +set ::actualAnalytPar(SD,typestr) "Delta" set ::actualAnalytPar(sumR_RG) "0.0" +set ::actualAnalytPar(SQ,s7,var) "0.0" +set ::actualAnalytPar(FF,l7,label) {eta_shell =} set ::actualAnalytPar(SD,a2,max) "1e+200" set ::actualAnalytPar(plottype) "-1" -set ::actualAnalytPar(SQ,s1,limits) "0" set ::actualAnalytPar(FF,l6,active) "0" +set ::actualAnalytPar(SQ,s1,limits) "0" set ::actualAnalytPar(SD,a8,min) "-1e+200" -set ::actualAnalytPar(sumR_lc) "0.0" -set ::actualAnalytPar() "0.0" set ::actualAnalytPar(SD,a3,limits) "0" -set ::actualAnalytPar(SQ,s2,max) "1e+200" +set ::actualAnalytPar() "0.0" +set ::actualAnalytPar(sumR_lc) "0.0" set ::actualAnalytPar(FF,l1,distr) "0" +set ::actualAnalytPar(SQ,s2,max) "1e+200" set ::actualAnalytPar(FF,l5,min) "-1e+200" -set ::actualAnalytPar(SQ,s3,label) "" set ::actualAnalytPar(FF,l8,limits) "0" -set ::actualAnalytPar(SQ,s8,min) "-1e+200" -set ::actualAnalytPar(sumR_li) "0.0" +set ::actualAnalytPar(SQ,s3,label) "" set ::actualAnalytPar(SD,a2,err) "0.0" +set ::actualAnalytPar(sumR_li) "0.0" +set ::actualAnalytPar(SQ,s8,min) "-1e+200" set ::actualAnalytPar(FF,l7,max) "1e+200" -set ::actualAnalytPar(FF,l6,label) {eta_core =} set ::actualAnalytPar() "0.0" +set ::actualAnalytPar(FF,l6,label) {eta_core =} set ::actualAnalytPar(FF,l4,active) "0" -set ::actualAnalytPar(SQ,s2,err) "0.0" set ::actualAnalytPar(SD,param_count_old) "10" +set ::actualAnalytPar(SQ,s2,err) "0.0" set ::actualAnalytPar(SD,a1,limits) "0" set ::actualAnalytPar(SD,a4,var) "10.0" set ::actualAnalytPar() "0.0" -set ::actualAnalytPar(FF,l6,limits) "0" set ::actualAnalytPar(FF,l7,err) "0.0" +set ::actualAnalytPar(FF,l6,limits) "0" set ::actualAnalytPar(SQ,s2,label) "" set ::actualAnalytPar(FF,l1,var) "30.0" set ::actualAnalytPar(SQ,s4,var) "0.0" set ::actualAnalytPar(FF,l5,label) "" -set ::actualAnalytPar(fitSDFF) "yes" set ::actualAnalytPar(FF,l2,active) "0" +set ::actualAnalytPar(fitSDFF) "yes" +set ::actualAnalytPar(FF,param_count_old) "8" set ::actualAnalytPar(R_VP) "0.0" -set ::actualAnalytPar(FF,param_count_old) "10" set ::actualAnalytPar(SD,a5,min) "-1e+200" -set ::actualAnalytPar(alambda) "-1.0" set ::actualAnalytPar() "0.0" -set ::actualAnalytPar(common_names) "" +set ::actualAnalytPar(alambda) "-1.0" set ::actualAnalytPar(max_SD) "1" +set ::actualAnalytPar(common_names) "" set ::actualAnalytPar(SD,a7,max) "1e+200" -set ::actualAnalytPar(SQ,s10,distr) "0" -set ::actualAnalytPar(FF,l2,min) "-1e+200" set ::actualAnalytPar(FF,l4,limits) "0" +set ::actualAnalytPar(FF,l2,min) "-1e+200" +set ::actualAnalytPar(SQ,s10,distr) "0" set ::actualAnalytPar(SD,a9,distr) "0" -set ::actualAnalytPar(SQ,s1,label) "" set ::actualAnalytPar(SQ,s5,min) "-1e+200" +set ::actualAnalytPar(SQ,s1,label) "" set ::actualAnalytPar(SQ,param_count) "10" set ::actualAnalytPar(FF,l4,max) "1e+200" set ::actualAnalytPar() "0.0" -set ::actualAnalytPar(FF,l4,label) "" -set ::actualAnalytPar(SQ,s7,max) "1e+200" set ::actualAnalytPar(sumR_VP) "0.0" +set ::actualAnalytPar(SQ,s7,max) "1e+200" +set ::actualAnalytPar(FF,l4,label) "" set ::actualAnalytPar(substrSDFF) "no" set ::actualAnalytPar(SD,a7,err) "0.0" set ::actualAnalytPar(SD,a1,var) "1.0" -set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l2,limits) "0" +set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l4,err) "0.0" set ::actualAnalytPar(SD,a8,distr) "0" -set ::actualAnalytPar(SD,a10,distr) "0" set ::actualAnalytPar(SQ,s7,err) "0.0" +set ::actualAnalytPar(SD,a10,distr) "0" set ::tmpactualAnalytPar(SQ,s1,var) "100.0" set ::tmpactualAnalytPar(SD,a9,var) "0.0" set ::tmpactualAnalytPar(SQ,s8,active) "0" @@ -2484,41 +2616,41 @@ set ::tmpactualAnalytPar(SD,a2,min) "-1e+200" set ::tmpactualAnalytPar(FF,l6,var) "0.0" set ::tmpactualAnalytPar(SQ,s9,var) "0.0" set ::tmpactualAnalytPar(SD,a4,max) "1e+200" -set ::tmpactualAnalytPar(SD,a7,distr) "0" set ::tmpactualAnalytPar(SQ,s2,min) "-1e+200" +set ::tmpactualAnalytPar(SD,a7,distr) "0" set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(FF,l1,max) "1e+200" -set ::tmpactualAnalytPar(SQ,s4,max) "1e+200" set ::tmpactualAnalytPar(SQ,s6,active) "0" -set ::tmpactualAnalytPar(FF,l2,label) {R_equitorial =} +set ::tmpactualAnalytPar(SQ,s4,max) "1e+200" set ::tmpactualAnalytPar(SD,a10,var) "0.0" -set ::tmpactualAnalytPar(FF,l7,min) "-1e+200" +set ::tmpactualAnalytPar(FF,l2,label) {R_equitorial =} set ::tmpactualAnalytPar(SQ,typestr) "None" +set ::tmpactualAnalytPar(FF,l7,min) "-1e+200" set ::tmpactualAnalytPar(SD,a8,active) "0" set ::tmpactualAnalytPar(SD,a4,err) "0.0" -set ::tmpactualAnalytPar(FF,l9,max) "1e+200" set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(FF,l9,max) "1e+200" set ::tmpactualAnalytPar(SQ,s8,limits) "0" set ::tmpactualAnalytPar(FF,l1,err) "0.0" set ::tmpactualAnalytPar(FF,l10,limits) "0" -set ::tmpactualAnalytPar(SD,a6,distr) "0" set ::tmpactualAnalytPar(SQ,s4,err) "0.0" +set ::tmpactualAnalytPar(SD,a6,distr) "0" set ::tmpactualAnalytPar(SD,a10,active) "0" -set ::tmpactualAnalytPar(SD,a6,var) "0.0" set ::tmpactualAnalytPar(SQ,s4,active) "0" +set ::tmpactualAnalytPar(SD,a6,var) "0.0" set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(FF,l1,label) {R_principle =} -set ::tmpactualAnalytPar(SD,a6,active) "0" set ::tmpactualAnalytPar(FF,l9,err) "0.0" +set ::tmpactualAnalytPar(SD,a6,active) "0" set ::tmpactualAnalytPar(FF,l3,var) "0.0" -set ::tmpactualAnalytPar(SQ,s9,distr) "0" set ::tmpactualAnalytPar(SQ,s6,var) "0.0" -set ::tmpactualAnalytPar(SD,a1,max) "1e+200" +set ::tmpactualAnalytPar(SQ,s9,distr) "0" set ::tmpactualAnalytPar(SQ,s6,limits) "0" +set ::tmpactualAnalytPar(SD,a1,max) "1e+200" set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(SD,a8,limits) "0" -set ::tmpactualAnalytPar(SD,a5,distr) "0" set ::tmpactualAnalytPar(SD,a7,min) "-1e+200" +set ::tmpactualAnalytPar(SD,a5,distr) "0" set ::tmpactualAnalytPar(SQ,s2,active) "0" set ::tmpactualAnalytPar(SQ,s1,max) "1e+200" set ::tmpactualAnalytPar(SD,a9,max) "1e+200" @@ -2598,7 +2730,7 @@ set ::tmpactualAnalytPar(FF,l1,active) "0" set ::tmpactualAnalytPar(SD,a6,label) "" set ::tmpactualAnalytPar(SQ,s3,max) "1e+200" set ::tmpactualAnalytPar(SQ,s4,distr) "0" -set ::tmpactualAnalytPar(FF,param_count) "8" +set ::tmpactualAnalytPar(FF,param_count) "10" set ::tmpactualAnalytPar(FF,l6,min) "-1e+200" set ::tmpactualAnalytPar(FF,l10,err) "0.0" set ::tmpactualAnalytPar(SQ,s9,min) "-1e+200" @@ -2662,119 +2794,119 @@ set ::tmpactualAnalytPar(FF,l10,distr) "0" set ::tmpactualAnalytPar(SD,a3,min) "-1e+200" set ::tmpactualAnalytPar(actual_SD) "1" set ::tmpactualAnalytPar(FF,l7,var) "0.0" +set ::tmpactualAnalytPar(SD,a5,active) "0" set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(FF,l9,label) "" -set ::tmpactualAnalytPar(SD,a5,active) "0" set ::tmpactualAnalytPar(SD,a2,label) "" set ::tmpactualAnalytPar(SD,a5,max) "1e+200" -set ::tmpactualAnalytPar(SQ,s5,limits) "0" set ::tmpactualAnalytPar(SQ,s3,min) "-1e+200" +set ::tmpactualAnalytPar(SQ,s5,limits) "0" set ::tmpactualAnalytPar(FF,l2,max) "1e+200" -set ::tmpactualAnalytPar(FF,l3,distr) "0" set ::tmpactualAnalytPar(SD,a7,limits) "0" -set ::tmpactualAnalytPar(SQ,s5,max) "1e+200" +set ::tmpactualAnalytPar(FF,l3,distr) "0" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(SQ,s1,active) "0" -set ::tmpactualAnalytPar(SQ,s5,label) "" +set ::tmpactualAnalytPar(SQ,s5,max) "1e+200" set ::tmpactualAnalytPar(FF,l8,min) "-1e+200" +set ::tmpactualAnalytPar(SQ,s5,label) "" +set ::tmpactualAnalytPar(SQ,s1,active) "0" set ::tmpactualAnalytPar(SD,a5,err) "0.0" set ::tmpactualAnalytPar(SD,a3,active) "0" set ::tmpactualAnalytPar(FF,l8,label) {eta_solv =} set ::tmpactualAnalytPar(SD,a1,label) {N =} set ::tmpactualAnalytPar(R_RG) "0.0" -set ::tmpactualAnalytPar(FF,l2,err) "0.0" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(FF,l8,active) "0" -set ::tmpactualAnalytPar(SQ,s3,limits) "0" +set ::tmpactualAnalytPar(FF,l2,err) "0.0" set ::tmpactualAnalytPar(SQ,s10,min) "-1e+200" +set ::tmpactualAnalytPar(SQ,s3,limits) "0" +set ::tmpactualAnalytPar(FF,l8,active) "0" set ::tmpactualAnalytPar(SQ,s5,err) "0.0" set ::tmpactualAnalytPar(SD,a5,limits) "0" -set ::tmpactualAnalytPar(SD,a7,var) "0.0" -set ::tmpactualAnalytPar(FF,l2,distr) "0" set ::tmpactualAnalytPar(R_lc) "0.0" +set ::tmpactualAnalytPar(FF,l2,distr) "0" +set ::tmpactualAnalytPar(SD,a7,var) "0.0" set ::tmpactualAnalytPar(SQ,s4,label) "" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(SD,a1,active) "0" set ::tmpactualAnalytPar(FF,l4,var) "1.0" -set ::tmpactualAnalytPar(R_li) "0.0" +set ::tmpactualAnalytPar(SD,a1,active) "0" set ::tmpactualAnalytPar(SD,typestr) "Delta" -set ::tmpactualAnalytPar(FF,l7,label) {eta_shell =} -set ::tmpactualAnalytPar(sumR_RG) "0.0" +set ::tmpactualAnalytPar(R_li) "0.0" set ::tmpactualAnalytPar(SQ,s7,var) "0.0" +set ::tmpactualAnalytPar(sumR_RG) "0.0" +set ::tmpactualAnalytPar(FF,l7,label) {eta_shell =} set ::tmpactualAnalytPar(SD,a2,max) "1e+200" set ::tmpactualAnalytPar(plottype) "-1" -set ::tmpactualAnalytPar(FF,l6,active) "0" set ::tmpactualAnalytPar(SQ,s1,limits) "0" +set ::tmpactualAnalytPar(FF,l6,active) "0" set ::tmpactualAnalytPar(SD,a8,min) "-1e+200" -set ::tmpactualAnalytPar(SD,a3,limits) "0" -set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(sumR_lc) "0.0" -set ::tmpactualAnalytPar(FF,l1,distr) "0" +set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(SD,a3,limits) "0" set ::tmpactualAnalytPar(SQ,s2,max) "1e+200" +set ::tmpactualAnalytPar(FF,l1,distr) "0" set ::tmpactualAnalytPar(FF,l5,min) "-1e+200" -set ::tmpactualAnalytPar(FF,l8,limits) "0" set ::tmpactualAnalytPar(SQ,s3,label) "" -set ::tmpactualAnalytPar(SD,a2,err) "0.0" -set ::tmpactualAnalytPar(sumR_li) "0.0" +set ::tmpactualAnalytPar(FF,l8,limits) "0" set ::tmpactualAnalytPar(SQ,s8,min) "-1e+200" +set ::tmpactualAnalytPar(sumR_li) "0.0" +set ::tmpactualAnalytPar(SD,a2,err) "0.0" set ::tmpactualAnalytPar(FF,l7,max) "1e+200" -set ::tmpactualAnalytPar(FF,l6,label) {eta_core =} set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(FF,l6,label) {eta_core =} set ::tmpactualAnalytPar(FF,l4,active) "0" -set ::tmpactualAnalytPar(SD,param_count_old) "10" set ::tmpactualAnalytPar(SQ,s2,err) "0.0" +set ::tmpactualAnalytPar(SD,param_count_old) "10" set ::tmpactualAnalytPar(SD,a1,limits) "0" set ::tmpactualAnalytPar(SD,a4,var) "10.0" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(FF,l7,err) "0.0" set ::tmpactualAnalytPar(FF,l6,limits) "0" +set ::tmpactualAnalytPar(FF,l7,err) "0.0" set ::tmpactualAnalytPar(SQ,s2,label) "" set ::tmpactualAnalytPar(FF,l1,var) "10.0" set ::tmpactualAnalytPar(SQ,s4,var) "0.0" set ::tmpactualAnalytPar(FF,l5,label) "" -set ::tmpactualAnalytPar(FF,l2,active) "0" set ::tmpactualAnalytPar(fitSDFF) "yes" -set ::tmpactualAnalytPar(FF,param_count_old) "10" +set ::tmpactualAnalytPar(FF,l2,active) "0" set ::tmpactualAnalytPar(R_VP) "0.0" +set ::tmpactualAnalytPar(FF,param_count_old) "8" set ::tmpactualAnalytPar(SD,a5,min) "-1e+200" -set ::tmpactualAnalytPar(FF,l9,var) "0.0" -set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(alambda) "-1.0" -set ::tmpactualAnalytPar(common_names) "" +set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(FF,l9,var) "0.0" set ::tmpactualAnalytPar(max_SD) "1" +set ::tmpactualAnalytPar(common_names) "" set ::tmpactualAnalytPar(SD,a7,max) "1e+200" -set ::tmpactualAnalytPar(SQ,s10,distr) "0" -set ::tmpactualAnalytPar(FF,l4,limits) "0" set ::tmpactualAnalytPar(FF,l2,min) "-1e+200" +set ::tmpactualAnalytPar(FF,l4,limits) "0" +set ::tmpactualAnalytPar(SQ,s10,distr) "0" set ::tmpactualAnalytPar(SD,a9,distr) "0" -set ::tmpactualAnalytPar(SQ,s1,label) "" set ::tmpactualAnalytPar(SQ,s5,min) "-1e+200" +set ::tmpactualAnalytPar(SQ,s1,label) "" set ::tmpactualAnalytPar(SQ,param_count) "10" set ::tmpactualAnalytPar(FF,l4,max) "1e+200" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(sumR_VP) "0.0" -set ::tmpactualAnalytPar(FF,l4,label) "" set ::tmpactualAnalytPar(SQ,s7,max) "1e+200" +set ::tmpactualAnalytPar(FF,l4,label) "" +set ::tmpactualAnalytPar(sumR_VP) "0.0" set ::tmpactualAnalytPar(substrSDFF) "no" set ::tmpactualAnalytPar(SD,a7,err) "0.0" set ::tmpactualAnalytPar(FF,l10,label) "" set ::tmpactualAnalytPar(SD,a1,var) "1.0" -set ::tmpactualAnalytPar(FF,l2,limits) "0" set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(FF,l2,limits) "0" set ::tmpactualAnalytPar(FF,l4,err) "0.0" set ::tmpactualAnalytPar(SD,a8,distr) "0" -set ::tmpactualAnalytPar(SD,a10,distr) "0" set ::tmpactualAnalytPar(SQ,s7,err) "0.0" -set ::GlobalAnalytPar(FF,typestr) { ff_ellipsoidal_shell_1 ff_ellipsoidal_shell_1t ff_ellipsoidal_shell_2 ff_ellipsoidal_shell_2t ff_ellipsoidal_shell_0 ff_ellipsoidal_shell_0t } -set ::GlobalAnalytPar(SD,typestr) { Delta Delta Delta Delta Delta Delta } -set ::GlobalAnalytPar(SQ,typestr) { None None None None None None } -set ::tmpGlobalAnalytPar(FF,typestr) { ff_ellipsoidal_shell_1 ff_ellipsoidal_shell_1t ff_ellipsoidal_shell_2 ff_ellipsoidal_shell_2t ff_ellipsoidal_shell_0 ff_ellipsoidal_shell_0t } -set ::tmpGlobalAnalytPar(SD,typestr) { Delta Delta Delta Delta Delta Delta } -set ::tmpGlobalAnalytPar(SQ,typestr) { None None None None None None } -set ::actualGlobalAnalytPar(FF,typestr) { ff_ellipsoidal_shell_0t } +set ::tmpactualAnalytPar(SD,a10,distr) "0" +set ::GlobalAnalytPar(FF,typestr) { ff_ellipsoidal_shell_0 ff_ellipsoidal_shell_0t ff_ellipsoidal_shell_rp ff_ellipsoidal_shell_rp_t ff_ellipsoidal_shell_re ff_ellipsoidal_shell_re_t ff_ellipsoidal_shell_2 ff_ellipsoidal_shell_2t } +set ::GlobalAnalytPar(SD,typestr) { Delta Delta Delta Delta Delta Delta Delta Delta } +set ::GlobalAnalytPar(SQ,typestr) { None None None None None None None None } +set ::tmpGlobalAnalytPar(FF,typestr) { ff_ellipsoidal_shell_0 ff_ellipsoidal_shell_0t ff_ellipsoidal_shell_rp ff_ellipsoidal_shell_rp_t ff_ellipsoidal_shell_re ff_ellipsoidal_shell_re_t ff_ellipsoidal_shell_2 ff_ellipsoidal_shell_2t } +set ::tmpGlobalAnalytPar(SD,typestr) { Delta Delta Delta Delta Delta Delta Delta Delta } +set ::tmpGlobalAnalytPar(SQ,typestr) { None None None None None None None None } +set ::actualGlobalAnalytPar(FF,typestr) { ff_ellipsoidal_shell_2t } set ::actualGlobalAnalytPar(SD,typestr) { Delta } set ::actualGlobalAnalytPar(SQ,typestr) { None } -set ::tmpactualGlobalAnalytPar(FF,typestr) { ff_ellipsoidal_shell_0t } +set ::tmpactualGlobalAnalytPar(FF,typestr) { ff_ellipsoidal_shell_2t } set ::tmpactualGlobalAnalytPar(SD,typestr) { Delta } set ::tmpactualGlobalAnalytPar(SQ,typestr) { None } set ::AnalytPar(FF,typestr) { ff_spheroid_R } @@ -2789,16 +2921,16 @@ set ::actualAnalytPar(SQ,typestr) { None } set ::tmpactualAnalytPar(FF,typestr) { ff_spheroid_R } set ::tmpactualAnalytPar(SD,typestr) { Delta } set ::tmpactualAnalytPar(SQ,typestr) { None } -set ::IQGraph(e,fill) "Black" +set ::IQGraph(e,fill) "" set ::IQGraph(e.resstipples) "" -set ::IQGraph(e,scale) "no" -set ::IQGraph(e,dash) "0" -set ::IQGraph(e,linewidth) "2" +set ::IQGraph(e,scale) "" +set ::IQGraph(e,dash) "" +set ::IQGraph(e,linewidth) "" set ::IQGraph(y,min) "" set ::IQGraph(l,hide) "yes" -set ::IQGraph(e,resoutline) "blue" -set ::IQGraph(e,xdata) {{0.01 0.0106770427203 0.0113999241252 0.0121717476894 0.012995827006 0.013875700013 0.0148151441813 0.0158181927332 0.0168891519571 0.0180326196956 0.019253505085 0.0205570496309 0.0219488497113 0.0234348806031 0.0250215221345 0.0267155860758 0.028524345383 0.0304555654225 0.0325175373088 0.0347191135006 0.0370697458059 0.0395795259602 0.0422592289528 0.0451203592858 0.0481752003651 0.051436867236 0.0549193628879 0.0586376383729 0.0626076569927 0.0668464628332 0.0713722539374 0.0762044604337 0.0813638279531 0.0868725066946 0.0927541465202 0.0990339984885 0.105739023263 0.112898006859 0.120541684227 0.128702871207 0.137416605411 0.146720296646 0.156653887523 0.167260024939 0.178584243168 0.190675159349 0.203584682208 0.217368234914 0.232084993022 0.247798138525 0.264575131105 0.282487997755 0.301613642002 0.322034174069 0.343837263395 0.367116515011 0.391971871412 0.418510041624 0.446844959331 0.477098272015 0.50939986321 0.543888410123 0.580711978999 0.620028660799 0.662007249918 0.706827968856 0.754683241941 0.805778521453 0.860333169669 0.918581400629 0.980773285663 1.047175827 1.11807410406 1.19377249735 1.27459599526 1.36089158926 1.45302976363 1.55140608602 1.6564429057 1.7685911668 1.88833234428 2.016180511 2.15268454479 2.29843048482 2.45404404761 2.6201933134 2.79759159427 2.98700049661 3.1892331908 3.40515790233 3.63570163927 3.88185417209 4.14467228296 4.4252843027 4.72489495496 5.04479052832 5.38634439861 5.75102292504 6.14039174564 6.55612249878 6.99999999993}} -set ::IQGraph(e,element) "1" +set ::IQGraph(e,resoutline) "" +set ::IQGraph(e,xdata) "" +set ::IQGraph(e,element) "0" set ::IQGraph(y,max) "" set ::IQGraph(x,linewidth) "2" set ::IQGraph(colorselection) {black red green blue cyan magenta yellow violet purple orange pink gray} @@ -2807,32 +2939,32 @@ set ::IQGraph(y,titlecolor) "black" set ::IQGraph(y,loose) "no" set ::IQGraph(fit,background) "#cccccc" set ::IQGraph(x,size) "12" -set ::IQGraph(e,dashcolor) "red" -set ::IQGraph(e,outlinewidth) "1" +set ::IQGraph(e,dashcolor) "" +set ::IQGraph(e,outlinewidth) "" set ::IQGraph(x,ticklength) "10" set ::IQGraph(l,posx) "10" -set ::IQGraph(e,errlinewidth) "1" +set ::IQGraph(e,errlinewidth) "" set ::IQGraph(l,posy) "10" -set ::IQGraph(e,linehide) "1" +set ::IQGraph(e,linehide) "" set ::IQGraph(graph,fg) "black" -set ::IQGraph(e,elementname) "graph1" +set ::IQGraph(e,elementname) "" set ::IQGraph(dashnames) {{-} {..} {--} {.-} {..-} {--.}} -set ::IQGraph(e,reshide) "no" +set ::IQGraph(e,reshide) "" set ::IQGraph(graph,relief) "flat" -set ::IQGraph(e,pixels) "4" +set ::IQGraph(e,pixels) "" set ::IQGraph(dashpattern) {{0} {2 2} {8 2 8 2} {2 2 8 2} {2 2 2 2 8 2} {8 2 8 2 2 2} } set ::IQGraph(x,tickcolor) "black" set ::IQGraph(x,logscale) "1" set ::IQGraph(e,resstipples) "hline1" set ::IQGraph(y,title) "I(Q)" set ::IQGraph(l,bg) "white" -set ::IQGraph(e,errtags) "{}" -set ::IQGraph(e,symbolhide) "no" +set ::IQGraph(e,errtags) "" +set ::IQGraph(e,symbolhide) "" set ::IQGraph(c,hide) "yes" set ::IQGraph(plot,borderwidth) "0" set ::IQGraph(y,rot) "0" -set ::IQGraph(e,smooth) "linear" -set ::IQGraph(e,offdashcolor) "White" +set ::IQGraph(e,smooth) "" +set ::IQGraph(e,offdashcolor) "" set ::IQGraph(g,dash) "0" set ::IQGraph(y,color) "Black" set ::IQGraph(x,subticks) "5" @@ -2842,16 +2974,16 @@ set ::IQGraph(l,pady) {0 0} set ::IQGraph(y,titlefont) {Helvetica 10} set ::IQGraph(x,loose) "no" set ::IQGraph(x,type) "log10(x)" -set ::IQGraph(c,x) "123" +set ::IQGraph(c,x) "413" set ::IQGraph(y,logscale) "1" +set ::IQGraph(c,y) "0" set ::IQGraph(e.errstipples) "" -set ::IQGraph(c,y) "19" set ::IQGraph(e,restags) "" set ::IQGraph(title) "unknown" set ::IQGraph(l,anchor) "n" set ::IQGraph(GraphName) "IQGraph" set ::IQGraph(symbolselection) {square circle diamond plus cross splus scross triangle} -set ::IQGraph(e,errorhide) "no" +set ::IQGraph(e,errorhide) "" set ::IQGraph(y,subticks) "5" set ::IQGraph(l,ipadx) {0 0} set ::IQGraph(c,color) "black" @@ -2866,41 +2998,41 @@ set ::IQGraph(margin,plotpady) {5 5} set ::IQGraph(fitrange) "no" set ::IQGraph(margin,right) "0" set ::IQGraph(x,min) "" -set ::IQGraph(e,errfill) "Black" +set ::IQGraph(e,errfill) "" set ::IQGraph(height) "512" -set ::IQGraph(e,erroutline) "blue" -set ::IQGraph(e,errdash) "0" +set ::IQGraph(e,erroutline) "" +set ::IQGraph(e,errdash) "" set ::IQGraph(y,ticklength) "10" set ::IQGraph(g,color) "black" set ::IQGraph(x,max) "" set ::IQGraph(g,linewidth) "1" set ::IQGraph(x,color) "Black" -set ::IQGraph(l,legendtext) "Fit" -set ::IQGraph(e,ydata) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::IQGraph(l,legendtext) "" +set ::IQGraph(e,ydata) "" set ::IQGraph(y,mapped) "1" set ::IQGraph(margin,top) "0" set ::IQGraph(l,borderwidth) "2" set ::IQGraph(e,errstipples) "hline1" -set ::IQGraph(e,symbol) "none" +set ::IQGraph(e,symbol) "" set ::IQGraph(y,tickfont) {Helvetica 10} set ::IQGraph(font) {Helvetica 10} set ::IQGraph(graph,bg) "white" set ::IQGraph(margin,bottom) "0" -set ::IQGraph(e,outline) "Black" -set ::IQGraph(e,resfill) "Black" +set ::IQGraph(e,outline) "" +set ::IQGraph(e,resfill) "" set ::IQGraph(plot,relief) "flat" -set ::IQGraph(e,resdash) "0" +set ::IQGraph(e,resdash) "" set ::IQGraph(x,showticks) "yes" set ::IQGraph(x,mapped) "1" set ::IQGraph(y,factor) "1.0" set ::IQGraph(stipples) {bdiagonal1 bdiagonal2 checker2 checker3 cross1 cross2 cross3 crossdiag dot1 dot2 dot3 dot4 fdiagonal1 fdiagonal2 hline1 hline2 lbottom ltop rbottom rtop vline1 vline2} set ::IQGraph(graph,borderwidth) "0" -set ::IQGraph(e,resdata) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::IQGraph(e,resdata) "" set ::IQGraph(x,titlecolor) "black" set ::IQGraph(c,dash) "0" set ::IQGraph(y,size) "12" set ::IQGraph(x,rot) "0" -set ::IQGraph(e,error) {{-1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0}} +set ::IQGraph(e,error) "" set ::IQGraph(x,factor) "1.0" set ::IQGraph(x,stepsize) "0" set ::IQGraph(plot,background) "gray90" @@ -2913,23 +3045,23 @@ set ::IQGraph(upper,x) "" set ::IQGraph(width) "768" set ::IQGraph(g,minor) "no" set ::IQGraph(upper,y) "" -set ::IQGraph(e,reslinewidth) "1" +set ::IQGraph(e,reslinewidth) "" set ::IQGraph(y,stepsize) "0" set ::IQGraph(y,showticks) "yes" set ::IQGraph(lower,x) "" set ::IQGraph(l,position) "right" set ::IQGraph(lower,y) "" set ::IQGraph(y,type) "log10(y)" -set ::GlobalFitIQGraph(e,fill) "" +set ::GlobalFitIQGraph(e,fill) {Black Black Black Black Black Black Black Black} set ::GlobalFitIQGraph(e.resstipples) "" -set ::GlobalFitIQGraph(e,scale) "" -set ::GlobalFitIQGraph(e,dash) "" -set ::GlobalFitIQGraph(e,linewidth) "" +set ::GlobalFitIQGraph(e,scale) {no no no no no no no no} +set ::GlobalFitIQGraph(e,dash) {0 0 0 0 0 0 0 0} +set ::GlobalFitIQGraph(e,linewidth) {2 2 2 2 2 2 2 2} set ::GlobalFitIQGraph(y,min) "" set ::GlobalFitIQGraph(l,hide) "no" -set ::GlobalFitIQGraph(e,resoutline) "" -set ::GlobalFitIQGraph(e,xdata) "" -set ::GlobalFitIQGraph(e,element) "0" +set ::GlobalFitIQGraph(e,resoutline) {blue blue blue blue blue blue blue blue} +set ::GlobalFitIQGraph(e,xdata) {{0.01 0.0101318837008 0.0102655067326 0.0104008920344 0.0105380628476 0.0106770427203 0.0108178555111 0.010960525393 0.0111050768581 0.0112515347214 0.0113999241252 0.0115502705434 0.0117025997858 0.0118569380026 0.012013311689 0.0121717476894 0.0123322732023 0.0124949157852 0.0126597033587 0.0128266642116 0.012995827006 0.013167220782 0.0133408749626 0.0135168193587 0.0136950841747 0.013875700013 0.0140586978798 0.0142441091902 0.0144319657736 0.0146222998792 0.0148151441813 0.0150105317855 0.0152084962337 0.0154090715104 0.015612292048 0.0158181927332 0.0160268089129 0.0162381764 0.0164523314797 0.0166693109158 0.0168891519571 0.0171118923434 0.0173375703123 0.0175662246058 0.0177978944767 0.0180326196956 0.0182704405576 0.0185113978891 0.0187555330551 0.019002887966 0.019253505085 0.0195074274353 0.0197646986076 0.0200253627672 0.0202894646623 0.0205570496309 0.0208281636091 0.0211028531388 0.0213811653756 0.0216631480972 0.0219488497113 0.0222383192641 0.0225316064484 0.0228287616126 0.0231298357691 0.0234348806031 0.0237439484811 0.0240570924607 0.0243743662991 0.0246958244622 0.0250215221345 0.0253515152283 0.0256858603931 0.0260246150256 0.0263678372797 0.0267155860758 0.0270679211118 0.0274249028726 0.0277865926409 0.0281530525078 0.028524345383 0.0289005350061 0.0292816859572 0.029667863668 0.0300591344334 0.0304555654225 0.0308572246901 0.0312641811888 0.0316765047805 0.0320942662482 0.0325175373088 0.0329463906248 0.033380899817 0.0338211394772 0.034267185181 0.0347191135006 0.0351770020182 0.0356409293389 0.0361109751049 0.0365872200084 0.0370697458059 0.0375586353322 0.0380539725145 0.0385558423868 0.0390643311048 0.0395795259602 0.0401015153959 0.0406303890216 0.0411662376283 0.0417091532048 0.0422592289528 0.0428165593033 0.0433812399328 0.0439533677793 0.0445330410597 0.0451203592858 0.045715423282 0.0463183352024 0.0469291985483 0.0475481181861 0.0481752003651 0.048810552736 0.0494542843691 0.0501065057732 0.0507673289145 0.051436867236 0.0521152356766 0.0528025506913 0.0534989302707 0.0542044939618 0.0549193628879 0.05564365977 0.0563775089474 0.0571210363993 0.0578743697665 0.0586376383729 0.0594109732481 0.0601945071498 0.0609883745866 0.061792711841 0.0626076569927 0.0634333499427 0.0642699324369 0.0651175480906 0.0659763424132 0.0668464628332 0.0677280587233 0.0686212814262 0.0695262842807 0.0704432226478 0.0713722539374 0.0723135376354 0.0732672353312 0.0742335107452 0.0752125297569 0.0762044604337 0.0772094730593 0.0782277401633 0.0792594365508 0.080304739332 0.0813638279531 0.0824368842269 0.083524092364 0.0846256390043 0.0857417132494 0.0868725066946 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1.6564429057 1.67828868775 1.70042258006 1.72284838233 1.74556994438 1.7685911668 1.79191600162 1.81554845299 1.83949257788 1.86375248675 1.88833234428 1.91323637006 1.93846883935 1.96403408378 1.98993649212 2.016180511 2.04277064572 2.06971146098 2.09700758167 2.12466369371 2.15268454479 2.18107494522 2.20983976876 2.23898395344 2.26851250241 2.29843048482 2.32874303664 2.35945536162 2.39057273211 2.42210048999 2.45404404761 2.48640888869 2.51920056928 2.55242471868 2.58608704046 2.6201933134 2.65474939248 2.68976120993 2.72523477618 2.76117618095 2.79759159427 2.83448726754 2.87186953459 2.90974481283 2.94811960424 2.98700049661 3.02639416458 3.06630737081 3.10674696718 3.14771989592 3.1892331908 3.23129397838 3.27390947919 3.31708700899 3.36083398004 3.40515790233 3.45006638491 3.49556713718 3.54166797021 3.58837679809 3.63570163927 3.68365061797 3.73223196555 3.78145402192 3.83132523699 3.88185417209 3.93304950149 3.98492001384 4.03747461371 4.09072232308 4.14467228296 4.19933375487 4.2547161225 4.31082889329 4.36768170006 4.4252843027 4.48364658977 4.54277858028 4.60269042537 4.66339241005 4.72489495496 4.78720861819 4.85034409708 4.91431223002 4.97912399838 5.04479052832 5.11132309276 5.17873311329 5.24703216211 5.31623196406 5.38634439861 5.45738150189 5.52935546878 5.60227865498 5.67616357915 5.75102292504 5.82686954369 5.90371645562 5.98157685305 6.06046410223 6.14039174564 6.22137350439 6.30342328054 6.38655515951 6.47078341246 6.55612249878 6.64258706856 6.73019196508 6.81895222739 6.90888309289 6.99999999993}} +set ::GlobalFitIQGraph(e,element) "8" set ::GlobalFitIQGraph(y,max) "" set ::GlobalFitIQGraph(x,linewidth) "2" set ::GlobalFitIQGraph(colorselection) {black red green blue cyan magenta yellow violet purple orange pink gray} @@ -2938,32 +3070,32 @@ set ::GlobalFitIQGraph(y,titlecolor) "black" set ::GlobalFitIQGraph(y,loose) "no" set ::GlobalFitIQGraph(fit,background) "#cccccc" set ::GlobalFitIQGraph(x,size) "12" -set ::GlobalFitIQGraph(e,dashcolor) "" -set ::GlobalFitIQGraph(e,outlinewidth) "" +set ::GlobalFitIQGraph(e,dashcolor) {black red green blue cyan magenta yellow violet} +set ::GlobalFitIQGraph(e,outlinewidth) {1 1 1 1 1 1 1 1} set ::GlobalFitIQGraph(x,ticklength) "10" set ::GlobalFitIQGraph(l,posx) "10" -set ::GlobalFitIQGraph(e,errlinewidth) "" +set ::GlobalFitIQGraph(e,errlinewidth) {1 1 1 1 1 1 1 1} set ::GlobalFitIQGraph(l,posy) "10" -set ::GlobalFitIQGraph(e,linehide) "" +set ::GlobalFitIQGraph(e,linehide) {1 1 1 1 1 1 1 1} set ::GlobalFitIQGraph(graph,fg) "black" -set ::GlobalFitIQGraph(e,elementname) "" +set ::GlobalFitIQGraph(e,elementname) {graph1 graph2 graph3 graph4 graph5 graph6 graph7 graph8} set ::GlobalFitIQGraph(dashnames) {{-} {..} {--} {.-} {..-} {--.}} -set ::GlobalFitIQGraph(e,reshide) "" +set ::GlobalFitIQGraph(e,reshide) {no no no no no no no no} set ::GlobalFitIQGraph(graph,relief) "flat" -set ::GlobalFitIQGraph(e,pixels) "" +set ::GlobalFitIQGraph(e,pixels) {4 4 4 4 4 4 4 4} set ::GlobalFitIQGraph(dashpattern) {{0} {2 2} {8 2 8 2} {2 2 8 2} {2 2 2 2 8 2} {8 2 8 2 2 2} } set ::GlobalFitIQGraph(x,tickcolor) "black" set ::GlobalFitIQGraph(x,logscale) "1" -set ::GlobalFitIQGraph(e,resstipples) {hline1 hline1 hline1 hline1 hline1 hline1} +set ::GlobalFitIQGraph(e,resstipples) {hline1 hline1 hline1 hline1 hline1 hline1 hline1 hline1} set ::GlobalFitIQGraph(y,title) "I(Q)" set ::GlobalFitIQGraph(l,bg) "white" -set ::GlobalFitIQGraph(e,errtags) "" -set ::GlobalFitIQGraph(e,symbolhide) "" +set ::GlobalFitIQGraph(e,errtags) {{} {} {} {} {} {} {} {}} +set ::GlobalFitIQGraph(e,symbolhide) {no no no no no no no no} set ::GlobalFitIQGraph(c,hide) "yes" set ::GlobalFitIQGraph(plot,borderwidth) "0" set ::GlobalFitIQGraph(y,rot) "0" -set ::GlobalFitIQGraph(e,smooth) "" -set ::GlobalFitIQGraph(e,offdashcolor) "" +set ::GlobalFitIQGraph(e,smooth) {linear linear linear linear linear linear linear linear} +set ::GlobalFitIQGraph(e,offdashcolor) {White White White White White White White White} set ::GlobalFitIQGraph(g,dash) "0" set ::GlobalFitIQGraph(y,color) "Black" set ::GlobalFitIQGraph(x,subticks) "5" @@ -2973,16 +3105,16 @@ set ::GlobalFitIQGraph(l,pady) {0 0} set ::GlobalFitIQGraph(y,titlefont) {Helvetica 10} set ::GlobalFitIQGraph(x,loose) "no" set ::GlobalFitIQGraph(x,type) "log10(x)" -set ::GlobalFitIQGraph(c,x) "5" +set ::GlobalFitIQGraph(c,x) "103" set ::GlobalFitIQGraph(y,logscale) "1" +set ::GlobalFitIQGraph(c,y) "424" set ::GlobalFitIQGraph(e.errstipples) "" -set ::GlobalFitIQGraph(c,y) "433" set ::GlobalFitIQGraph(e,restags) "" set ::GlobalFitIQGraph(title) "unknown" set ::GlobalFitIQGraph(l,anchor) "n" set ::GlobalFitIQGraph(GraphName) "GlobalFitIQGraph" set ::GlobalFitIQGraph(symbolselection) {square circle diamond plus cross splus scross triangle} -set ::GlobalFitIQGraph(e,errorhide) "" +set ::GlobalFitIQGraph(e,errorhide) {no no no no no no no no} set ::GlobalFitIQGraph(y,subticks) "5" set ::GlobalFitIQGraph(l,ipadx) {0 0} set ::GlobalFitIQGraph(c,color) "black" @@ -2997,41 +3129,41 @@ set ::GlobalFitIQGraph(margin,plotpady) {5 5} set ::GlobalFitIQGraph(fitrange) "no" set ::GlobalFitIQGraph(margin,right) "0" set ::GlobalFitIQGraph(x,min) "" -set ::GlobalFitIQGraph(e,errfill) "" +set ::GlobalFitIQGraph(e,errfill) {Black Black Black Black Black Black Black Black} set ::GlobalFitIQGraph(height) "512" -set ::GlobalFitIQGraph(e,erroutline) "" -set ::GlobalFitIQGraph(e,errdash) "" +set ::GlobalFitIQGraph(e,erroutline) {blue blue blue blue blue blue blue blue} +set ::GlobalFitIQGraph(e,errdash) {0 0 0 0 0 0 0 0} set ::GlobalFitIQGraph(y,ticklength) "10" set ::GlobalFitIQGraph(g,color) "black" set ::GlobalFitIQGraph(x,max) "" set ::GlobalFitIQGraph(g,linewidth) "1" set ::GlobalFitIQGraph(x,color) "Black" -set ::GlobalFitIQGraph(l,legendtext) "" -set ::GlobalFitIQGraph(e,ydata) "" +set ::GlobalFitIQGraph(l,legendtext) {{Sim.: 1} {Sim.: 1t} {Sim.: 2} {Sim.: 2t} {Sim.: 0} {Sim.: 0t} {Sim.: Re Rp} {Sim.: Re Rp t}} +set ::GlobalFitIQGraph(e,ydata) {{6.06753e+010 6.06109e+010 6.05449e+010 6.04772e+010 6.04077e+010 6.03365e+010 6.02635e+010 6.01887e+010 6.01119e+010 6.00332e+010 5.99525e+010 5.98698e+010 5.9785e+010 5.96981e+010 5.9609e+010 5.95177e+010 5.9424e+010 5.93281e+010 5.92297e+010 5.91289e+010 5.90256e+010 5.89197e+010 5.88112e+010 5.87e+010 5.85861e+010 5.84694e+010 5.83498e+010 5.82272e+010 5.81017e+010 5.79731e+010 5.78414e+010 5.77065e+010 5.75683e+010 5.74268e+010 5.72819e+010 5.71334e+010 5.69815e+010 5.68259e+010 5.66666e+010 5.65035e+010 5.63365e+010 5.61656e+010 5.59907e+010 5.58117e+010 5.56285e+010 5.5441e+010 5.52492e+010 5.50529e+010 5.48522e+010 5.46468e+010 5.44368e+010 5.4222e+010 5.40023e+010 5.37777e+010 5.35481e+010 5.33133e+010 5.30734e+010 5.28281e+010 5.25775e+010 5.23214e+010 5.20598e+010 5.17925e+010 5.15195e+010 5.12407e+010 5.0956e+010 5.06653e+010 5.03686e+010 5.00657e+010 4.97567e+010 4.94413e+010 4.91196e+010 4.87914e+010 4.84567e+010 4.81154e+010 4.77675e+010 4.74129e+010 4.70515e+010 4.66832e+010 4.63081e+010 4.59261e+010 4.55371e+010 4.51411e+010 4.4738e+010 4.43279e+010 4.39107e+010 4.34863e+010 4.30549e+010 4.26162e+010 4.21705e+010 4.17176e+010 4.12577e+010 4.07906e+010 4.03165e+010 3.98354e+010 3.93473e+010 3.88523e+010 3.83506e+010 3.7842e+010 3.73268e+010 3.68051e+010 3.62769e+010 3.57425e+010 3.52018e+010 3.46552e+010 3.41027e+010 3.35445e+010 3.29809e+010 3.2412e+010 3.18381e+010 3.12593e+010 3.0676e+010 3.00884e+010 2.94967e+010 2.89014e+010 2.83027e+010 2.77009e+010 2.70963e+010 2.64894e+010 2.58805e+010 2.527e+010 2.46583e+010 2.40458e+010 2.3433e+010 2.28203e+010 2.22081e+010 2.1597e+010 2.09874e+010 2.03798e+010 1.97748e+010 1.91728e+010 1.85744e+010 1.79801e+010 1.73904e+010 1.68059e+010 1.62271e+010 1.56545e+010 1.50888e+010 1.45305e+010 1.398e+010 1.34379e+010 1.29047e+010 1.2381e+010 1.18673e+010 1.13639e+010 1.08714e+010 1.03903e+010 9.92087e+009 9.46358e+009 9.01879e+009 8.58682e+009 8.16799e+009 7.76257e+009 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6.97789e+007 6.5965e+007 6.24553e+007 5.93089e+007 5.65598e+007 5.42135e+007 5.2247e+007 5.06098e+007 4.92289e+007 4.80149e+007 4.68702e+007 4.56974e+007 4.44084e+007 4.29324e+007 4.12224e+007 3.92596e+007 3.70546e+007 3.46459e+007 3.20958e+007 2.94831e+007 2.68948e+007 2.44163e+007 2.21227e+007 2.00704e+007 1.82919e+007 1.67933e+007 1.55553e+007 1.45374e+007 1.36845e+007 1.29359e+007 1.22344e+007 1.15342e+007 1.08075e+007 1.00468e+007 9.26494e+006 8.4903e+006 7.76036e+006 7.11311e+006 6.5787e+006 6.17277e+006 5.8927e+006 5.71756e+006 5.61194e+006 5.53273e+006 5.43749e+006 5.29264e+006 5.07958e+006 4.79748e+006 4.4619e+006 4.09985e+006 3.74229e+006 3.41624e+006 3.13822e+006 2.9111e+006 2.72474e+006 2.56046e+006 2.39773e+006 2.22105e+006 2.02493e+006 1.81528e+006 1.60701e+006 1.41853e+006 1.26515e+006 1.15384e+006 1.08099e+006 1.03407e+006 996421 953299 896732 827372 752723 682703 624641 579983 544135 509318 468833 420491 367479 316324 273243 240963 217765 199092 180551 160348 139731 121387 107129 96555.6 87524.9 77878.8 66964.9 55809.6 45984.9 38264.2 32205.3 26848.3 21695.1 17005.1 13252.8 10473.5 8236.43 6182.66 4399.21 3170.94 2492.75 2041.12 1643.17 1528.7 1920.83 2542.36 2888.18 3020 3660.23 5196.76 6966.93 8108.58 8921.83 10500.6 12835.3 14390.3 14348 14193.5 15634 17816.3 18749.5 18989.3 20925.7 24224.9 25723.7 24866.3 24810.9 26456 26771.1 25358.2 26011.6 29064.3 30225.2 29238.1 29918 31100.3 29227.8 27277.9 28606.6 29438.5 28232.7 28981 30084.7 27829.6 26104.2 26532 25150.9 24133 25399.7 24450.7 22602.5 22420.8 20597.6 19099.7 19551 18345.1 17436.6 16938.1 14842.6 14106.2 13383.9 12237.2 12000.3 10602.6 9638.78 8796.85 7777.54 7413.46 6442.04 5813.96 4970.77 4332.16 3823.51 3248.22 2786.71 2245.69 1870.89 1486.17 1192.55 900.868 672.35 480.862 330.148 219.596 142.329 91.9997 85.4589 89.1511 144.641 165.798 248.723 347.773 428.144 544.372 586.825 758.987 851.709 880.959 1023.1 1078.92 1138.64 1199.4 1193.91 1249.28 1264.66 1198.4 1194.58 1185.34 1096.27 1023.03 971.106 887.699 793.661 699.531 606.332 524.341 438.446 350.809 276.096 210.477 153.572 106.974 70.995 45.1879 30.5914 24.7364 28.2718 42.7903 58.3037 84.4567 109.13 133.599 162.739 179.932 203.33 213.158 222.322 223.511 217.084 208.279 191.004 174.265 152.035 130.242 105.898 82.6524 61.2905 43.2778 28.8807 19.2967 14.041 12.8649 14.2477 22.3326 29.4978 36.7039 47.9704 54.5455 60.096 64.468 63.8446 62.2884 56.6387 49.9933 41.4183 32.6795} {6.06753e+010 6.06109e+010 6.05449e+010 6.04772e+010 6.04077e+010 6.03365e+010 6.02635e+010 6.01887e+010 6.01119e+010 6.00332e+010 5.99525e+010 5.98698e+010 5.9785e+010 5.96981e+010 5.9609e+010 5.95177e+010 5.9424e+010 5.93281e+010 5.92297e+010 5.91289e+010 5.90256e+010 5.89197e+010 5.88112e+010 5.87e+010 5.85861e+010 5.84694e+010 5.83498e+010 5.82272e+010 5.81017e+010 5.79731e+010 5.78414e+010 5.77065e+010 5.75683e+010 5.74268e+010 5.72819e+010 5.71334e+010 5.69815e+010 5.68259e+010 5.66666e+010 5.65035e+010 5.63365e+010 5.61656e+010 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8.53605e+007 8.10043e+007 7.68537e+007 7.28955e+007 6.91182e+007 6.55117e+007 6.20671e+007 5.87764e+007 5.56326e+007 5.26296e+007 4.97616e+007 4.70237e+007 4.44111e+007 4.19196e+007 3.95452e+007 3.72841e+007 3.51325e+007 3.3087e+007 3.11441e+007 2.93004e+007 2.75523e+007 2.58965e+007 2.43296e+007 2.28481e+007 2.14486e+007 2.01277e+007 1.8882e+007 1.77079e+007 1.66022e+007 1.55615e+007 1.45826e+007 1.36621e+007 1.27969e+007 1.1984e+007 1.12205e+007 1.05034e+007 9.83011e+006 9.19793e+006 8.60442e+006 8.0472e+006 7.52406e+006 7.03289e+006 6.57174e+006 6.13873e+006 5.73216e+006 5.35039e+006 4.99192e+006 4.65534e+006 4.33935e+006 4.04271e+006 3.7643e+006 3.50305e+006 3.25796e+006 3.02811e+006 2.81262e+006 2.61069e+006 2.42155e+006 2.24447e+006 2.07877e+006 1.92382e+006 1.779e+006 1.64373e+006 1.51748e+006 1.39973e+006 1.28998e+006 1.18777e+006 1.09266e+006 1.00422e+006 922064 845803 775083 709563 648921 592851 541066 493291 449269 408757 371524 337354 306041 277393 251227 227374 205670 185965 168114 151984 137447 124385 112684 102240 92953.9 84731.6 77486 71135.1 65601.6 60813.4 56702.7 53206.2 50264.5 47822.2 45827.4 44231.9 42990.7 42061.8 41600.4 40988.4 40774.3 40733.2 40836.4 41057.9 41097.5 41190.6 41951.9 42555.6 43147.8 43612.4 44085.1 44560 44968.9 45349.2 45653.8 45902.1 46086.7 46226.1 46293.8 46390.7 46198.2 46138.2 45893.8 45473.6 45067.4 44692.6 44044 43411.7 42824.1 42065.3 41244.3 40261.4 39431.4 38357.4 37419.7 36213.5 35246.5 34111.5 32950.8 31769.3 30572 29363.8 28149.3 26933.3 25720.3 24514.5 23320.2 22141.3 20987.8 19851.2 18842 17953.7 16310.1 15527.5 14587 13400.8 12983.8 11856.5 10921.6 10404.6 9542.25 8785.31 8228.15 7611.72 7019.85 6512.42 6011.61 5539.83 5116.13 4731.15 4356.11 4030.06 3733.53 3471.01 3228.64 3012.89 2816.71 2642.02 2482.27 2339.73 2211.74 2097.27 1995.51 1905.54 1824.5 1748.77 1681.02 1616.93 1553.89 1488.06 1439.96 1388.24 1342.04 1292.12 1246.03 1202.96 1148.26 1101.31 1055.46 1008.83 962.326 922.817 885.592 839.957 794.446 768.572 734.188 682.268 654.95 626.231 585.882 550.046 524.199 493.424 467.561 440.354 413.067 390.685 371.688 348.149 331.145 314.125 294.281 281.322 266.535 252.55 239.163 226.894 215.282 204.619 194.279 184.44 175.045 166.365 157.949 150.174 142.711 135.529 128.824 122.246 116.092 110.425 104.731 99.397 94.2292 89.485 85.0021 80.6549 76.3028 72.3582 68.8584 65.2814 61.9768 58.9672 55.7931 52.803 50.3221 47.8273 45.0731 43.1485 40.6636 38.5788 36.8541 34.6778 33.0279 31.4814}} set ::GlobalFitIQGraph(y,mapped) "1" set ::GlobalFitIQGraph(margin,top) "0" set ::GlobalFitIQGraph(l,borderwidth) "2" -set ::GlobalFitIQGraph(e,errstipples) {hline1 hline1 hline1 hline1 hline1 hline1} -set ::GlobalFitIQGraph(e,symbol) "" +set ::GlobalFitIQGraph(e,errstipples) {hline1 hline1 hline1 hline1 hline1 hline1 hline1 hline1} +set ::GlobalFitIQGraph(e,symbol) {none none none none none none none none} set ::GlobalFitIQGraph(y,tickfont) {Helvetica 10} set ::GlobalFitIQGraph(font) {Helvetica 10} set ::GlobalFitIQGraph(graph,bg) "white" set ::GlobalFitIQGraph(margin,bottom) "0" -set ::GlobalFitIQGraph(e,outline) "" -set ::GlobalFitIQGraph(e,resfill) "" +set ::GlobalFitIQGraph(e,outline) {Black Black Black Black Black Black Black Black} +set ::GlobalFitIQGraph(e,resfill) {Black Black Black Black Black Black Black Black} set ::GlobalFitIQGraph(plot,relief) "flat" -set ::GlobalFitIQGraph(e,resdash) "" +set ::GlobalFitIQGraph(e,resdash) {0 0 0 0 0 0 0 0} set ::GlobalFitIQGraph(x,showticks) "yes" set ::GlobalFitIQGraph(x,mapped) "1" set ::GlobalFitIQGraph(y,factor) "1.0" set ::GlobalFitIQGraph(stipples) {bdiagonal1 bdiagonal2 checker2 checker3 cross1 cross2 cross3 crossdiag dot1 dot2 dot3 dot4 fdiagonal1 fdiagonal2 hline1 hline2 lbottom ltop rbottom rtop vline1 vline2} set ::GlobalFitIQGraph(graph,borderwidth) "0" -set ::GlobalFitIQGraph(e,resdata) "" +set ::GlobalFitIQGraph(e,resdata) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 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"black" set ::GlobalFitIQGraph(c,dash) "0" set ::GlobalFitIQGraph(y,size) "12" set ::GlobalFitIQGraph(x,rot) "0" -set ::GlobalFitIQGraph(e,error) "" +set ::GlobalFitIQGraph(e,error) {{-1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 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-1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0}} set ::GlobalFitIQGraph(x,factor) "1.0" set ::GlobalFitIQGraph(x,stepsize) "0" set ::GlobalFitIQGraph(plot,background) "gray90" @@ -3044,23 +3176,23 @@ set ::GlobalFitIQGraph(upper,x) "" set ::GlobalFitIQGraph(width) "768" set ::GlobalFitIQGraph(g,minor) "no" set ::GlobalFitIQGraph(upper,y) "" -set ::GlobalFitIQGraph(e,reslinewidth) "" +set ::GlobalFitIQGraph(e,reslinewidth) {1 1 1 1 1 1 1 1} set ::GlobalFitIQGraph(y,stepsize) "0" set ::GlobalFitIQGraph(y,showticks) "yes" set ::GlobalFitIQGraph(lower,x) "" set ::GlobalFitIQGraph(l,position) "right" set ::GlobalFitIQGraph(lower,y) "" set ::GlobalFitIQGraph(y,type) "log10(y)" -set ::ResIQGraph(e,fill) "Black" +set ::ResIQGraph(e,fill) "" set ::ResIQGraph(e.resstipples) "" -set ::ResIQGraph(e,scale) "no" -set ::ResIQGraph(e,dash) "0" -set ::ResIQGraph(e,linewidth) "2" +set ::ResIQGraph(e,scale) "" +set ::ResIQGraph(e,dash) "" +set ::ResIQGraph(e,linewidth) "" set ::ResIQGraph(y,min) "" -set ::ResIQGraph(l,hide) "yes" -set ::ResIQGraph(e,resoutline) "blue" -set ::ResIQGraph(e,xdata) {{0.01 0.0106770427203 0.0113999241252 0.0121717476894 0.012995827006 0.013875700013 0.0148151441813 0.0158181927332 0.0168891519571 0.0180326196956 0.019253505085 0.0205570496309 0.0219488497113 0.0234348806031 0.0250215221345 0.0267155860758 0.028524345383 0.0304555654225 0.0325175373088 0.0347191135006 0.0370697458059 0.0395795259602 0.0422592289528 0.0451203592858 0.0481752003651 0.051436867236 0.0549193628879 0.0586376383729 0.0626076569927 0.0668464628332 0.0713722539374 0.0762044604337 0.0813638279531 0.0868725066946 0.0927541465202 0.0990339984885 0.105739023263 0.112898006859 0.120541684227 0.128702871207 0.137416605411 0.146720296646 0.156653887523 0.167260024939 0.178584243168 0.190675159349 0.203584682208 0.217368234914 0.232084993022 0.247798138525 0.264575131105 0.282487997755 0.301613642002 0.322034174069 0.343837263395 0.367116515011 0.391971871412 0.418510041624 0.446844959331 0.477098272015 0.50939986321 0.543888410123 0.580711978999 0.620028660799 0.662007249918 0.706827968856 0.754683241941 0.805778521453 0.860333169669 0.918581400629 0.980773285663 1.047175827 1.11807410406 1.19377249735 1.27459599526 1.36089158926 1.45302976363 1.55140608602 1.6564429057 1.7685911668 1.88833234428 2.016180511 2.15268454479 2.29843048482 2.45404404761 2.6201933134 2.79759159427 2.98700049661 3.1892331908 3.40515790233 3.63570163927 3.88185417209 4.14467228296 4.4252843027 4.72489495496 5.04479052832 5.38634439861 5.75102292504 6.14039174564 6.55612249878 6.99999999993}} -set ::ResIQGraph(e,element) "1" +set ::ResIQGraph(l,hide) "no" +set ::ResIQGraph(e,resoutline) "" +set ::ResIQGraph(e,xdata) "" +set ::ResIQGraph(e,element) "0" set ::ResIQGraph(y,max) "" set ::ResIQGraph(x,linewidth) "2" set ::ResIQGraph(colorselection) {black red green blue cyan magenta yellow violet purple orange pink gray} @@ -3069,32 +3201,32 @@ set ::ResIQGraph(y,titlecolor) "black" set ::ResIQGraph(y,loose) "no" set ::ResIQGraph(fit,background) "#cccccc" set ::ResIQGraph(x,size) "12" -set ::ResIQGraph(e,dashcolor) "Black" -set ::ResIQGraph(e,outlinewidth) "1" +set ::ResIQGraph(e,dashcolor) "" +set ::ResIQGraph(e,outlinewidth) "" set ::ResIQGraph(x,ticklength) "10" set ::ResIQGraph(l,posx) "10" -set ::ResIQGraph(e,errlinewidth) "1" +set ::ResIQGraph(e,errlinewidth) "" set ::ResIQGraph(l,posy) "10" -set ::ResIQGraph(e,linehide) "0" +set ::ResIQGraph(e,linehide) "" set ::ResIQGraph(graph,fg) "black" -set ::ResIQGraph(e,elementname) "graph1" +set ::ResIQGraph(e,elementname) "" set ::ResIQGraph(dashnames) {{-} {..} {--} {.-} {..-} {--.}} -set ::ResIQGraph(e,reshide) "no" +set ::ResIQGraph(e,reshide) "" set ::ResIQGraph(graph,relief) "flat" -set ::ResIQGraph(e,pixels) "4" +set ::ResIQGraph(e,pixels) "" set ::ResIQGraph(dashpattern) {{0} {2 2} {8 2 8 2} {2 2 8 2} {2 2 2 2 8 2} {8 2 8 2 2 2} } set ::ResIQGraph(x,tickcolor) "black" set ::ResIQGraph(x,logscale) "0" set ::ResIQGraph(e,resstipples) "hline1" set ::ResIQGraph(y,title) "(I(Q)-Ith(Q))/DI(Q)" set ::ResIQGraph(l,bg) "white" -set ::ResIQGraph(e,errtags) "{}" -set ::ResIQGraph(e,symbolhide) "no" +set ::ResIQGraph(e,errtags) "" +set ::ResIQGraph(e,symbolhide) "" set ::ResIQGraph(c,hide) "yes" set ::ResIQGraph(plot,borderwidth) "0" set ::ResIQGraph(y,rot) "0" -set ::ResIQGraph(e,smooth) "linear" -set ::ResIQGraph(e,offdashcolor) "White" +set ::ResIQGraph(e,smooth) "" +set ::ResIQGraph(e,offdashcolor) "" set ::ResIQGraph(g,dash) "0" set ::ResIQGraph(y,color) "Black" set ::ResIQGraph(x,subticks) "5" @@ -3111,7 +3243,7 @@ set ::ResIQGraph(title) "unknown" set ::ResIQGraph(l,anchor) "n" set ::ResIQGraph(GraphName) "ResIQGraph" set ::ResIQGraph(symbolselection) {square circle diamond plus cross splus scross triangle} -set ::ResIQGraph(e,errorhide) "no" +set ::ResIQGraph(e,errorhide) "" set ::ResIQGraph(y,subticks) "5" set ::ResIQGraph(l,ipadx) {0 0} set ::ResIQGraph(c,color) "black" @@ -3126,41 +3258,41 @@ set ::ResIQGraph(margin,plotpady) {5 5} set ::ResIQGraph(fitrange) "no" set ::ResIQGraph(margin,right) "0" set ::ResIQGraph(x,min) "" -set ::ResIQGraph(e,errfill) "Black" +set ::ResIQGraph(e,errfill) "" set ::ResIQGraph(height) "512" -set ::ResIQGraph(e,erroutline) "blue" -set ::ResIQGraph(e,errdash) "0" +set ::ResIQGraph(e,erroutline) "" +set ::ResIQGraph(e,errdash) "" set ::ResIQGraph(y,ticklength) "10" set ::ResIQGraph(g,color) "black" set ::ResIQGraph(x,max) "" set ::ResIQGraph(g,linewidth) "1" set ::ResIQGraph(x,color) "Black" -set ::ResIQGraph(l,legendtext) "{}" -set ::ResIQGraph(e,ydata) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::ResIQGraph(l,legendtext) "" +set ::ResIQGraph(e,ydata) "" set ::ResIQGraph(y,mapped) "1" set ::ResIQGraph(margin,top) "0" set ::ResIQGraph(l,borderwidth) "2" set ::ResIQGraph(e,errstipples) "hline1" -set ::ResIQGraph(e,symbol) "circle" +set ::ResIQGraph(e,symbol) "" set ::ResIQGraph(y,tickfont) {Helvetica 10} set ::ResIQGraph(font) {Helvetica 10} set ::ResIQGraph(graph,bg) "white" set ::ResIQGraph(margin,bottom) "0" -set ::ResIQGraph(e,outline) "Black" -set ::ResIQGraph(e,resfill) "Black" +set ::ResIQGraph(e,outline) "" +set ::ResIQGraph(e,resfill) "" set ::ResIQGraph(plot,relief) "flat" -set ::ResIQGraph(e,resdash) "0" +set ::ResIQGraph(e,resdash) "" set ::ResIQGraph(x,showticks) "yes" set ::ResIQGraph(x,mapped) "1" set ::ResIQGraph(y,factor) "1.0" set ::ResIQGraph(stipples) {bdiagonal1 bdiagonal2 checker2 checker3 cross1 cross2 cross3 crossdiag dot1 dot2 dot3 dot4 fdiagonal1 fdiagonal2 hline1 hline2 lbottom ltop rbottom rtop vline1 vline2} set ::ResIQGraph(graph,borderwidth) "0" -set ::ResIQGraph(e,resdata) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::ResIQGraph(e,resdata) "" set ::ResIQGraph(x,titlecolor) "black" set ::ResIQGraph(c,dash) "0" set ::ResIQGraph(y,size) "12" set ::ResIQGraph(x,rot) "0" -set ::ResIQGraph(e,error) {{-1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0}} +set ::ResIQGraph(e,error) "" set ::ResIQGraph(x,factor) "1.0" set ::ResIQGraph(x,stepsize) "0" set ::ResIQGraph(plot,background) "gray90" @@ -3173,7 +3305,7 @@ set ::ResIQGraph(upper,x) "" set ::ResIQGraph(width) "768" set ::ResIQGraph(g,minor) "no" set ::ResIQGraph(upper,y) "" -set ::ResIQGraph(e,reslinewidth) "1" +set ::ResIQGraph(e,reslinewidth) "" set ::ResIQGraph(y,stepsize) "0" set ::ResIQGraph(y,showticks) "yes" set ::ResIQGraph(lower,x) "" @@ -3355,8 +3487,8 @@ set ::StructParData(isp_text_export) {description;value;error Guinier approx.: I(Q) = I0 exp(-Rg^2*Q^2/3);; 1st data point (ascending);1; number of points;7; -Q_min;; -Q_max;; +Q_min;0.01; +Q_max;0.0148151441813; Guinier radius RG;-1.0000e+000;-1.0000e+000 forward scattering I(0);-1.0000e+000;-1.0000e+000 chisq(Guinier);-1.0; @@ -3364,8 +3496,8 @@ chisq(Guinier);-1.0; Porod approx.: I(Q) = c0+c4*Q^(D-4);; 1st data point (descending);1; number of points;25; -Q_min;; -Q_max;; +Q_min;1.45302976363; +Q_max;6.99999999993; background c_0;-1.0000e+000;-1.0000e+000 Porod constant c_4;-1.0000e+000;-1.0000e+000 potential law D;0.0000e+000;-1.0000e+000 @@ -3412,38 +3544,38 @@ set ::StructParData(Dc4) "-1.0" set ::StructParData(Dlc) "-1.0" set ::StructParData(DQc4) "-1.0" set ::StructParData(isp_text_display) {Guinier approx.: - I(Q) = I0 exp(-Rg^2*Q^2/3) - 1st data point (ascending) = 1 - number of points = 7 - Q_min - Q_max - Guinier radius RG = -1.0000e+000 ± -1.0000e+000 - forward scattering I(0) = -1.0000e+000 ± -1.0000e+000 - chisq(Guinier) = -1.0 - + I(Q) = I0 exp(-Rg^2*Q^2/3) + 1st data point (ascending) = 1 + number of points = 7 + Q_min = 0.01 + Q_max = 0.0148151441813 + Guinier radius RG = -1.0000e+000 ± -1.0000e+000 + forward scattering I(0) = -1.0000e+000 ± -1.0000e+000 + chisq(Guinier) = -1.0 + Porod approx.: - I(Q) = c0+c4*Q^(D-4) - 1st data point (descending) = 1 - number of points = 25 - Q_min - Q_max - background c_0 = -1.0000e+000 ± -1.0000e+000 - Porod constant c_4 = -1.0000e+000 ± -1.0000e+000 - potential law D = 0.0000e+000 ± -1.0000e+000 - chisq(Porod) = -1.0 - - integral structural parameters: - correlation length lc = -1.0000e+000 ± -1.0000e+000 - correlation area Ac = -1.0000e+000 ± -1.0000e+000 - intersection length li = -1.0000e+000 ± -1.0000e+000 - Porod volume VP = -1.0000e+000 ± -1.0000e+000 - Porod radius RP = -1.0000e+000 ± -1.0000e+000 - specific surface S/V = -1.0000e+000 ± -1.0000e+000 - scattering invariant Inv = -1.0000e+000 ± -1.0000e+000 -integrated intensity iI = int(I(Q)*Q)dQ = -1.0000e+000 ± -1.0000e+000 - integral intensity intI = int(I(Q))dQ = -1.0000e+000 ± -1.0000e+000 - Q_min = -1.0 - Q_max = -1.0 } + I(Q) = c0+c4*Q^(D-4) + 1st data point (descending) = 1 + number of points = 25 + Q_min = 1.45302976363 + Q_max = 6.99999999993 + background c_0 = -1.0000e+000 ± -1.0000e+000 + Porod constant c_4 = -1.0000e+000 ± -1.0000e+000 + potential law D = 0.0000e+000 ± -1.0000e+000 + chisq(Porod) = -1.0 + + integral structural parameters: + correlation length lc = -1.0000e+000 ± -1.0000e+000 + correlation area Ac = -1.0000e+000 ± -1.0000e+000 + intersection length li = -1.0000e+000 ± -1.0000e+000 + Porod volume VP = -1.0000e+000 ± -1.0000e+000 + Porod radius RP = -1.0000e+000 ± -1.0000e+000 + specific surface S/V = -1.0000e+000 ± -1.0000e+000 + scattering invariant Inv = -1.0000e+000 ± -1.0000e+000 +integrated intensity iI = int(I(Q)*Q)dQ = -1.0000e+000 ± -1.0000e+000 + integral intensity intI = int(I(Q))dQ = -1.0000e+000 ± -1.0000e+000 + Q_min = -1.0 + Q_max = -1.0 } set ::StructParData(li) "-1.0" set ::StructParData(DRP) "-1.0" set ::StructParData(w) "123" diff --git a/data/triaxialellipsoid.sas b/data/triaxialellipsoid.sas index bb39a9cb..109534be 100644 --- a/data/triaxialellipsoid.sas +++ b/data/triaxialellipsoid.sas @@ -113,8 +113,8 @@ set sasfit(export,filename) "" set sasfit(Nth,file,Dlambda) "" set sasfit(Nth,file,DI) "" set sasfit(datatypes) { { Ascii ".*" } { BerSANS "D???????.???" } { SESANS "*.ses"} { ALV5000 "*.ASC"} { All "*" } } -set sasfit(SQ,root_menu) ".analytical.fitpar.sq.lay.wrl.whichsq.menu" set sasfit(FF,root_menu) ".analytical.fitpar.ff.lay.wrl.whichff.menu" +set sasfit(SQ,root_menu) ".analytical.fitpar.sq.lay.wrl.whichsq.menu" set sasfit(Nth,hide) "" set sasfit(print,ipady1) "0" set sasfit(print,file) "sasfit.ps" @@ -255,7 +255,7 @@ set addsasfit(print,tmp2ps) "sasfit2.ps" set addsasfit(print,ipadx1) "0" set addsasfit(print,ipadx2) "0" set addsasfit(file,dr_percent) "" -set addsasfit(sim,N) "1500" +set addsasfit(sim,N) "500" set addsasfit(file,dr_max_Dq_q) "" set addsasfit(Nth,file,hide) "" set addsasfit(print,units) "m" @@ -311,104 +311,381 @@ set addsasfit(file,lastskip) "" set addsasfit(file,r1) "" set addsasfit(Nth,file,l1) "" set ::ask4dataset_var(simorfit) "simulate" +set ::ask4dataset_var(datasetlabel) {1 2 3 4 5 6 7 8} set ::ask4dataset_var(go_on) "1" -set ::ask4dataset_var(datasetlabel) {1 2 3 4 5 6} set ::ask4dataset_var(N_datasets) "8" set ::ask4dataset_var(dataset) "6" -set ::GlobalAnalytPar(R_lc) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(R_lc) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(P1) "10.0" -set ::GlobalAnalytPar(wR) "0" +set ::GlobalAnalytPar(wR) "4.45573e+008" set ::GlobalAnalytPar(P2) "20.0" -set ::GlobalAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::GlobalAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar(P3) "30.0" set ::GlobalAnalytPar(sumfp) "0.0" set ::GlobalAnalytPar(P4) "5.0" set ::GlobalAnalytPar() "0.0" set ::GlobalAnalytPar(resolution) "no" -set ::GlobalAnalytPar(SD,param_count) {10 10 10 10 10 10 10 0} -set ::GlobalAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::GlobalAnalytPar(SD,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::GlobalAnalytPar(SD,param_count) {10 10 10 10 10 10 10 10} +set ::GlobalAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(SD,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} set ::GlobalAnalytPar(P5) "0.2" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(P6) "1.0" -set ::GlobalAnalytPar(fp) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(R_li) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(fp) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(R_li) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(alpha) "" -set ::GlobalAnalytPar(calcSDFF) {yes yes yes yes yes yes yes} -set ::GlobalAnalytPar(SD,typestr) {Delta Delta Delta Delta Delta Delta LogNorm} -set ::GlobalAnalytPar(P7) "0.5" +set ::GlobalAnalytPar(calcSDFF) {yes yes yes yes yes yes yes yes} +set ::GlobalAnalytPar(SD,typestr) {Delta Delta Delta Delta Delta Delta Delta Delta} +set ::GlobalAnalytPar(P7) "0.0" set ::GlobalAnalytPar(sumR_RG) "0.0" -set ::GlobalAnalytPar(SD,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(SD,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar(P8) "0.0" set ::GlobalAnalytPar(par_w) ".obW.tab.analytpar" set ::GlobalAnalytPar(mom_descr) {moments of_analytical_size distrib.} set ::GlobalAnalytPar(sumR_Ac) "0.0" set ::GlobalAnalytPar(covar) "" -set ::GlobalAnalytPar(SD,a) {{1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.2 1.0 5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(SD,a) {{1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.2 1.0 5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::GlobalAnalytPar(sumR_lc) "0.0" set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(SQ,how) {0 0 0 0 0 0 0} -set ::GlobalAnalytPar(mfit) "0" +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SQ,how) {0 0 0 0 0 0 0 0} +set ::GlobalAnalytPar(mfit) "1" set ::GlobalAnalytPar(Q) "0" set ::GlobalAnalytPar(error) "0" -set ::GlobalAnalytPar(R) "0" +set ::GlobalAnalytPar(R) "2.61389e+008" set ::GlobalAnalytPar(sumR_li) "0.0" -set ::GlobalAnalytPar(SQ,typestr) {None None None None None None None} -set ::GlobalAnalytPar(FF,typestr) {299 300 301 302 303 304 304} -set ::GlobalAnalytPar(reducedchisq) "0" +set ::GlobalAnalytPar(SQ,typestr) {None None None None None None None None} +set ::GlobalAnalytPar(FF,typestr) {311 312 313 314 315 316 309 310} +set ::GlobalAnalytPar(reducedchisq) "1.98585e+017" set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(SQ,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::GlobalAnalytPar(FF,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::GlobalAnalytPar(ndata) "12008" +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SQ,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::GlobalAnalytPar(FF,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} set ::GlobalAnalytPar(par_text_export) {description;value;error;factor;global_param;description;value;error;factor;global_param;description;value;error;factor;global_param scattering contribution;1;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; -dataset;1;;;;label;;;;;;;;; -LogNorm;;;;;Sphere;;;;;None;;;; -N;1.0;;;;R;distr.;;;;;;;; -s;0.05;;;;;;;;;;;;; -p;1.0;;;;;;;;;;;;; -mu;10.0;;;;eta;1.0;;;;;;;;} +dataset;1;;;;label;1;;;;;;;; +Delta;;;;;triax ellip shell 1;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;2;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;2;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 1t;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;3;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;3;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 2;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;4;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;4;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 2t;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;5;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;5;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 3;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;6;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;6;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 3t;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;7;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;7;;;;label;0;;;;;;;; +Delta;;;;;triax ellip shell;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.0;;;;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;8;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;8;;;;label;0t;;;;;;;; +Delta;;;;;triax ellip shell t;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.0;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;;} +set ::GlobalAnalytPar(ndata) "4008" set ::GlobalAnalytPar(par_x_X) "1.1" -set ::GlobalAnalytPar(mom_text_display) {scattering contribution = 1 calculate = yes - LogNorm Sphere - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - +set ::GlobalAnalytPar(SD,param_count_old) {10 10 10 10 10 10 10 10} +set ::GlobalAnalytPar(mom_text_display) {scattering contribution = 1 calculate = yes + Delta triax ellip shell 1 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 2 calculate = yes + Delta triax ellip shell 1t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 3 calculate = yes + Delta triax ellip shell 2 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 4 calculate = yes + Delta triax ellip shell 2t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 5 calculate = yes + Delta triax ellip shell 3 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 6 calculate = yes + Delta triax ellip shell 3t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 7 calculate = yes + Delta triax ellip shell + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 8 calculate = yes + Delta triax ellip shell t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + scattering contribution - of all size distrib. sum N_i = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - sumR_lc = 0.0000e+000 sumlc = 0.0000e+000 - sumR_li = 0.0000e+000 sumli = 0.0000e+000 - sumR_Ac = 0.0000e+000 sumAc = 0.0000e+000 - sumR_VP = 0.0000e+000 sumVP = 0.0000e+000 - sumR_RG = 0.0000e+000 sumRG = 0.0000e+000 - sumfp(Sph.) = 0.0000e+000 } -set ::GlobalAnalytPar(SD,param_count_old) {10 10 10 10 10 10 10} -set ::GlobalAnalytPar(datalabel) {I_1 {} {} {} {} {} 0} + of all size distrib. sum N_i = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + sumR_lc = 0.0000e+000 sumlc = 0.0000e+000 + sumR_li = 0.0000e+000 sumli = 0.0000e+000 + sumR_Ac = 0.0000e+000 sumAc = 0.0000e+000 + sumR_VP = 0.0000e+000 sumVP = 0.0000e+000 + sumR_RG = 0.0000e+000 sumRG = 0.0000e+000 + sumfp(Sph.) = 0.0000e+000 } +set ::GlobalAnalytPar(datalabel) {1 {} {} {} {} {} 0 0t} set ::GlobalAnalytPar(GraphName) "AnalytPar" set ::GlobalAnalytPar(isGlobal) "1" set ::GlobalAnalytPar(w_MomentsAnalytPar) "" -set ::GlobalAnalytPar(SD,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(SD,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar(mom_text_export) {description;value;description;value scattering contribution;1;calculate;yes -LogNorm;;Sphere; +Delta;;triax ellip shell 1; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;2;calculate;yes +Delta;;triax ellip shell 1t; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;3;calculate;yes +Delta;;triax ellip shell 2; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;4;calculate;yes +Delta;;triax ellip shell 2t; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;5;calculate;yes +Delta;;triax ellip shell 3; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;6;calculate;yes +Delta;;triax ellip shell 3t; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;7;calculate;yes +Delta;;triax ellip shell; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;8;calculate;yes +Delta;;triax ellip shell t; ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -433,156 +710,491 @@ sumR_RG;0.0000e+000;sumRG;0.0000e+000 sumfp(Sph.);0.0000e+000;;} set ::GlobalAnalytPar() "0.0" set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(chisq) "0" +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(chisq) "7.95729e+020" set ::GlobalAnalytPar(file) "unknown.par" -set ::GlobalAnalytPar(varianceOFfit) "0" +set ::GlobalAnalytPar(varianceOFfit) "1.98585e+017" set ::GlobalAnalytPar(par_descr) {parameters of_analytical_size distrib.} -set ::GlobalAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 1 label - LogNorm Sphere None - N = 1.0 R = distr. - s = 0.05 - p = 1.0 - mu = 10.0 eta = 1.0 } -set ::GlobalAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::GlobalAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::GlobalAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::GlobalAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::GlobalAnalytPar(fitSDFF) {yes yes yes yes yes yes yes} -set ::GlobalAnalytPar(SQ,param_count_old) {10 10 10 10 10 10 10} -set ::GlobalAnalytPar(FF,param_count_old) {8 8 8 8 8 8 8} -set ::GlobalAnalytPar(R_VP) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(actual_SD) "7" +set ::GlobalAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 1 label = 1 + Delta triax ellip shell 1 None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 2 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 2 label + Delta triax ellip shell 1t None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 3 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 3 label + Delta triax ellip shell 2 None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 4 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 4 label + Delta triax ellip shell 2t None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 5 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 5 label + Delta triax ellip shell 3 None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 6 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 6 label + Delta triax ellip shell 3t None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 7 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 7 label = 0 + Delta triax ellip shell None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.0 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 8 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 8 label = 0t + Delta triax ellip shell t None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.0 P7 + eta_sol = 0.0 P8 } +set ::GlobalAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::GlobalAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::GlobalAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::GlobalAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::GlobalAnalytPar(fitSDFF) {yes yes yes yes yes yes yes yes} +set ::GlobalAnalytPar(FF,param_count_old) {8 8 8 8 8 8 8 8} +set ::GlobalAnalytPar(SQ,param_count_old) {10 10 10 10 10 10 10 10} +set ::GlobalAnalytPar(R_VP) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(actual_SD) "8" set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(SQ,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} -set ::GlobalAnalytPar(FF,common) {{P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 NONE P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SQ,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::GlobalAnalytPar(FF,common) {{P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 NONE P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} set ::GlobalAnalytPar(alambda) "-1" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(fit) "no" -set ::GlobalAnalytPar(max_SD) "7" +set ::GlobalAnalytPar(max_SD) "8" set ::GlobalAnalytPar(common_names) {NONE NEW P1 P2 P3 P4 P5 P6 P7 P8} -set ::GlobalAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::GlobalAnalytPar(FF,active) {{0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::GlobalAnalytPar(FF,active) {{0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::GlobalAnalytPar(mom_w) ".obW.tab.analytmoments" set ::GlobalAnalytPar(common_i) "8" -set ::GlobalAnalytPar(SQ,param_count) {10 10 10 10 10 10 10 0} -set ::GlobalAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::GlobalAnalytPar(FF,param_count) {8 8 8 8 8 8 8 0} -set ::GlobalAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(SQ,param_count) {10 10 10 10 10 10 10 10} +set ::GlobalAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(FF,param_count) {8 8 8 8 8 8 8 8} +set ::GlobalAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(w_AnalytPar) "" -set ::GlobalAnalytPar(SD,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SD,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar(sumR_VP) "0.0" -set ::GlobalAnalytPar(FF,l) {{10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar(FF,l) {{10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::GlobalAnalytPar(geometrical/datafile) "yes" -set ::GlobalAnalytPar(substrSDFF) {no no no no no no no} +set ::GlobalAnalytPar(substrSDFF) {no no no no no no no no} set ::GlobalAnalytPar(w) "" -set ::GlobalAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::GlobalAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::GlobalAnalytPar(R_RG) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::GlobalAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::GlobalAnalytPar(R_RG) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::GlobalAnalytPar() "0.0" -set ::GlobalAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(R_Ac) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::GlobalAnalytPar(old_actual_SD) "7" -set ::GlobalAnalytPar(dataset) {1 2 3 4 5 6 7} -set ::tmpGlobalAnalytPar(R_lc) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(P1) "10.0" +set ::GlobalAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::GlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(R_Ac) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::GlobalAnalytPar(old_actual_SD) "8" +set ::GlobalAnalytPar(dataset) {1 2 3 4 5 6 7 8} +set ::tmpGlobalAnalytPar(R_lc) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(wR) "0" +set ::tmpGlobalAnalytPar(P1) "10.0" +set ::tmpGlobalAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar(P2) "20.0" -set ::tmpGlobalAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpGlobalAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpGlobalAnalytPar(P3) "30.0" set ::tmpGlobalAnalytPar(sumfp) "0.0" -set ::tmpGlobalAnalytPar(P4) "5.0" -set ::tmpGlobalAnalytPar(SD,param_count) {10 10 10 10 10 10 10 0} -set ::tmpGlobalAnalytPar() "0.0" +set ::tmpGlobalAnalytPar(P3) "30.0" set ::tmpGlobalAnalytPar(resolution) "no" -set ::tmpGlobalAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::tmpGlobalAnalytPar(SD,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::tmpGlobalAnalytPar() "0.0" +set ::tmpGlobalAnalytPar(SD,param_count) {10 10 10 10 10 10 10 10} +set ::tmpGlobalAnalytPar(P4) "5.0" +set ::tmpGlobalAnalytPar(SD,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(SD,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} set ::tmpGlobalAnalytPar(P5) "0.2" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(P6) "1.0" -set ::tmpGlobalAnalytPar(SD,typestr) {Delta Delta Delta Delta Delta Delta LogNorm} -set ::tmpGlobalAnalytPar(fp) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(R_li) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SD,typestr) {Delta Delta Delta Delta Delta Delta Delta Delta} +set ::tmpGlobalAnalytPar(fp) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(R_li) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(alpha) "" -set ::tmpGlobalAnalytPar(calcSDFF) {yes yes yes yes yes yes yes} -set ::tmpGlobalAnalytPar(P7) "0.5" +set ::tmpGlobalAnalytPar(calcSDFF) {yes yes yes yes yes yes yes yes} +set ::tmpGlobalAnalytPar(P7) "0.0" set ::tmpGlobalAnalytPar(sumR_RG) "0.0" -set ::tmpGlobalAnalytPar(SD,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(SD,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar(P8) "0.0" set ::tmpGlobalAnalytPar(par_w) ".obW.tab.analytpar" set ::tmpGlobalAnalytPar(mom_descr) {moments of_analytical_size distrib.} set ::tmpGlobalAnalytPar(sumR_Ac) "0.0" set ::tmpGlobalAnalytPar(covar) "" -set ::tmpGlobalAnalytPar(SD,a) {{1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.2 1.0 5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(SD,a) {{1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.2 1.0 5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {1.0 0.05 1.0 10.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpGlobalAnalytPar(sumR_lc) "0.0" set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(SQ,how) {0 0 0 0 0 0 0} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SQ,how) {0 0 0 0 0 0 0 0} +set ::tmpGlobalAnalytPar(mfit) "0" set ::tmpGlobalAnalytPar(Q) "0" set ::tmpGlobalAnalytPar(error) "0" set ::tmpGlobalAnalytPar(R) "0" -set ::tmpGlobalAnalytPar(SQ,typestr) {None None None None None None None} -set ::tmpGlobalAnalytPar(FF,typestr) {299 300 301 302 303 304 304} +set ::tmpGlobalAnalytPar(SQ,typestr) {None None None None None None None None} +set ::tmpGlobalAnalytPar(FF,typestr) {311 312 313 314 315 316 309 310} set ::tmpGlobalAnalytPar(sumR_li) "0.0" set ::tmpGlobalAnalytPar(reducedchisq) "0" set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(SQ,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::tmpGlobalAnalytPar(FF,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SQ,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::tmpGlobalAnalytPar(FF,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::tmpGlobalAnalytPar(ndata) "12008" set ::tmpGlobalAnalytPar(par_text_export) {description;value;error;factor;global_param;description;value;error;factor;global_param;description;value;error;factor;global_param scattering contribution;1;;;;approximation type;monodisperse approx.;;;;;;;; calculate;yes;;;;substract;no;;;;fit;yes;;; -dataset;1;;;;label;;;;;;;;; -LogNorm;;;;;Sphere;;;;;None;;;; -N;1.0;;;;R;distr.;;;;;;;; -s;0.05;;;;;;;;;;;;; -p;1.0;;;;;;;;;;;;; -mu;10.0;;;;eta;1.0;;;;;;;;} +dataset;1;;;;label;I_1;;;;;;;; +Delta;;;;;triax ellip shell 1;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;2;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;2;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 1t;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;3;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;3;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 2;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;4;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;4;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 2t;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;5;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;5;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 3;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;6;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;6;;;;label;;;;;;;;; +Delta;;;;;triax ellip shell 3t;;;;;None;;;; +N;1.0;;;;a;10.0;;;P1;;;;; +;;;;;b;20.0;;;P2;;;;; +;;;;;c;30.0;;;P3;;;;; +;;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.2;;;P5;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;; +;;;;;;;;;;;;;; +scattering contribution;7;;;;approximation type;monodisperse approx.;;;;;;;; +calculate;yes;;;;substract;no;;;;fit;yes;;; +dataset;7;;;;label;0;;;;;;;; +LogNorm;;;;;triax ellip shell 3t;;;;;None;;;; +N;1.0;;;;a;distr.;;;P1;;;;; +s;0.2;;;;b;20.0;;;P2;;;;; +p;1.0;;;;c;30.0;;;P3;;;;; +mu;5;;;;t;5.0;0.0;;P4;;;;; +;;;;;sigma;0.0;;;;;;;; +;;;;;eta_c;1.0;;;P6;;;;; +;;;;;eta_sh;0.5;;;P7;;;;; +;;;;;eta_sol;0.0;;;P8;;;;;} set ::tmpGlobalAnalytPar(par_x_X) "1.1" -set ::tmpGlobalAnalytPar(datalabel) {I_1 {} {} {} {} {} 0} -set ::tmpGlobalAnalytPar(mom_text_display) {scattering contribution = 1 calculate = yes - LogNorm Sphere - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - R_lc = 0.0000e+000 lc = 0.0000e+000 - R_li = 0.0000e+000 li = 0.0000e+000 - R_Ac = 0.0000e+000 Ac = 0.0000e+000 - R_VP = 0.0000e+000 VP = 0.0000e+000 - R_RG = 0.0000e+000 RG = 0.0000e+000 - fp = 0.0000e+000 - +set ::tmpGlobalAnalytPar(SD,param_count_old) {10 10 10 10 10 10 10 10} +set ::tmpGlobalAnalytPar(mom_text_display) {scattering contribution = 1 calculate = yes + Delta triax ellip shell 1 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 2 calculate = yes + Delta triax ellip shell 1t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 3 calculate = yes + Delta triax ellip shell 2 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 4 calculate = yes + Delta triax ellip shell 2t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 5 calculate = yes + Delta triax ellip shell 3 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 6 calculate = yes + Delta triax ellip shell 3t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + +scattering contribution = 7 calculate = yes + LogNorm triax ellip shell 3t + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + R_lc = 0.0000e+000 lc = 0.0000e+000 + R_li = 0.0000e+000 li = 0.0000e+000 + R_Ac = 0.0000e+000 Ac = 0.0000e+000 + R_VP = 0.0000e+000 VP = 0.0000e+000 + R_RG = 0.0000e+000 RG = 0.0000e+000 + fp = 0.0000e+000 + scattering contribution - of all size distrib. sum N_i = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - = 0.0000e+000 = 0.0000e+000 - sumR_lc = 0.0000e+000 sumlc = 0.0000e+000 - sumR_li = 0.0000e+000 sumli = 0.0000e+000 - sumR_Ac = 0.0000e+000 sumAc = 0.0000e+000 - sumR_VP = 0.0000e+000 sumVP = 0.0000e+000 - sumR_RG = 0.0000e+000 sumRG = 0.0000e+000 - sumfp(Sph.) = 0.0000e+000 } -set ::tmpGlobalAnalytPar(SD,param_count_old) {10 10 10 10 10 10 10} + of all size distrib. sum N_i = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + = 0.0000e+000 = 0.0000e+000 + sumR_lc = 0.0000e+000 sumlc = 0.0000e+000 + sumR_li = 0.0000e+000 sumli = 0.0000e+000 + sumR_Ac = 0.0000e+000 sumAc = 0.0000e+000 + sumR_VP = 0.0000e+000 sumVP = 0.0000e+000 + sumR_RG = 0.0000e+000 sumRG = 0.0000e+000 + sumfp(Sph.) = 0.0000e+000 } +set ::tmpGlobalAnalytPar(datalabel) {1 {} {} {} {} {} 0 0t} set ::tmpGlobalAnalytPar(GraphName) "AnalytPar" -set ::tmpGlobalAnalytPar(SD,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpGlobalAnalytPar(w_MomentsAnalytPar) "" set ::tmpGlobalAnalytPar(isGlobal) "1" +set ::tmpGlobalAnalytPar(w_MomentsAnalytPar) "" +set ::tmpGlobalAnalytPar(SD,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar(mom_text_export) {description;value;description;value scattering contribution;1;calculate;yes -LogNorm;;Sphere; +Delta;;triax ellip shell 1; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;2;calculate;yes +Delta;;triax ellip shell 1t; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;3;calculate;yes +Delta;;triax ellip shell 2; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;4;calculate;yes +Delta;;triax ellip shell 2t; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;5;calculate;yes +Delta;;triax ellip shell 3; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;6;calculate;yes +Delta;;triax ellip shell 3t; +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +;0.0000e+000;;0.0000e+000 +R_lc;0.0000e+000;lc;0.0000e+000 +R_li;0.0000e+000;li;0.0000e+000 +R_Ac;0.0000e+000;Ac;0.0000e+000 +R_VP;0.0000e+000;VP;0.0000e+000 +R_RG;0.0000e+000;RG;0.0000e+000 +fp;0.0000e+000;; +;;; +scattering contribution;7;calculate;yes +LogNorm;;triax ellip shell 3t; ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 ;0.0000e+000;;0.0000e+000 @@ -606,65 +1218,147 @@ sumR_VP;0.0000e+000;sumVP;0.0000e+000 sumR_RG;0.0000e+000;sumRG;0.0000e+000 sumfp(Sph.);0.0000e+000;;} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar(file) "unknown.par" -set ::tmpGlobalAnalytPar(chisq) "0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar() "0.0" +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(chisq) "0" +set ::tmpGlobalAnalytPar(file) "unknown.par" set ::tmpGlobalAnalytPar(varianceOFfit) "0" set ::tmpGlobalAnalytPar(par_descr) {parameters of_analytical_size distrib.} -set ::tmpGlobalAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::tmpGlobalAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::tmpGlobalAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. - calculate = yes substract = no fit = yes - dataset = 1 label - LogNorm Sphere None - N = 1.0 R = distr. - s = 0.05 - p = 1.0 - mu = 10.0 eta = 1.0 } -set ::tmpGlobalAnalytPar(fitSDFF) {yes yes yes yes yes yes yes} -set ::tmpGlobalAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::tmpGlobalAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::tmpGlobalAnalytPar(R_VP) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(SQ,param_count_old) {10 10 10 10 10 10 10} -set ::tmpGlobalAnalytPar(FF,param_count_old) {8 8 8 8 8 8 8} +set ::tmpGlobalAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 1 label = I_1 + Delta triax ellip shell 1 None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 2 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 2 label + Delta triax ellip shell 1t None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 3 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 3 label + Delta triax ellip shell 2 None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 4 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 4 label + Delta triax ellip shell 2t None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 5 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 5 label + Delta triax ellip shell 3 None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 6 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 6 label + Delta triax ellip shell 3t None + N = 1.0 a = 10.0 P1 + b = 20.0 P2 + c = 30.0 P3 + t = 5.0 ± 0.0 P4 + sigma = 0.2 P5 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 + +scattering contribution = 7 approximation type = monodisperse approx. + calculate = yes substract = no fit = yes + dataset = 7 label = 0 + LogNorm triax ellip shell 3t None + N = 1.0 a = distr. P1 + s = 0.2 b = 20.0 P2 + p = 1.0 c = 30.0 P3 + mu = 5 t = 5.0 ± 0.0 P4 + sigma = 0.0 + eta_c = 1.0 P6 + eta_sh = 0.5 P7 + eta_sol = 0.0 P8 } +set ::tmpGlobalAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpGlobalAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpGlobalAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpGlobalAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpGlobalAnalytPar(fitSDFF) {yes yes yes yes yes yes yes yes} +set ::tmpGlobalAnalytPar(FF,param_count_old) {8 8 8 8 8 8 8 8} +set ::tmpGlobalAnalytPar(SQ,param_count_old) {10 10 10 10 10 10 10 10} +set ::tmpGlobalAnalytPar(R_VP) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(actual_SD) "7" -set ::tmpGlobalAnalytPar(FF,common) {{P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 NONE P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} -set ::tmpGlobalAnalytPar(SQ,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SQ,common) {{NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} +set ::tmpGlobalAnalytPar(FF,common) {{P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 NONE P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE} {P1 P2 P3 P4 P5 P6 P7 P8 NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE NONE}} set ::tmpGlobalAnalytPar(alambda) "-1" +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(fit) "no" -set ::tmpGlobalAnalytPar(FF,active) {{0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpGlobalAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpGlobalAnalytPar(max_SD) "7" set ::tmpGlobalAnalytPar(common_names) {NONE NEW P1 P2 P3 P4 P5 P6 P7 P8} +set ::tmpGlobalAnalytPar(max_SD) "8" +set ::tmpGlobalAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpGlobalAnalytPar(FF,active) {{0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0} {0 0 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpGlobalAnalytPar(mom_w) ".obW.tab.analytmoments" -set ::tmpGlobalAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} -set ::tmpGlobalAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(FF,param_count) {8 8 8 8 8 8 8 8} +set ::tmpGlobalAnalytPar(SQ,param_count) {10 10 10 10 10 10 10 10} set ::tmpGlobalAnalytPar(common_i) "8" -set ::tmpGlobalAnalytPar(SQ,param_count) {10 10 10 10 10 10 10 0} -set ::tmpGlobalAnalytPar(FF,param_count) {8 8 8 8 8 8 8 0} -set ::tmpGlobalAnalytPar(SD,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} -set ::tmpGlobalAnalytPar(w_AnalytPar) "" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(SQ,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(FF,err) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(FF,l) {{10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(w_AnalytPar) "" +set ::tmpGlobalAnalytPar(SD,factor) {{1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1} {1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1}} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(sumR_VP) "0.0" +set ::tmpGlobalAnalytPar(FF,l) {{10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.0 1.0 0.5 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {10.0 20.0 30.0 5.0 0.2 1.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} set ::tmpGlobalAnalytPar(geometrical/datafile) "yes" -set ::tmpGlobalAnalytPar(substrSDFF) {no no no no no no no} -set ::tmpGlobalAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpGlobalAnalytPar(substrSDFF) {no no no no no no no no} set ::tmpGlobalAnalytPar(w) "" -set ::tmpGlobalAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::tmpGlobalAnalytPar(R_RG) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200} {-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpGlobalAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200} {1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpGlobalAnalytPar(R_RG) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar() "0.0" -set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(R_Ac) {0.0 0.0 0.0 0.0 0.0 0.0 0.0} -set ::tmpGlobalAnalytPar(dataset) {1 2 3 4 5 6 7} +set ::tmpGlobalAnalytPar(SQ,s) {{100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} {100.0 0.2 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::tmpGlobalAnalytPar() {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} +set ::tmpGlobalAnalytPar(R_Ac) {0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0} set ::tmpGlobalAnalytPar(old_actual_SD) "7" +set ::tmpGlobalAnalytPar(dataset) {1 2 3 4 5 6 7 8} set ::actualGlobalAnalytPar(SQ,s8,common) "NONE" set ::actualGlobalAnalytPar(P1) "10.0" set ::actualGlobalAnalytPar(SQ,s1,var) "100.0" @@ -677,40 +1371,40 @@ set ::actualGlobalAnalytPar(sumfp) "0.0" set ::actualGlobalAnalytPar(P4) "5.0" set ::actualGlobalAnalytPar(P5) "0.2" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(P6) "1.0" -set ::actualGlobalAnalytPar(SD,a2,min) "-1e+200" set ::actualGlobalAnalytPar(fp) "0.0" -set ::actualGlobalAnalytPar(P7) "0.5" +set ::actualGlobalAnalytPar(SD,a2,min) "-1e+200" +set ::actualGlobalAnalytPar(P6) "1.0" set ::actualGlobalAnalytPar(FF,l6,var) "1.0" -set ::actualGlobalAnalytPar(P8) "0.0" +set ::actualGlobalAnalytPar(P7) "0.0" set ::actualGlobalAnalytPar(SD,a10,factor) "1" +set ::actualGlobalAnalytPar(P8) "0.0" set ::actualGlobalAnalytPar(SQ,s9,var) "0.0" -set ::actualGlobalAnalytPar(SD,a4,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s4,factor) "1" -set ::actualGlobalAnalytPar(SD,a7,distr) "0" -set ::actualGlobalAnalytPar(SD,a6,factor) "1" +set ::actualGlobalAnalytPar(SD,a4,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s2,min) "-1e+200" -set ::actualGlobalAnalytPar(SQ,s6,common) "NONE" +set ::actualGlobalAnalytPar(SD,a6,factor) "1" +set ::actualGlobalAnalytPar(SD,a7,distr) "0" set ::actualGlobalAnalytPar() "0.0" +set ::actualGlobalAnalytPar(SQ,s6,common) "NONE" set ::actualGlobalAnalytPar(FF,l1,max) "1e+200" -set ::actualGlobalAnalytPar(SD,a8,common) "NONE" -set ::actualGlobalAnalytPar(SQ,s6,active) "0" set ::actualGlobalAnalytPar(SQ,s4,max) "1e+200" +set ::actualGlobalAnalytPar(SQ,s6,active) "0" +set ::actualGlobalAnalytPar(SD,a8,common) "NONE" set ::actualGlobalAnalytPar(FF,l2,label) {b =} set ::actualGlobalAnalytPar(SD,a10,var) "0.0" -set ::actualGlobalAnalytPar(SQ,typestr) "None" set ::actualGlobalAnalytPar(FF,l7,min) "-1e+200" +set ::actualGlobalAnalytPar(SQ,typestr) "None" set ::actualGlobalAnalytPar(SD,a8,active) "0" set ::actualGlobalAnalytPar(SD,a4,err) "0.0" set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(SQ,s2,factor) "1" set ::actualGlobalAnalytPar(SQ,s8,limits) "0" -set ::actualGlobalAnalytPar(SD,a10,common) "NONE" set ::actualGlobalAnalytPar(FF,l1,err) "0.0" +set ::actualGlobalAnalytPar(SD,a10,common) "NONE" set ::actualGlobalAnalytPar(SD,a4,factor) "1" -set ::actualGlobalAnalytPar(SD,a6,distr) "0" -set ::actualGlobalAnalytPar(SQ,s4,common) "NONE" set ::actualGlobalAnalytPar(SQ,s4,err) "0.0" +set ::actualGlobalAnalytPar(SQ,s4,common) "NONE" +set ::actualGlobalAnalytPar(SD,a6,distr) "0" set ::actualGlobalAnalytPar(SD,a10,active) "0" set ::actualGlobalAnalytPar(SD,a6,common) "NONE" set ::actualGlobalAnalytPar(SD,a6,var) "0.0" @@ -860,72 +1554,72 @@ set ::actualGlobalAnalytPar(SD,a7,factor) "1" set ::actualGlobalAnalytPar(SQ,s8,label) "" set ::actualGlobalAnalytPar(SQ,s7,common) "NONE" set ::actualGlobalAnalytPar(SQ,s10,err) "0.0" -set ::actualGlobalAnalytPar(SD,a9,common) "NONE" -set ::actualGlobalAnalytPar(SD,a6,min) "-1e+200" set ::actualGlobalAnalytPar(SQ,s7,active) "0" -set ::actualGlobalAnalytPar(SD,a4,label) {mu =} +set ::actualGlobalAnalytPar(SD,a6,min) "-1e+200" +set ::actualGlobalAnalytPar(SD,a9,common) "NONE" +set ::actualGlobalAnalytPar(SD,a4,label) "" set ::actualGlobalAnalytPar(SD,a9,active) "0" -set ::actualGlobalAnalytPar(datasetlabel) {1 2 3 4 5 6 7 8} set ::actualGlobalAnalytPar(SD,a8,max) "1e+200" -set ::actualGlobalAnalytPar(SQ,s2,distr) "0" +set ::actualGlobalAnalytPar(datasetlabel) {1 2 3 4 5 6 7 8} set ::actualGlobalAnalytPar(FF,l3,min) "-1e+200" -set ::actualGlobalAnalytPar(SQ,s6,min) "-1e+200" +set ::actualGlobalAnalytPar(SQ,s2,distr) "0" set ::actualGlobalAnalytPar(SQ,s3,factor) "1" -set ::actualGlobalAnalytPar(error) "0" +set ::actualGlobalAnalytPar(SQ,s6,min) "-1e+200" set ::actualGlobalAnalytPar(SQ,s9,limits) "0" -set ::actualGlobalAnalytPar(FF,typestr) "304" -set ::actualGlobalAnalytPar(FF,l5,max) "1e+200" +set ::actualGlobalAnalytPar(error) "0" set ::actualGlobalAnalytPar(FF,l5,distr) "0" -set ::actualGlobalAnalytPar(SD,a5,factor) "1" +set ::actualGlobalAnalytPar(FF,l5,max) "1e+200" +set ::actualGlobalAnalytPar(FF,typestr) "309" set ::actualGlobalAnalytPar(reducedchisq) "0" -set ::actualGlobalAnalytPar(SQ,s8,max) "1e+200" +set ::actualGlobalAnalytPar(SD,a5,factor) "1" set ::actualGlobalAnalytPar(SQ,s5,common) "NONE" +set ::actualGlobalAnalytPar(SQ,s8,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s7,label) "" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(SD,a7,common) "NONE" set ::actualGlobalAnalytPar(SQ,s5,active) "0" +set ::actualGlobalAnalytPar(SD,a7,common) "NONE" set ::actualGlobalAnalytPar(SD,a8,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s10,limits) "0" set ::actualGlobalAnalytPar(datalabel) "0" -set ::actualGlobalAnalytPar(SD,a3,label) {p =} -set ::actualGlobalAnalytPar(SD,a7,active) "0" +set ::actualGlobalAnalytPar(SQ,s10,limits) "0" +set ::actualGlobalAnalytPar(SD,a3,label) "" set ::actualGlobalAnalytPar(SD,a2,var) "0.2" -set ::actualGlobalAnalytPar(SQ,s1,distr) "0" +set ::actualGlobalAnalytPar(SD,a7,active) "0" set ::actualGlobalAnalytPar(FF,l5,err) "0.0" +set ::actualGlobalAnalytPar(SQ,s1,distr) "0" set ::actualGlobalAnalytPar(SQ,s1,factor) "1" -set ::actualGlobalAnalytPar(SQ,s8,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s7,limits) "0" set ::actualGlobalAnalytPar() "0.0" +set ::actualGlobalAnalytPar(SQ,s7,limits) "0" +set ::actualGlobalAnalytPar(SQ,s8,err) "0.0" set ::actualGlobalAnalytPar(varianceOFfit) "0" -set ::actualGlobalAnalytPar(SD,a3,factor) "1" -set ::actualGlobalAnalytPar(FF,l4,distr) "0" set ::actualGlobalAnalytPar(SQ,s2,var) "0.2" -set ::actualGlobalAnalytPar(SD,a9,limits) "0" +set ::actualGlobalAnalytPar(FF,l4,distr) "0" +set ::actualGlobalAnalytPar(SD,a3,factor) "1" set ::actualGlobalAnalytPar(SQ,s3,common) "NONE" +set ::actualGlobalAnalytPar(SD,a9,limits) "0" set ::actualGlobalAnalytPar(SQ,s6,label) "" -set ::actualGlobalAnalytPar(SD,a5,common) "NONE" set ::actualGlobalAnalytPar(SQ,s3,active) "0" -set ::actualGlobalAnalytPar(SD,a3,min) "-1e+200" +set ::actualGlobalAnalytPar(SD,a5,common) "NONE" set ::actualGlobalAnalytPar(FF,l8,factor) "1" +set ::actualGlobalAnalytPar(SD,a3,min) "-1e+200" +set ::actualGlobalAnalytPar(FF,l7,var) "0.0" set ::actualGlobalAnalytPar(actual_SD) "7" -set ::actualGlobalAnalytPar(FF,l7,var) "0.5" -set ::actualGlobalAnalytPar(SD,a5,active) "0" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(SD,a2,label) {s =} +set ::actualGlobalAnalytPar(SD,a5,active) "0" +set ::actualGlobalAnalytPar(SD,a2,label) "" set ::actualGlobalAnalytPar(SD,a5,max) "1e+200" -set ::actualGlobalAnalytPar(SQ,s5,limits) "0" set ::actualGlobalAnalytPar(SQ,s3,min) "-1e+200" -set ::actualGlobalAnalytPar(SD,a1,factor) "1" +set ::actualGlobalAnalytPar(SQ,s5,limits) "0" set ::actualGlobalAnalytPar(FF,l2,max) "1e+200" -set ::actualGlobalAnalytPar(SD,a7,limits) "0" -set ::actualGlobalAnalytPar(FF,l3,distr) "0" +set ::actualGlobalAnalytPar(SD,a1,factor) "1" set ::actualGlobalAnalytPar(SQ,s1,common) "NONE" -set ::actualGlobalAnalytPar(SQ,s5,max) "1e+200" +set ::actualGlobalAnalytPar(FF,l3,distr) "0" +set ::actualGlobalAnalytPar(SD,a7,limits) "0" set ::actualGlobalAnalytPar() "0.0" +set ::actualGlobalAnalytPar(SQ,s5,max) "1e+200" set ::actualGlobalAnalytPar(SQ,s5,label) "" -set ::actualGlobalAnalytPar(SD,a3,common) "NONE" -set ::actualGlobalAnalytPar(FF,l8,min) "-1e+200" set ::actualGlobalAnalytPar(SQ,s1,active) "0" +set ::actualGlobalAnalytPar(FF,l8,min) "-1e+200" +set ::actualGlobalAnalytPar(SD,a3,common) "NONE" set ::actualGlobalAnalytPar(FF,l6,factor) "1" set ::actualGlobalAnalytPar(SD,a5,err) "0.0" set ::actualGlobalAnalytPar(SD,a3,active) "0" @@ -933,77 +1627,77 @@ set ::actualGlobalAnalytPar(FF,l8,label) {eta_sol =} set ::actualGlobalAnalytPar(SD,a1,label) {N =} set ::actualGlobalAnalytPar(FF,l8,common) "P8" set ::actualGlobalAnalytPar(R_RG) "0.0" -set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l2,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s10,min) "-1e+200" -set ::actualGlobalAnalytPar(SQ,s3,limits) "0" +set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l8,active) "0" +set ::actualGlobalAnalytPar(SQ,s3,limits) "0" +set ::actualGlobalAnalytPar(SQ,s10,min) "-1e+200" set ::actualGlobalAnalytPar(SQ,s5,err) "0.0" set ::actualGlobalAnalytPar(dataset) "7" set ::actualGlobalAnalytPar(SD,a5,limits) "0" -set ::actualGlobalAnalytPar(SD,a7,var) "0.0" -set ::actualGlobalAnalytPar(R_lc) "0.0" set ::actualGlobalAnalytPar(FF,l2,distr) "0" +set ::actualGlobalAnalytPar(R_lc) "0.0" +set ::actualGlobalAnalytPar(SD,a7,var) "0.0" set ::actualGlobalAnalytPar(SD,a1,common) "NONE" set ::actualGlobalAnalytPar(SQ,s4,label) "" set ::actualGlobalAnalytPar(FF,l4,factor) "1" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(SD,a1,active) "0" set ::actualGlobalAnalytPar(FF,l4,var) "5.0" -set ::actualGlobalAnalytPar(SD,typestr) "LogNorm" +set ::actualGlobalAnalytPar(SD,a1,active) "0" set ::actualGlobalAnalytPar(R_li) "0.0" +set ::actualGlobalAnalytPar(SD,typestr) "Delta" set ::actualGlobalAnalytPar(FF,l7,label) {eta_sh =} -set ::actualGlobalAnalytPar(SQ,s7,var) "0.0" -set ::actualGlobalAnalytPar(sumR_RG) "0.0" set ::actualGlobalAnalytPar(FF,l6,common) "P6" +set ::actualGlobalAnalytPar(sumR_RG) "0.0" +set ::actualGlobalAnalytPar(SQ,s7,var) "0.0" set ::actualGlobalAnalytPar(SD,a2,max) "1e+200" set ::actualGlobalAnalytPar(plottype) "-1" -set ::actualGlobalAnalytPar(FF,l6,active) "0" set ::actualGlobalAnalytPar(SQ,s1,limits) "0" +set ::actualGlobalAnalytPar(FF,l6,active) "0" set ::actualGlobalAnalytPar(SD,a8,min) "-1e+200" -set ::actualGlobalAnalytPar(SD,a3,limits) "0" -set ::actualGlobalAnalytPar(sumR_lc) "0.0" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(FF,l1,distr) "1" +set ::actualGlobalAnalytPar(sumR_lc) "0.0" +set ::actualGlobalAnalytPar(SD,a3,limits) "0" set ::actualGlobalAnalytPar(SQ,s2,max) "1e+200" -set ::actualGlobalAnalytPar(FF,l2,factor) "1" +set ::actualGlobalAnalytPar(FF,l1,distr) "0" set ::actualGlobalAnalytPar(FF,l5,min) "-1e+200" +set ::actualGlobalAnalytPar(FF,l2,factor) "1" set ::actualGlobalAnalytPar(SQ,s3,label) "" set ::actualGlobalAnalytPar(FF,l8,limits) "0" -set ::actualGlobalAnalytPar(SD,a2,err) "0.0" -set ::actualGlobalAnalytPar(SQ,s8,min) "-1e+200" set ::actualGlobalAnalytPar(sumR_li) "0.0" -set ::actualGlobalAnalytPar(FF,l4,common) "P4" +set ::actualGlobalAnalytPar(SQ,s8,min) "-1e+200" +set ::actualGlobalAnalytPar(SD,a2,err) "0.0" set ::actualGlobalAnalytPar(FF,l7,max) "1e+200" +set ::actualGlobalAnalytPar(FF,l4,common) "P4" set ::actualGlobalAnalytPar(FF,l6,label) {eta_c =} set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l4,active) "1" -set ::actualGlobalAnalytPar(SD,param_count_old) "10" set ::actualGlobalAnalytPar(SQ,s2,err) "0.0" +set ::actualGlobalAnalytPar(SD,param_count_old) "10" set ::actualGlobalAnalytPar(SD,a1,limits) "0" set ::actualGlobalAnalytPar(SD,a4,var) "5" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(FF,l6,limits) "0" set ::actualGlobalAnalytPar(FF,l7,err) "0.0" +set ::actualGlobalAnalytPar(FF,l6,limits) "0" set ::actualGlobalAnalytPar(SQ,s2,label) "" set ::actualGlobalAnalytPar(FF,l1,var) "10.0" set ::actualGlobalAnalytPar(FF,l2,common) "P2" set ::actualGlobalAnalytPar(SQ,s4,var) "0.0" set ::actualGlobalAnalytPar(FF,l5,label) {sigma =} -set ::actualGlobalAnalytPar(fitSDFF) "yes" set ::actualGlobalAnalytPar(FF,l2,active) "0" -set ::actualGlobalAnalytPar(FF,param_count_old) "8" +set ::actualGlobalAnalytPar(fitSDFF) "yes" set ::actualGlobalAnalytPar(R_VP) "0.0" +set ::actualGlobalAnalytPar(FF,param_count_old) "8" set ::actualGlobalAnalytPar(SD,a5,min) "-1e+200" -set ::actualGlobalAnalytPar(alambda) "-1" set ::actualGlobalAnalytPar() "0.0" -set ::actualGlobalAnalytPar(max_SD) "7" +set ::actualGlobalAnalytPar(alambda) "-1" set ::actualGlobalAnalytPar(common_names) {NONE NEW P1 P2 P3 P4 P5 P6 P7 P8} +set ::actualGlobalAnalytPar(max_SD) "8" set ::actualGlobalAnalytPar(SD,a7,max) "1e+200" -set ::actualGlobalAnalytPar(SQ,s10,distr) "0" -set ::actualGlobalAnalytPar(SQ,s8,factor) "1" -set ::actualGlobalAnalytPar(FF,l2,min) "-1e+200" set ::actualGlobalAnalytPar(FF,l4,limits) "0" +set ::actualGlobalAnalytPar(FF,l2,min) "-1e+200" +set ::actualGlobalAnalytPar(SQ,s8,factor) "1" +set ::actualGlobalAnalytPar(SQ,s10,distr) "0" set ::actualGlobalAnalytPar(SD,a9,distr) "0" set ::actualGlobalAnalytPar(SQ,s1,label) "" set ::actualGlobalAnalytPar(SQ,s5,min) "-1e+200" @@ -1011,19 +1705,19 @@ set ::actualGlobalAnalytPar(SQ,param_count) "10" set ::actualGlobalAnalytPar(FF,l4,max) "1e+200" set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l4,label) {t =} -set ::actualGlobalAnalytPar(SQ,s7,max) "1e+200" set ::actualGlobalAnalytPar(sumR_VP) "0.0" +set ::actualGlobalAnalytPar(SQ,s7,max) "1e+200" set ::actualGlobalAnalytPar(substrSDFF) "no" set ::actualGlobalAnalytPar(SD,a7,err) "0.0" set ::actualGlobalAnalytPar(SD,a1,var) "1.0" -set ::actualGlobalAnalytPar(SQ,s6,factor) "1" -set ::actualGlobalAnalytPar() "0.0" set ::actualGlobalAnalytPar(FF,l2,limits) "0" +set ::actualGlobalAnalytPar() "0.0" +set ::actualGlobalAnalytPar(SQ,s6,factor) "1" set ::actualGlobalAnalytPar(FF,l4,err) "0.0" set ::actualGlobalAnalytPar(SD,a8,distr) "0" -set ::actualGlobalAnalytPar(SD,a10,distr) "0" -set ::actualGlobalAnalytPar(SD,a8,factor) "1" set ::actualGlobalAnalytPar(SQ,s7,err) "0.0" +set ::actualGlobalAnalytPar(SD,a8,factor) "1" +set ::actualGlobalAnalytPar(SD,a10,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s8,common) "NONE" set ::tmpactualGlobalAnalytPar(P1) "10.0" set ::tmpactualGlobalAnalytPar(SQ,s1,var) "100.0" @@ -1035,42 +1729,42 @@ set ::tmpactualGlobalAnalytPar(FF,l3,label) {c =} set ::tmpactualGlobalAnalytPar(sumfp) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s8,active) "0" set ::tmpactualGlobalAnalytPar(P4) "5.0" -set ::tmpactualGlobalAnalytPar(P5) "0.2" -set ::tmpactualGlobalAnalytPar(FF,l10,active) "0" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(P6) "1.0" -set ::tmpactualGlobalAnalytPar(fp) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l10,active) "0" +set ::tmpactualGlobalAnalytPar(P5) "0.2" set ::tmpactualGlobalAnalytPar(SD,a2,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(P7) "0.5" +set ::tmpactualGlobalAnalytPar(fp) "0.0" +set ::tmpactualGlobalAnalytPar(P6) "1.0" set ::tmpactualGlobalAnalytPar(FF,l6,var) "1.0" -set ::tmpactualGlobalAnalytPar(P8) "0.0" +set ::tmpactualGlobalAnalytPar(P7) "0.0" set ::tmpactualGlobalAnalytPar(SD,a10,factor) "1" +set ::tmpactualGlobalAnalytPar(P8) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s9,var) "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s4,factor) "1" set ::tmpactualGlobalAnalytPar(SD,a4,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SD,a7,distr) "0" -set ::tmpactualGlobalAnalytPar(SQ,s2,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s4,factor) "1" set ::tmpactualGlobalAnalytPar(SD,a6,factor) "1" -set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(SQ,s2,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SD,a7,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s6,common) "NONE" +set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(FF,l1,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s4,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s6,active) "0" set ::tmpactualGlobalAnalytPar(SD,a8,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l2,label) {b =} +set ::tmpactualGlobalAnalytPar(SQ,s6,active) "0" +set ::tmpactualGlobalAnalytPar(SQ,s4,max) "1e+200" set ::tmpactualGlobalAnalytPar(SD,a10,var) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l7,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(FF,l2,label) {b =} set ::tmpactualGlobalAnalytPar(SQ,typestr) "None" +set ::tmpactualGlobalAnalytPar(FF,l7,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SD,a8,active) "0" set ::tmpactualGlobalAnalytPar(SD,a4,err) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l9,max) "1e+200" set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l9,max) "1e+200" set ::tmpactualGlobalAnalytPar(SQ,s2,factor) "1" set ::tmpactualGlobalAnalytPar(SQ,s8,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l1,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a10,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l10,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l1,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a4,factor) "1" +set ::tmpactualGlobalAnalytPar(FF,l10,limits) "0" set ::tmpactualGlobalAnalytPar(SD,a6,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s4,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s4,err) "0.0" @@ -1214,195 +1908,195 @@ set ::tmpactualGlobalAnalytPar(SQ,s9,active) "0" set ::tmpactualGlobalAnalytPar(datalabel,7) "0" set ::tmpactualGlobalAnalytPar(SD,a10,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SD,a5,label) "" +set ::tmpactualGlobalAnalytPar(old_actual_SD) "7" +set ::tmpactualGlobalAnalytPar(SQ,s10,max) "1e+200" set ::tmpactualGlobalAnalytPar(datalabel,8) "0t" set ::tmpactualGlobalAnalytPar(SD,a5,var) "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s10,max) "1e+200" -set ::tmpactualGlobalAnalytPar(old_actual_SD) "7" set ::tmpactualGlobalAnalytPar(SQ,s3,distr) "0" -set ::tmpactualGlobalAnalytPar(SQ,s10,common) "NONE" -set ::tmpactualGlobalAnalytPar(wR) "0" set ::tmpactualGlobalAnalytPar(FF,l8,err) "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s5,factor) "1" -set ::tmpactualGlobalAnalytPar(FF,l1,limits) "0" +set ::tmpactualGlobalAnalytPar(wR) "0" +set ::tmpactualGlobalAnalytPar(SQ,s10,common) "NONE" set ::tmpactualGlobalAnalytPar(FF,l2,var) "20.0" -set ::tmpactualGlobalAnalytPar(SD,param_count) "10" -set ::tmpactualGlobalAnalytPar(SQ,s10,active) "0" +set ::tmpactualGlobalAnalytPar(FF,l1,limits) "0" +set ::tmpactualGlobalAnalytPar(SQ,s5,factor) "1" set ::tmpactualGlobalAnalytPar(FF,l6,distr) "0" +set ::tmpactualGlobalAnalytPar(SQ,s10,active) "0" +set ::tmpactualGlobalAnalytPar(SD,param_count) "10" set ::tmpactualGlobalAnalytPar(SQ,s5,var) "0.0" set ::tmpactualGlobalAnalytPar(SD,a7,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s7,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s8,label) "" +set ::tmpactualGlobalAnalytPar(SQ,s7,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s10,err) "0.0" -set ::tmpactualGlobalAnalytPar(SD,a9,common) "NONE" -set ::tmpactualGlobalAnalytPar(SD,a6,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s7,active) "0" -set ::tmpactualGlobalAnalytPar(SD,a4,label) {mu =} +set ::tmpactualGlobalAnalytPar(SD,a6,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SD,a9,common) "NONE" +set ::tmpactualGlobalAnalytPar(SD,a4,label) "" set ::tmpactualGlobalAnalytPar(SD,a9,active) "0" -set ::tmpactualGlobalAnalytPar(datasetlabel) {1 2 3 4 5 6 7 8} set ::tmpactualGlobalAnalytPar(SD,a8,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s2,distr) "0" +set ::tmpactualGlobalAnalytPar(datasetlabel) {1 2 3 4 5 6 7 8} set ::tmpactualGlobalAnalytPar(FF,l3,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s3,factor) "1" +set ::tmpactualGlobalAnalytPar(SQ,s2,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s6,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s9,limits) "0" +set ::tmpactualGlobalAnalytPar(SQ,s3,factor) "1" set ::tmpactualGlobalAnalytPar(error) "0" -set ::tmpactualGlobalAnalytPar(FF,l5,distr) "0" +set ::tmpactualGlobalAnalytPar(SQ,s9,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,typestr) "309" set ::tmpactualGlobalAnalytPar(FF,l5,max) "1e+200" -set ::tmpactualGlobalAnalytPar(FF,typestr) "304" -set ::tmpactualGlobalAnalytPar(reducedchisq) "0" +set ::tmpactualGlobalAnalytPar(FF,l5,distr) "0" set ::tmpactualGlobalAnalytPar(SD,a5,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s5,common) "NONE" +set ::tmpactualGlobalAnalytPar(reducedchisq) "0" set ::tmpactualGlobalAnalytPar(SQ,s8,max) "1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s5,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s7,label) "" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s5,active) "0" set ::tmpactualGlobalAnalytPar(SD,a7,common) "NONE" +set ::tmpactualGlobalAnalytPar(SQ,s5,active) "0" set ::tmpactualGlobalAnalytPar(SD,a8,err) "0.0" -set ::tmpactualGlobalAnalytPar(datalabel) "0" set ::tmpactualGlobalAnalytPar(SQ,s10,limits) "0" -set ::tmpactualGlobalAnalytPar(SD,a3,label) {p =} -set ::tmpactualGlobalAnalytPar(SD,a2,var) "0.05" +set ::tmpactualGlobalAnalytPar(datalabel) "0" set ::tmpactualGlobalAnalytPar(SD,a7,active) "0" -set ::tmpactualGlobalAnalytPar(SQ,s1,distr) "0" +set ::tmpactualGlobalAnalytPar(SD,a2,var) "0.2" +set ::tmpactualGlobalAnalytPar(SD,a3,label) "" set ::tmpactualGlobalAnalytPar(FF,l5,err) "0.0" +set ::tmpactualGlobalAnalytPar(SQ,s1,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s1,factor) "1" -set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s7,limits) "0" set ::tmpactualGlobalAnalytPar(SQ,s8,err) "0.0" +set ::tmpactualGlobalAnalytPar(SQ,s7,limits) "0" +set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(varianceOFfit) "0" -set ::tmpactualGlobalAnalytPar(SQ,s2,var) "0.2" -set ::tmpactualGlobalAnalytPar(FF,l4,distr) "0" set ::tmpactualGlobalAnalytPar(SD,a3,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s3,common) "NONE" +set ::tmpactualGlobalAnalytPar(FF,l4,distr) "0" +set ::tmpactualGlobalAnalytPar(SQ,s2,var) "0.2" set ::tmpactualGlobalAnalytPar(SD,a9,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l10,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s3,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s6,label) "" -set ::tmpactualGlobalAnalytPar(SQ,s3,active) "0" +set ::tmpactualGlobalAnalytPar(FF,l10,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SD,a5,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l10,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,l8,factor) "1" +set ::tmpactualGlobalAnalytPar(SQ,s3,active) "0" set ::tmpactualGlobalAnalytPar(SD,a3,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(FF,l7,var) "0.5" +set ::tmpactualGlobalAnalytPar(FF,l8,factor) "1" +set ::tmpactualGlobalAnalytPar(FF,l10,distr) "0" set ::tmpactualGlobalAnalytPar(actual_SD) "7" -set ::tmpactualGlobalAnalytPar(FF,l9,label) "" -set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l7,var) "0.0" set ::tmpactualGlobalAnalytPar(SD,a5,active) "0" -set ::tmpactualGlobalAnalytPar(SD,a2,label) {s =} +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l9,label) "" +set ::tmpactualGlobalAnalytPar(SD,a2,label) "" set ::tmpactualGlobalAnalytPar(SD,a5,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s3,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s5,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l2,max) "1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s3,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SD,a1,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s1,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l3,distr) "0" +set ::tmpactualGlobalAnalytPar(FF,l2,max) "1e+200" set ::tmpactualGlobalAnalytPar(SD,a7,limits) "0" -set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l3,distr) "0" +set ::tmpactualGlobalAnalytPar(SQ,s1,common) "NONE" set ::tmpactualGlobalAnalytPar(SQ,s5,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s1,active) "0" -set ::tmpactualGlobalAnalytPar(FF,l8,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s5,label) "" +set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(SD,a3,common) "NONE" +set ::tmpactualGlobalAnalytPar(SQ,s5,label) "" +set ::tmpactualGlobalAnalytPar(FF,l8,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s1,active) "0" set ::tmpactualGlobalAnalytPar(FF,l6,factor) "1" set ::tmpactualGlobalAnalytPar(SD,a5,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a3,active) "0" set ::tmpactualGlobalAnalytPar(FF,l8,label) {eta_sol =} -set ::tmpactualGlobalAnalytPar(FF,l8,common) "P8" set ::tmpactualGlobalAnalytPar(SD,a1,label) {N =} +set ::tmpactualGlobalAnalytPar(FF,l8,common) "P8" set ::tmpactualGlobalAnalytPar(R_RG) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l2,err) "0.0" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l8,active) "0" -set ::tmpactualGlobalAnalytPar(SQ,s3,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l2,err) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s10,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s3,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l8,active) "0" set ::tmpactualGlobalAnalytPar(SQ,s5,err) "0.0" set ::tmpactualGlobalAnalytPar(dataset) "7" set ::tmpactualGlobalAnalytPar(SD,a5,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l2,distr) "0" -set ::tmpactualGlobalAnalytPar(R_lc) "0.0" set ::tmpactualGlobalAnalytPar(SD,a7,var) "0.0" +set ::tmpactualGlobalAnalytPar(R_lc) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l2,distr) "0" set ::tmpactualGlobalAnalytPar(SD,a1,common) "NONE" -set ::tmpactualGlobalAnalytPar(FF,l4,factor) "1" set ::tmpactualGlobalAnalytPar(SQ,s4,label) "" +set ::tmpactualGlobalAnalytPar(FF,l4,factor) "1" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l4,var) "5.0" set ::tmpactualGlobalAnalytPar(SD,a1,active) "0" +set ::tmpactualGlobalAnalytPar(FF,l4,var) "5.0" +set ::tmpactualGlobalAnalytPar(SD,typestr) "Delta" set ::tmpactualGlobalAnalytPar(R_li) "0.0" -set ::tmpactualGlobalAnalytPar(SD,typestr) "LogNorm" -set ::tmpactualGlobalAnalytPar(FF,l6,common) "P6" -set ::tmpactualGlobalAnalytPar(FF,l7,label) {eta_sh =} -set ::tmpactualGlobalAnalytPar(sumR_RG) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s7,var) "0.0" +set ::tmpactualGlobalAnalytPar(sumR_RG) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l7,label) {eta_sh =} +set ::tmpactualGlobalAnalytPar(FF,l6,common) "P6" set ::tmpactualGlobalAnalytPar(SD,a2,max) "1e+200" set ::tmpactualGlobalAnalytPar(plottype) "-1" -set ::tmpactualGlobalAnalytPar(SQ,s1,limits) "0" set ::tmpactualGlobalAnalytPar(FF,l6,active) "0" +set ::tmpactualGlobalAnalytPar(SQ,s1,limits) "0" set ::tmpactualGlobalAnalytPar(SD,a8,min) "-1e+200" -set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(sumR_lc) "0.0" set ::tmpactualGlobalAnalytPar(SD,a3,limits) "0" +set ::tmpactualGlobalAnalytPar(sumR_lc) "0.0" +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l1,distr) "0" set ::tmpactualGlobalAnalytPar(SQ,s2,max) "1e+200" -set ::tmpactualGlobalAnalytPar(FF,l1,distr) "1" -set ::tmpactualGlobalAnalytPar(FF,l5,min) "-1e+200" set ::tmpactualGlobalAnalytPar(FF,l2,factor) "1" -set ::tmpactualGlobalAnalytPar(FF,l8,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l5,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s3,label) "" -set ::tmpactualGlobalAnalytPar(sumR_li) "0.0" -set ::tmpactualGlobalAnalytPar(SQ,s8,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(FF,l8,limits) "0" set ::tmpactualGlobalAnalytPar(SD,a2,err) "0.0" -set ::tmpactualGlobalAnalytPar(FF,l7,max) "1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s8,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(sumR_li) "0.0" set ::tmpactualGlobalAnalytPar(FF,l4,common) "P4" -set ::tmpactualGlobalAnalytPar(FF,l6,label) {eta_c =} +set ::tmpactualGlobalAnalytPar(FF,l7,max) "1e+200" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l4,active) "0" -set ::tmpactualGlobalAnalytPar(SQ,s2,err) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l6,label) {eta_c =} +set ::tmpactualGlobalAnalytPar(FF,l4,active) "1" set ::tmpactualGlobalAnalytPar(SD,param_count_old) "10" +set ::tmpactualGlobalAnalytPar(SQ,s2,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a1,limits) "0" -set ::tmpactualGlobalAnalytPar(SD,a4,var) "10.0" +set ::tmpactualGlobalAnalytPar(SD,a4,var) "5" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l7,err) "0.0" set ::tmpactualGlobalAnalytPar(FF,l6,limits) "0" +set ::tmpactualGlobalAnalytPar(FF,l7,err) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s2,label) "" set ::tmpactualGlobalAnalytPar(FF,l1,var) "10.0" set ::tmpactualGlobalAnalytPar(FF,l2,common) "P2" set ::tmpactualGlobalAnalytPar(SQ,s4,var) "0.0" set ::tmpactualGlobalAnalytPar(FF,l5,label) {sigma =} -set ::tmpactualGlobalAnalytPar(FF,l2,active) "0" set ::tmpactualGlobalAnalytPar(fitSDFF) "yes" -set ::tmpactualGlobalAnalytPar(R_VP) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l2,active) "0" set ::tmpactualGlobalAnalytPar(FF,param_count_old) "8" +set ::tmpactualGlobalAnalytPar(R_VP) "0.0" set ::tmpactualGlobalAnalytPar(SD,a5,min) "-1e+200" -set ::tmpactualGlobalAnalytPar(FF,l9,var) "0.0" -set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(alambda) "-1" -set ::tmpactualGlobalAnalytPar(max_SD) "7" +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l9,var) "0.0" set ::tmpactualGlobalAnalytPar(common_names) {NONE NEW P1 P2 P3 P4 P5 P6 P7 P8} +set ::tmpactualGlobalAnalytPar(max_SD) "8" set ::tmpactualGlobalAnalytPar(SD,a7,max) "1e+200" -set ::tmpactualGlobalAnalytPar(SQ,s10,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,l4,limits) "0" -set ::tmpactualGlobalAnalytPar(FF,l2,min) "-1e+200" set ::tmpactualGlobalAnalytPar(SQ,s8,factor) "1" +set ::tmpactualGlobalAnalytPar(FF,l2,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(FF,l4,limits) "0" +set ::tmpactualGlobalAnalytPar(SQ,s10,distr) "0" set ::tmpactualGlobalAnalytPar(SD,a9,distr) "0" -set ::tmpactualGlobalAnalytPar(FF,l10,factor) "1" -set ::tmpactualGlobalAnalytPar(SQ,s1,label) "" set ::tmpactualGlobalAnalytPar(SQ,s5,min) "-1e+200" +set ::tmpactualGlobalAnalytPar(SQ,s1,label) "" +set ::tmpactualGlobalAnalytPar(FF,l10,factor) "1" set ::tmpactualGlobalAnalytPar(SQ,param_count) "10" set ::tmpactualGlobalAnalytPar(FF,l4,max) "1e+200" set ::tmpactualGlobalAnalytPar() "0.0" -set ::tmpactualGlobalAnalytPar(FF,l4,label) {t =} -set ::tmpactualGlobalAnalytPar(sumR_VP) "0.0" set ::tmpactualGlobalAnalytPar(SQ,s7,max) "1e+200" +set ::tmpactualGlobalAnalytPar(sumR_VP) "0.0" +set ::tmpactualGlobalAnalytPar(FF,l4,label) {t =} set ::tmpactualGlobalAnalytPar(substrSDFF) "no" set ::tmpactualGlobalAnalytPar(SD,a7,err) "0.0" set ::tmpactualGlobalAnalytPar(FF,l10,label) "" set ::tmpactualGlobalAnalytPar(SD,a1,var) "1.0" -set ::tmpactualGlobalAnalytPar(FF,l2,limits) "0" -set ::tmpactualGlobalAnalytPar() "0.0" set ::tmpactualGlobalAnalytPar(SQ,s6,factor) "1" +set ::tmpactualGlobalAnalytPar() "0.0" +set ::tmpactualGlobalAnalytPar(FF,l2,limits) "0" set ::tmpactualGlobalAnalytPar(FF,l4,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a8,distr) "0" -set ::tmpactualGlobalAnalytPar(SD,a10,distr) "0" -set ::tmpactualGlobalAnalytPar(SQ,s7,err) "0.0" set ::tmpactualGlobalAnalytPar(SD,a8,factor) "1" +set ::tmpactualGlobalAnalytPar(SQ,s7,err) "0.0" +set ::tmpactualGlobalAnalytPar(SD,a10,distr) "0" set ::AnalytPar(R_lc) "0.0507835" set ::AnalytPar(wR) "1.75904e+009" set ::AnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} @@ -1410,7 +2104,7 @@ set ::AnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 set ::AnalytPar(sumfp) "0" set ::AnalytPar() "86597.1" set ::AnalytPar(SD,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::AnalytPar(SD,param_count) "10" +set ::AnalytPar(SD,param_count) "0" set ::AnalytPar(resolution) "no" set ::AnalytPar() "324349" set ::AnalytPar(fp) "0" @@ -1435,7 +2129,7 @@ set ::AnalytPar(R) "1.07532e+009" set ::AnalytPar(error) "0" set ::AnalytPar(sumR_li) "17755.2" set ::AnalytPar(SQ,typestr) "None" -set ::AnalytPar(FF,typestr) "302" +set ::AnalytPar(FF,typestr) "314" set ::AnalytPar(reducedchisq) "3.09424e+018" set ::AnalytPar() "6.80386e-066" set ::AnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} @@ -1533,8 +2227,8 @@ set ::AnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+20 set ::AnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} set ::AnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} set ::AnalytPar(fitSDFF) "yes" -set ::AnalytPar(SQ,param_count_old) "10" set ::AnalytPar(FF,param_count_old) "8" +set ::AnalytPar(SQ,param_count_old) "10" set ::AnalytPar(R_VP) "0.00733088" set ::AnalytPar(actual_SD) "1" set ::AnalytPar() "18.2678" @@ -1547,9 +2241,9 @@ set ::AnalytPar(max_SD) "1" set ::AnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::AnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::AnalytPar(mom_w) ".obW.tab.analytmoments" -set ::AnalytPar(SQ,param_count) "10" +set ::AnalytPar(SQ,param_count) "0" set ::AnalytPar(SQ,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::AnalytPar(FF,param_count) "8" +set ::AnalytPar(FF,param_count) "0" set ::AnalytPar(FF,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::AnalytPar() "324349" set ::AnalytPar(w_AnalytPar) "" @@ -1570,16 +2264,16 @@ set ::AnalytPar(R_Ac) "0.516708" set ::AnalytPar(old_actual_SD) "1" set ::tmpAnalytPar(R_lc) "0.0" set ::tmpAnalytPar(wR) "3.45943e+009" -set ::tmpAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar(SQ,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpAnalytPar(FF,limits) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar(sumfp) "0" -set ::tmpAnalytPar(resolution) "no" -set ::tmpAnalytPar(SD,param_count) "10" -set ::tmpAnalytPar(SD,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar(SD,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpAnalytPar(SD,param_count) "0" +set ::tmpAnalytPar(resolution) "no" set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar(calcSDFF) "yes" set ::tmpAnalytPar(SD,typestr) "Delta" +set ::tmpAnalytPar(calcSDFF) "yes" set ::tmpAnalytPar(fp) "0" set ::tmpAnalytPar(alpha) "" set ::tmpAnalytPar(R_li) "0.0" @@ -1600,7 +2294,7 @@ set ::tmpAnalytPar(R) "2.00392e+009" set ::tmpAnalytPar(error) "0" set ::tmpAnalytPar(sumR_li) "0.0" set ::tmpAnalytPar(SQ,typestr) "None" -set ::tmpAnalytPar(FF,typestr) "302" +set ::tmpAnalytPar(FF,typestr) "314" set ::tmpAnalytPar(reducedchisq) "1.19676e+019" set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar(FF,distr) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} @@ -1676,13 +2370,13 @@ sumR_VP;0.0000e+000;sumVP;0.0000e+000 sumR_RG;0.0000e+000;sumRG;0.0000e+000 sumfp(Sph.);0.0000e+000;;} set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar(chisq) "1.20873e+021" -set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar(file) "unknown.par" set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar(file) "unknown.par" +set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar(chisq) "1.20873e+021" set ::tmpAnalytPar(varianceOFfit) "1.19676e+019" set ::tmpAnalytPar(par_descr) {parameters of_analytical_size distrib.} -set ::tmpAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} set ::tmpAnalytPar(par_text_display) {scattering contribution = 1 approximation type = monodisperse approx. calculate = yes substract = no fit = yes Delta triax ellip shell 3t None @@ -1694,42 +2388,42 @@ set ::tmpAnalytPar(par_text_display) {scattering contribution = 1 approxi eta_c = 1 eta_sh = 0.5 eta_sol = 0 } -set ::tmpAnalytPar(SQ,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} -set ::tmpAnalytPar(fitSDFF) "yes" -set ::tmpAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpAnalytPar(FF,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} set ::tmpAnalytPar(SQ,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} -set ::tmpAnalytPar(SQ,param_count_old) "10" -set ::tmpAnalytPar(FF,param_count_old) "8" +set ::tmpAnalytPar(FF,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} +set ::tmpAnalytPar(fitSDFF) "yes" set ::tmpAnalytPar(R_VP) "0.0" +set ::tmpAnalytPar(FF,param_count_old) "8" +set ::tmpAnalytPar(SQ,param_count_old) "10" set ::tmpAnalytPar(actual_SD) "1" -set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar() "0" +set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar(alambda) "-1" +set ::tmpAnalytPar() "0" set ::tmpAnalytPar(fit) "no" -set ::tmpAnalytPar(common_names) "" -set ::tmpAnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar(max_SD) "1" +set ::tmpAnalytPar(SQ,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpAnalytPar(FF,active) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} +set ::tmpAnalytPar(common_names) "" set ::tmpAnalytPar(mom_w) ".obW.tab.analytmoments" -set ::tmpAnalytPar(FF,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpAnalytPar(FF,param_count) "8" +set ::tmpAnalytPar(SQ,param_count) "0" set ::tmpAnalytPar(SQ,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} -set ::tmpAnalytPar(SQ,param_count) "10" -set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar(w_AnalytPar) "" +set ::tmpAnalytPar(FF,param_count) "0" +set ::tmpAnalytPar(FF,err) {{0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar(w_AnalytPar) "" +set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar() "0.0" -set ::tmpAnalytPar(FF,l) {{10 20 30 5 0.3 1 0.5 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar(sumR_VP) "0.0" +set ::tmpAnalytPar(FF,l) {{10 20 30 5 0.3 1 0.5 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar(geometrical/datafile) "yes" set ::tmpAnalytPar(substrSDFF) "no" -set ::tmpAnalytPar(w) "" set ::tmpAnalytPar(SD,min) {{-1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200 -1e+200}} +set ::tmpAnalytPar(w) "" set ::tmpAnalytPar(SD,max) {{1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200 1e+200}} set ::tmpAnalytPar(R_RG) "0.0" -set ::tmpAnalytPar(SQ,s) {{100 0.2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar() "0.0" +set ::tmpAnalytPar(SQ,s) {{100 0.2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0}} set ::tmpAnalytPar() "0.0" set ::tmpAnalytPar(R_Ac) "0.0" set ::tmpAnalytPar(old_actual_SD) "1" @@ -1744,43 +2438,43 @@ set ::actualAnalytPar(SD,a2,min) "-1e+200" set ::actualAnalytPar(FF,l6,var) "1" set ::actualAnalytPar(SQ,s9,var) "0" set ::actualAnalytPar(SD,a4,max) "1e+200" -set ::actualAnalytPar(SD,a7,distr) "0" set ::actualAnalytPar(SQ,s2,min) "-1e+200" +set ::actualAnalytPar(SD,a7,distr) "0" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l1,max) "1e+200" -set ::actualAnalytPar(SQ,s6,active) "0" set ::actualAnalytPar(SQ,s4,max) "1e+200" -set ::actualAnalytPar(FF,l2,label) {b =} +set ::actualAnalytPar(SQ,s6,active) "0" set ::actualAnalytPar(SD,a10,var) "0" -set ::actualAnalytPar(SQ,typestr) "None" +set ::actualAnalytPar(FF,l2,label) {b =} set ::actualAnalytPar(FF,l7,min) "-1e+200" +set ::actualAnalytPar(SQ,typestr) "None" set ::actualAnalytPar(SD,a8,active) "0" set ::actualAnalytPar(SD,a4,err) "0" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(SQ,s8,limits) "0" set ::actualAnalytPar(FF,l1,err) "0" -set ::actualAnalytPar(SD,a6,distr) "0" set ::actualAnalytPar(SQ,s4,err) "0" +set ::actualAnalytPar(SD,a6,distr) "0" set ::actualAnalytPar(SD,a10,active) "0" -set ::actualAnalytPar(SQ,s4,active) "0" set ::actualAnalytPar(SD,a6,var) "0" +set ::actualAnalytPar(SQ,s4,active) "0" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l1,label) {a =} set ::actualAnalytPar(SD,a6,active) "0" set ::actualAnalytPar(FF,l3,var) "30" -set ::actualAnalytPar(SQ,s9,distr) "0" set ::actualAnalytPar(SQ,s6,var) "0" -set ::actualAnalytPar(SQ,s6,limits) "0" +set ::actualAnalytPar(SQ,s9,distr) "0" set ::actualAnalytPar(SD,a1,max) "1e+200" +set ::actualAnalytPar(SQ,s6,limits) "0" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(SD,a8,limits) "0" -set ::actualAnalytPar(SD,a5,distr) "0" set ::actualAnalytPar(SD,a7,min) "-1e+200" +set ::actualAnalytPar(SD,a5,distr) "0" set ::actualAnalytPar(SQ,s2,active) "0" set ::actualAnalytPar(SQ,s1,max) "1e+200" set ::actualAnalytPar(SD,a9,max) "1e+200" -set ::actualAnalytPar(FF,l4,min) "-1e+200" set ::actualAnalytPar(SD,a4,active) "0" +set ::actualAnalytPar(FF,l4,min) "-1e+200" set ::actualAnalytPar(SQ,s7,min) "-1e+200" set ::actualAnalytPar() "0.0" set ::actualAnalytPar(w_AnalytPar) "" @@ -1885,7 +2579,7 @@ set ::actualAnalytPar(FF,l3,min) "-1e+200" set ::actualAnalytPar(SQ,s6,min) "-1e+200" set ::actualAnalytPar(error) "0" set ::actualAnalytPar(SQ,s9,limits) "0" -set ::actualAnalytPar(FF,typestr) "302" +set ::actualAnalytPar(FF,typestr) "314" set ::actualAnalytPar(FF,l5,max) "1e+200" set ::actualAnalytPar(FF,l5,distr) "0" set ::actualAnalytPar(SQ,s8,max) "1e+200" @@ -1929,87 +2623,87 @@ set ::actualAnalytPar(SD,a3,active) "0" set ::actualAnalytPar(FF,l8,label) {eta_sol =} set ::actualAnalytPar(SD,a1,label) {N =} set ::actualAnalytPar(R_RG) "0.0" -set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l2,err) "0" -set ::actualAnalytPar(SQ,s10,min) "-1e+200" -set ::actualAnalytPar(SQ,s3,limits) "0" +set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l8,active) "0" +set ::actualAnalytPar(SQ,s3,limits) "0" +set ::actualAnalytPar(SQ,s10,min) "-1e+200" set ::actualAnalytPar(SQ,s5,err) "0" set ::actualAnalytPar(SD,a5,limits) "0" -set ::actualAnalytPar(R_lc) "0.0" -set ::actualAnalytPar(FF,l2,distr) "0" set ::actualAnalytPar(SD,a7,var) "0" +set ::actualAnalytPar(FF,l2,distr) "0" +set ::actualAnalytPar(R_lc) "0.0" set ::actualAnalytPar(SQ,s4,label) "" set ::actualAnalytPar() "0.0" -set ::actualAnalytPar(FF,l4,var) "5" set ::actualAnalytPar(SD,a1,active) "0" -set ::actualAnalytPar(SD,typestr) "Delta" +set ::actualAnalytPar(FF,l4,var) "5" set ::actualAnalytPar(R_li) "0.0" -set ::actualAnalytPar(FF,l7,label) {eta_sh =} -set ::actualAnalytPar(SQ,s7,var) "0" +set ::actualAnalytPar(SD,typestr) "Delta" set ::actualAnalytPar(sumR_RG) "0.0" +set ::actualAnalytPar(SQ,s7,var) "0" +set ::actualAnalytPar(FF,l7,label) {eta_sh =} set ::actualAnalytPar(SD,a2,max) "1e+200" set ::actualAnalytPar(plottype) "-1" -set ::actualAnalytPar(SQ,s1,limits) "0" set ::actualAnalytPar(FF,l6,active) "0" +set ::actualAnalytPar(SQ,s1,limits) "0" set ::actualAnalytPar(SD,a8,min) "-1e+200" -set ::actualAnalytPar(sumR_lc) "0.0" -set ::actualAnalytPar() "0.0" set ::actualAnalytPar(SD,a3,limits) "0" -set ::actualAnalytPar(SQ,s2,max) "1e+200" +set ::actualAnalytPar() "0.0" +set ::actualAnalytPar(sumR_lc) "0.0" set ::actualAnalytPar(FF,l1,distr) "0" +set ::actualAnalytPar(SQ,s2,max) "1e+200" set ::actualAnalytPar(FF,l5,min) "-1e+200" -set ::actualAnalytPar(SQ,s3,label) "" set ::actualAnalytPar(FF,l8,limits) "0" -set ::actualAnalytPar(SQ,s8,min) "-1e+200" -set ::actualAnalytPar(sumR_li) "0.0" +set ::actualAnalytPar(SQ,s3,label) "" set ::actualAnalytPar(SD,a2,err) "0" +set ::actualAnalytPar(sumR_li) "0.0" +set ::actualAnalytPar(SQ,s8,min) "-1e+200" set ::actualAnalytPar(FF,l7,max) "1e+200" -set ::actualAnalytPar(FF,l6,label) {eta_c =} set ::actualAnalytPar() "0.0" +set ::actualAnalytPar(FF,l6,label) {eta_c =} set ::actualAnalytPar(FF,l4,active) "0" -set ::actualAnalytPar(SQ,s2,err) "0" set ::actualAnalytPar(SD,param_count_old) "10" +set ::actualAnalytPar(SQ,s2,err) "0" set ::actualAnalytPar(SD,a1,limits) "0" set ::actualAnalytPar(SD,a4,var) "10" set ::actualAnalytPar() "0.0" -set ::actualAnalytPar(FF,l6,limits) "0" set ::actualAnalytPar(FF,l7,err) "0" +set ::actualAnalytPar(FF,l6,limits) "0" set ::actualAnalytPar(SQ,s2,label) "" set ::actualAnalytPar(FF,l1,var) "10" set ::actualAnalytPar(SQ,s4,var) "0" set ::actualAnalytPar(FF,l5,label) {sigma =} -set ::actualAnalytPar(fitSDFF) "yes" set ::actualAnalytPar(FF,l2,active) "0" -set ::actualAnalytPar(R_VP) "0.0" +set ::actualAnalytPar(fitSDFF) "yes" set ::actualAnalytPar(FF,param_count_old) "8" +set ::actualAnalytPar(R_VP) "0.0" set ::actualAnalytPar(SD,a5,min) "-1e+200" -set ::actualAnalytPar(alambda) "-1" set ::actualAnalytPar() "0" -set ::actualAnalytPar(common_names) "" +set ::actualAnalytPar(alambda) "-1" set ::actualAnalytPar(max_SD) "1" +set ::actualAnalytPar(common_names) "" set ::actualAnalytPar(SD,a7,max) "1e+200" -set ::actualAnalytPar(SQ,s10,distr) "0" -set ::actualAnalytPar(FF,l2,min) "-1e+200" set ::actualAnalytPar(FF,l4,limits) "0" +set ::actualAnalytPar(FF,l2,min) "-1e+200" +set ::actualAnalytPar(SQ,s10,distr) "0" set ::actualAnalytPar(SD,a9,distr) "0" -set ::actualAnalytPar(SQ,s1,label) "" set ::actualAnalytPar(SQ,s5,min) "-1e+200" +set ::actualAnalytPar(SQ,s1,label) "" set ::actualAnalytPar(SQ,param_count) "10" set ::actualAnalytPar(FF,l4,max) "1e+200" set ::actualAnalytPar() "0.0" -set ::actualAnalytPar(FF,l4,label) {t =} -set ::actualAnalytPar(SQ,s7,max) "1e+200" set ::actualAnalytPar(sumR_VP) "0.0" +set ::actualAnalytPar(SQ,s7,max) "1e+200" +set ::actualAnalytPar(FF,l4,label) {t =} set ::actualAnalytPar(substrSDFF) "no" set ::actualAnalytPar(SD,a7,err) "0" set ::actualAnalytPar(SD,a1,var) "1" -set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l2,limits) "0" +set ::actualAnalytPar() "0.0" set ::actualAnalytPar(FF,l4,err) "0" set ::actualAnalytPar(SD,a8,distr) "0" -set ::actualAnalytPar(SD,a10,distr) "0" set ::actualAnalytPar(SQ,s7,err) "0" +set ::actualAnalytPar(SD,a10,distr) "0" set ::tmpactualAnalytPar(SQ,s1,var) "100" set ::tmpactualAnalytPar(SD,a9,var) "0" set ::tmpactualAnalytPar(SQ,s8,active) "0" @@ -2022,41 +2716,41 @@ set ::tmpactualAnalytPar(SD,a2,min) "-1e+200" set ::tmpactualAnalytPar(FF,l6,var) "1" set ::tmpactualAnalytPar(SQ,s9,var) "0" set ::tmpactualAnalytPar(SD,a4,max) "1e+200" -set ::tmpactualAnalytPar(SD,a7,distr) "0" set ::tmpactualAnalytPar(SQ,s2,min) "-1e+200" +set ::tmpactualAnalytPar(SD,a7,distr) "0" set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(FF,l1,max) "1e+200" -set ::tmpactualAnalytPar(SQ,s4,max) "1e+200" set ::tmpactualAnalytPar(SQ,s6,active) "0" -set ::tmpactualAnalytPar(FF,l2,label) {b =} +set ::tmpactualAnalytPar(SQ,s4,max) "1e+200" set ::tmpactualAnalytPar(SD,a10,var) "0" -set ::tmpactualAnalytPar(FF,l7,min) "-1e+200" +set ::tmpactualAnalytPar(FF,l2,label) {b =} set ::tmpactualAnalytPar(SQ,typestr) "None" +set ::tmpactualAnalytPar(FF,l7,min) "-1e+200" set ::tmpactualAnalytPar(SD,a8,active) "0" set ::tmpactualAnalytPar(SD,a4,err) "0" -set ::tmpactualAnalytPar(FF,l9,max) "1e+200" set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(FF,l9,max) "1e+200" set ::tmpactualAnalytPar(SQ,s8,limits) "0" set ::tmpactualAnalytPar(FF,l1,err) "0" set ::tmpactualAnalytPar(FF,l10,limits) "0" -set ::tmpactualAnalytPar(SD,a6,distr) "0" set ::tmpactualAnalytPar(SQ,s4,err) "0" +set ::tmpactualAnalytPar(SD,a6,distr) "0" set ::tmpactualAnalytPar(SD,a10,active) "0" -set ::tmpactualAnalytPar(SD,a6,var) "0" set ::tmpactualAnalytPar(SQ,s4,active) "0" +set ::tmpactualAnalytPar(SD,a6,var) "0" set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(FF,l1,label) {a =} -set ::tmpactualAnalytPar(SD,a6,active) "0" set ::tmpactualAnalytPar(FF,l9,err) "0.0" +set ::tmpactualAnalytPar(SD,a6,active) "0" set ::tmpactualAnalytPar(FF,l3,var) "30" -set ::tmpactualAnalytPar(SQ,s9,distr) "0" set ::tmpactualAnalytPar(SQ,s6,var) "0" -set ::tmpactualAnalytPar(SD,a1,max) "1e+200" +set ::tmpactualAnalytPar(SQ,s9,distr) "0" set ::tmpactualAnalytPar(SQ,s6,limits) "0" +set ::tmpactualAnalytPar(SD,a1,max) "1e+200" set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(SD,a8,limits) "0" -set ::tmpactualAnalytPar(SD,a5,distr) "0" set ::tmpactualAnalytPar(SD,a7,min) "-1e+200" +set ::tmpactualAnalytPar(SD,a5,distr) "0" set ::tmpactualAnalytPar(SQ,s2,active) "0" set ::tmpactualAnalytPar(SQ,s1,max) "1e+200" set ::tmpactualAnalytPar(SD,a9,max) "1e+200" @@ -2136,7 +2830,7 @@ set ::tmpactualAnalytPar(FF,l1,active) "0" set ::tmpactualAnalytPar(SD,a6,label) "" set ::tmpactualAnalytPar(SQ,s3,max) "1e+200" set ::tmpactualAnalytPar(SQ,s4,distr) "0" -set ::tmpactualAnalytPar(FF,param_count) "8" +set ::tmpactualAnalytPar(FF,param_count) "10" set ::tmpactualAnalytPar(FF,l6,min) "-1e+200" set ::tmpactualAnalytPar(FF,l10,err) "0.0" set ::tmpactualAnalytPar(SQ,s9,min) "-1e+200" @@ -2173,7 +2867,7 @@ set ::tmpactualAnalytPar(FF,l3,min) "-1e+200" set ::tmpactualAnalytPar(SQ,s6,min) "-1e+200" set ::tmpactualAnalytPar(error) "0" set ::tmpactualAnalytPar(SQ,s9,limits) "0" -set ::tmpactualAnalytPar(FF,typestr) "302" +set ::tmpactualAnalytPar(FF,typestr) "314" set ::tmpactualAnalytPar(FF,l5,max) "1e+200" set ::tmpactualAnalytPar(FF,l5,distr) "0" set ::tmpactualAnalytPar(SQ,s8,max) "1e+200" @@ -2200,120 +2894,120 @@ set ::tmpactualAnalytPar(FF,l10,distr) "0" set ::tmpactualAnalytPar(SD,a3,min) "-1e+200" set ::tmpactualAnalytPar(actual_SD) "1" set ::tmpactualAnalytPar(FF,l7,var) "0.5" +set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(FF,l9,label) "" set ::tmpactualAnalytPar(SD,a5,active) "0" -set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(SD,a2,label) "" set ::tmpactualAnalytPar(SD,a5,max) "1e+200" -set ::tmpactualAnalytPar(SQ,s5,limits) "0" set ::tmpactualAnalytPar(SQ,s3,min) "-1e+200" +set ::tmpactualAnalytPar(SQ,s5,limits) "0" set ::tmpactualAnalytPar(FF,l2,max) "1e+200" -set ::tmpactualAnalytPar(FF,l3,distr) "0" set ::tmpactualAnalytPar(SD,a7,limits) "0" -set ::tmpactualAnalytPar(SQ,s5,max) "1e+200" +set ::tmpactualAnalytPar(FF,l3,distr) "0" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(SQ,s1,active) "0" -set ::tmpactualAnalytPar(SQ,s5,label) "" +set ::tmpactualAnalytPar(SQ,s5,max) "1e+200" set ::tmpactualAnalytPar(FF,l8,min) "-1e+200" +set ::tmpactualAnalytPar(SQ,s5,label) "" +set ::tmpactualAnalytPar(SQ,s1,active) "0" set ::tmpactualAnalytPar(SD,a5,err) "0" set ::tmpactualAnalytPar(SD,a3,active) "0" set ::tmpactualAnalytPar(FF,l8,label) {eta_sol =} set ::tmpactualAnalytPar(SD,a1,label) {N =} set ::tmpactualAnalytPar(R_RG) "0.0" -set ::tmpactualAnalytPar(FF,l2,err) "0" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(FF,l8,active) "0" -set ::tmpactualAnalytPar(SQ,s3,limits) "0" +set ::tmpactualAnalytPar(FF,l2,err) "0" set ::tmpactualAnalytPar(SQ,s10,min) "-1e+200" +set ::tmpactualAnalytPar(SQ,s3,limits) "0" +set ::tmpactualAnalytPar(FF,l8,active) "0" set ::tmpactualAnalytPar(SQ,s5,err) "0" set ::tmpactualAnalytPar(SD,a5,limits) "0" -set ::tmpactualAnalytPar(SD,a7,var) "0" -set ::tmpactualAnalytPar(FF,l2,distr) "0" set ::tmpactualAnalytPar(R_lc) "0.0" +set ::tmpactualAnalytPar(FF,l2,distr) "0" +set ::tmpactualAnalytPar(SD,a7,var) "0" set ::tmpactualAnalytPar(SQ,s4,label) "" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(SD,a1,active) "0" set ::tmpactualAnalytPar(FF,l4,var) "5" -set ::tmpactualAnalytPar(R_li) "0.0" +set ::tmpactualAnalytPar(SD,a1,active) "0" set ::tmpactualAnalytPar(SD,typestr) "Delta" -set ::tmpactualAnalytPar(FF,l7,label) {eta_sh =} -set ::tmpactualAnalytPar(sumR_RG) "0.0" +set ::tmpactualAnalytPar(R_li) "0.0" set ::tmpactualAnalytPar(SQ,s7,var) "0" +set ::tmpactualAnalytPar(sumR_RG) "0.0" +set ::tmpactualAnalytPar(FF,l7,label) {eta_sh =} set ::tmpactualAnalytPar(SD,a2,max) "1e+200" set ::tmpactualAnalytPar(plottype) "-1" -set ::tmpactualAnalytPar(FF,l6,active) "0" set ::tmpactualAnalytPar(SQ,s1,limits) "0" +set ::tmpactualAnalytPar(FF,l6,active) "0" set ::tmpactualAnalytPar(SD,a8,min) "-1e+200" -set ::tmpactualAnalytPar(SD,a3,limits) "0" -set ::tmpactualAnalytPar() "0.0" set ::tmpactualAnalytPar(sumR_lc) "0.0" -set ::tmpactualAnalytPar(FF,l1,distr) "0" +set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(SD,a3,limits) "0" set ::tmpactualAnalytPar(SQ,s2,max) "1e+200" +set ::tmpactualAnalytPar(FF,l1,distr) "0" set ::tmpactualAnalytPar(FF,l5,min) "-1e+200" -set ::tmpactualAnalytPar(FF,l8,limits) "0" set ::tmpactualAnalytPar(SQ,s3,label) "" -set ::tmpactualAnalytPar(SD,a2,err) "0" -set ::tmpactualAnalytPar(sumR_li) "0.0" +set ::tmpactualAnalytPar(FF,l8,limits) "0" set ::tmpactualAnalytPar(SQ,s8,min) "-1e+200" +set ::tmpactualAnalytPar(sumR_li) "0.0" +set ::tmpactualAnalytPar(SD,a2,err) "0" set ::tmpactualAnalytPar(FF,l7,max) "1e+200" -set ::tmpactualAnalytPar(FF,l6,label) {eta_c =} set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(FF,l6,label) {eta_c =} set ::tmpactualAnalytPar(FF,l4,active) "0" -set ::tmpactualAnalytPar(SD,param_count_old) "10" set ::tmpactualAnalytPar(SQ,s2,err) "0" +set ::tmpactualAnalytPar(SD,param_count_old) "10" set ::tmpactualAnalytPar(SD,a1,limits) "0" set ::tmpactualAnalytPar(SD,a4,var) "10" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(FF,l7,err) "0" set ::tmpactualAnalytPar(FF,l6,limits) "0" +set ::tmpactualAnalytPar(FF,l7,err) "0" set ::tmpactualAnalytPar(SQ,s2,label) "" set ::tmpactualAnalytPar(FF,l1,var) "10" set ::tmpactualAnalytPar(SQ,s4,var) "0" set ::tmpactualAnalytPar(FF,l5,label) {sigma =} -set ::tmpactualAnalytPar(FF,l2,active) "0" set ::tmpactualAnalytPar(fitSDFF) "yes" -set ::tmpactualAnalytPar(FF,param_count_old) "8" +set ::tmpactualAnalytPar(FF,l2,active) "0" set ::tmpactualAnalytPar(R_VP) "0.0" +set ::tmpactualAnalytPar(FF,param_count_old) "8" set ::tmpactualAnalytPar(SD,a5,min) "-1e+200" -set ::tmpactualAnalytPar(FF,l9,var) "0.0" -set ::tmpactualAnalytPar() "0" set ::tmpactualAnalytPar(alambda) "-1" -set ::tmpactualAnalytPar(common_names) "" +set ::tmpactualAnalytPar() "0" +set ::tmpactualAnalytPar(FF,l9,var) "0.0" set ::tmpactualAnalytPar(max_SD) "1" +set ::tmpactualAnalytPar(common_names) "" set ::tmpactualAnalytPar(SD,a7,max) "1e+200" -set ::tmpactualAnalytPar(SQ,s10,distr) "0" -set ::tmpactualAnalytPar(FF,l4,limits) "0" set ::tmpactualAnalytPar(FF,l2,min) "-1e+200" +set ::tmpactualAnalytPar(FF,l4,limits) "0" +set ::tmpactualAnalytPar(SQ,s10,distr) "0" set ::tmpactualAnalytPar(SD,a9,distr) "0" -set ::tmpactualAnalytPar(SQ,s1,label) "" set ::tmpactualAnalytPar(SQ,s5,min) "-1e+200" +set ::tmpactualAnalytPar(SQ,s1,label) "" set ::tmpactualAnalytPar(SQ,param_count) "10" set ::tmpactualAnalytPar(FF,l4,max) "1e+200" set ::tmpactualAnalytPar() "0.0" -set ::tmpactualAnalytPar(sumR_VP) "0.0" -set ::tmpactualAnalytPar(FF,l4,label) {t =} set ::tmpactualAnalytPar(SQ,s7,max) "1e+200" +set ::tmpactualAnalytPar(FF,l4,label) {t =} +set ::tmpactualAnalytPar(sumR_VP) "0.0" set ::tmpactualAnalytPar(substrSDFF) "no" set ::tmpactualAnalytPar(SD,a7,err) "0" set ::tmpactualAnalytPar(FF,l10,label) "" set ::tmpactualAnalytPar(SD,a1,var) "1" -set ::tmpactualAnalytPar(FF,l2,limits) "0" set ::tmpactualAnalytPar() "0.0" +set ::tmpactualAnalytPar(FF,l2,limits) "0" set ::tmpactualAnalytPar(FF,l4,err) "0" set ::tmpactualAnalytPar(SD,a8,distr) "0" -set ::tmpactualAnalytPar(SD,a10,distr) "0" set ::tmpactualAnalytPar(SQ,s7,err) "0" -set ::GlobalAnalytPar(FF,typestr) { ff_triax_ellip_shell_1 ff_triax_ellip_shell_1t ff_triax_ellip_shell_2 ff_triax_ellip_shell_2t ff_triax_ellip_shell_3 ff_triax_ellip_shell_3t ff_triax_ellip_shell_3t } -set ::GlobalAnalytPar(SD,typestr) { Delta Delta Delta Delta Delta Delta LogNorm } -set ::GlobalAnalytPar(SQ,typestr) { None None None None None None None } -set ::tmpGlobalAnalytPar(FF,typestr) { ff_triax_ellip_shell_1 ff_triax_ellip_shell_1t ff_triax_ellip_shell_2 ff_triax_ellip_shell_2t ff_triax_ellip_shell_3 ff_triax_ellip_shell_3t ff_triax_ellip_shell_3t } -set ::tmpGlobalAnalytPar(SD,typestr) { Delta Delta Delta Delta Delta Delta LogNorm } -set ::tmpGlobalAnalytPar(SQ,typestr) { None None None None None None None } -set ::actualGlobalAnalytPar(FF,typestr) { ff_triax_ellip_shell_3t } -set ::actualGlobalAnalytPar(SD,typestr) { LogNorm } +set ::tmpactualAnalytPar(SD,a10,distr) "0" +set ::GlobalAnalytPar(FF,typestr) { ff_triax_ellip_shell_1 ff_triax_ellip_shell_1t ff_triax_ellip_shell_2 ff_triax_ellip_shell_2t ff_triax_ellip_shell_3 ff_triax_ellip_shell_3t ff_triax_ellip_shell ff_triax_ellip_shell_t } +set ::GlobalAnalytPar(SD,typestr) { Delta Delta Delta Delta Delta Delta Delta Delta } +set ::GlobalAnalytPar(SQ,typestr) { None None None None None None None None } +set ::tmpGlobalAnalytPar(FF,typestr) { ff_triax_ellip_shell_1 ff_triax_ellip_shell_1t ff_triax_ellip_shell_2 ff_triax_ellip_shell_2t ff_triax_ellip_shell_3 ff_triax_ellip_shell_3t ff_triax_ellip_shell ff_triax_ellip_shell_t } +set ::tmpGlobalAnalytPar(SD,typestr) { Delta Delta Delta Delta Delta Delta Delta Delta } +set ::tmpGlobalAnalytPar(SQ,typestr) { None None None None None None None None } +set ::actualGlobalAnalytPar(FF,typestr) { ff_triax_ellip_shell } +set ::actualGlobalAnalytPar(SD,typestr) { Delta } set ::actualGlobalAnalytPar(SQ,typestr) { None } -set ::tmpactualGlobalAnalytPar(FF,typestr) { ff_triax_ellip_shell_3t } -set ::tmpactualGlobalAnalytPar(SD,typestr) { LogNorm } +set ::tmpactualGlobalAnalytPar(FF,typestr) { ff_triax_ellip_shell } +set ::tmpactualGlobalAnalytPar(SD,typestr) { Delta } set ::tmpactualGlobalAnalytPar(SQ,typestr) { None } set ::AnalytPar(FF,typestr) { ff_triax_ellip_shell_2t } set ::AnalytPar(SD,typestr) { Delta } @@ -2327,16 +3021,16 @@ set ::actualAnalytPar(SQ,typestr) { None } set ::tmpactualAnalytPar(FF,typestr) { ff_triax_ellip_shell_2t } set ::tmpactualAnalytPar(SD,typestr) { Delta } set ::tmpactualAnalytPar(SQ,typestr) { None } -set ::IQGraph(e,fill) "Black" +set ::IQGraph(e,fill) "" set ::IQGraph(e.resstipples) "" -set ::IQGraph(e,scale) "no" -set ::IQGraph(e,dash) "0" -set ::IQGraph(e,linewidth) "2" +set ::IQGraph(e,scale) "" +set ::IQGraph(e,dash) "" +set ::IQGraph(e,linewidth) "" set ::IQGraph(y,min) "" set ::IQGraph(l,hide) "yes" -set ::IQGraph(e,resoutline) "blue" -set ::IQGraph(e,xdata) {{0.01 0.0105869585454 0.0112083691242 0.011866253928 0.0125627538425 0.0133001354146 0.0140807982283 0.0149072827129 0.0157822784106 0.0167086327285 0.0176893602047 0.0187276523182 0.0198268878746 0.0209906440013 0.0222227077883 0.0235270886121 0.0249080311831 0.0263700293583 0.0279178407657 0.0295565022864 0.0312913464453 0.0331280187647 0.0350724961353 0.0371311062668 0.0393105482792 0.0416179145029 0.0440607135588 0.0466468947928 0.0493848741444 0.0522835615336 0.0553523898563 0.0586013456798 0.0620410017417 0.0656825513554 0.0695378448356 0.0736194280612 0.077940583302 0.0825153724423 0.0873586827406 0.0924862752756 0.0979148362361 0.103662031221 0.109746562727 0.116188231009 0.123007998516 0.130228058104 0.13787190526 0.145964414556 0.154531920601 0.163602303734 0.173205080757 0.183371500983 0.194134647931 0.205529546988 0.217593279381 0.230365102857 0.243886579425 0.258201710616 0.273357080664 0.289402008109 0.30638870628 0.324372453217 0.343411771548 0.363568618938 0.384908589711 0.407501128304 0.431419755256 0.456742306456 0.483551186439 0.511933636541 0.541982018806 0.573794116545 0.607473452546 0.643129625954 0.68087866893 0.720843424241 0.763153945017 0.807947917965 0.855371111435 0.90557784977 0.958731515515 1.01500508109 1.07458167169 1.13765516118 1.20443080304 1.27512589826 1.34997050251 1.42920817476 1.51309676989 1.6019092778 1.69593471176 1.79547904891 1.900866226 2.0124391935 2.13056103167 2.25561613208 2.38801144846 2.52817782108 2.67657137872 2.83367502304 3.0}} -set ::IQGraph(e,element) "1" +set ::IQGraph(e,resoutline) "" +set ::IQGraph(e,xdata) "" +set ::IQGraph(e,element) "0" set ::IQGraph(y,max) "" set ::IQGraph(x,linewidth) "2" set ::IQGraph(colorselection) {black red green blue cyan magenta yellow violet purple orange pink gray} @@ -2345,32 +3039,32 @@ set ::IQGraph(y,titlecolor) "black" set ::IQGraph(y,loose) "no" set ::IQGraph(fit,background) "#cccccc" set ::IQGraph(x,size) "12" -set ::IQGraph(e,dashcolor) "red" -set ::IQGraph(e,outlinewidth) "1" +set ::IQGraph(e,dashcolor) "" +set ::IQGraph(e,outlinewidth) "" set ::IQGraph(x,ticklength) "10" set ::IQGraph(l,posx) "10" -set ::IQGraph(e,errlinewidth) "1" +set ::IQGraph(e,errlinewidth) "" set ::IQGraph(l,posy) "10" -set ::IQGraph(e,linehide) "1" +set ::IQGraph(e,linehide) "" set ::IQGraph(graph,fg) "black" -set ::IQGraph(e,elementname) "graph1" +set ::IQGraph(e,elementname) "" set ::IQGraph(dashnames) {{-} {..} {--} {.-} {..-} {--.}} -set ::IQGraph(e,reshide) "no" +set ::IQGraph(e,reshide) "" set ::IQGraph(graph,relief) "flat" -set ::IQGraph(e,pixels) "4" +set ::IQGraph(e,pixels) "" set ::IQGraph(dashpattern) {{0} {2 2} {8 2 8 2} {2 2 8 2} {2 2 2 2 8 2} {8 2 8 2 2 2} } set ::IQGraph(x,tickcolor) "black" set ::IQGraph(x,logscale) "1" set ::IQGraph(e,resstipples) "hline1" set ::IQGraph(y,title) "I(Q)" set ::IQGraph(l,bg) "white" -set ::IQGraph(e,errtags) "{}" -set ::IQGraph(e,symbolhide) "no" +set ::IQGraph(e,errtags) "" +set ::IQGraph(e,symbolhide) "" set ::IQGraph(c,hide) "yes" set ::IQGraph(plot,borderwidth) "0" set ::IQGraph(y,rot) "0" -set ::IQGraph(e,smooth) "linear" -set ::IQGraph(e,offdashcolor) "White" +set ::IQGraph(e,smooth) "" +set ::IQGraph(e,offdashcolor) "" set ::IQGraph(g,dash) "0" set ::IQGraph(y,color) "Black" set ::IQGraph(x,subticks) "5" @@ -2380,16 +3074,16 @@ set ::IQGraph(l,pady) {0 0} set ::IQGraph(y,titlefont) {Helvetica 10} set ::IQGraph(x,loose) "no" set ::IQGraph(x,type) "log10(x)" -set ::IQGraph(c,x) "113" +set ::IQGraph(c,x) "243" set ::IQGraph(y,logscale) "1" +set ::IQGraph(c,y) "0" set ::IQGraph(e.errstipples) "" -set ::IQGraph(c,y) "6" set ::IQGraph(e,restags) "" set ::IQGraph(title) "unknown" set ::IQGraph(l,anchor) "n" set ::IQGraph(GraphName) "IQGraph" set ::IQGraph(symbolselection) {square circle diamond plus cross splus scross triangle} -set ::IQGraph(e,errorhide) "no" +set ::IQGraph(e,errorhide) "" set ::IQGraph(y,subticks) "5" set ::IQGraph(l,ipadx) {0 0} set ::IQGraph(c,color) "black" @@ -2404,41 +3098,41 @@ set ::IQGraph(margin,plotpady) {5 5} set ::IQGraph(fitrange) "no" set ::IQGraph(margin,right) "0" set ::IQGraph(x,min) "" -set ::IQGraph(e,errfill) "Black" +set ::IQGraph(e,errfill) "" set ::IQGraph(height) "512" -set ::IQGraph(e,erroutline) "blue" -set ::IQGraph(e,errdash) "0" +set ::IQGraph(e,erroutline) "" +set ::IQGraph(e,errdash) "" set ::IQGraph(y,ticklength) "10" set ::IQGraph(g,color) "black" set ::IQGraph(x,max) "" set ::IQGraph(g,linewidth) "1" set ::IQGraph(x,color) "Black" -set ::IQGraph(l,legendtext) "Fit" -set ::IQGraph(e,ydata) {{3.55652e+009 3.54734e+009 3.53709e+009 3.52564e+009 3.51285e+009 3.49859e+009 3.48267e+009 3.46494e+009 3.44518e+009 3.42318e+009 3.39872e+009 3.37154e+009 3.34136e+009 3.30791e+009 3.27086e+009 3.22989e+009 3.18466e+009 3.13481e+009 3.07998e+009 3.0198e+009 2.95392e+009 2.882e+009 2.80371e+009 2.71877e+009 2.62698e+009 2.52818e+009 2.42233e+009 2.30951e+009 2.18995e+009 2.06403e+009 1.93233e+009 1.79566e+009 1.65503e+009 1.5117e+009 1.36713e+009 1.22301e+009 1.08118e+009 9.43566e+008 8.12134e+008 6.8877e+008 5.75173e+008 4.72737e+008 3.82444e+008 3.0477e+008 2.39637e+008 1.86409e+008 1.43959e+008 1.10794e+008 8.52268e+007 6.55806e+007 5.03704e+007 3.84322e+007 2.89653e+007 2.14822e+007 1.56905e+007 1.1361e+007 8.23792e+006 6.02427e+006 4.43182e+006 3.24445e+006 2.34247e+006 1.67228e+006 1.195e+006 860547 619535 442520 316822 230478 170063 128649 102115 83519 70341.3 62408.3 55400 49709.7 45099.5 39849.2 35477.8 30563.4 26306.7 21952.8 18210.8 14761.2 11797.5 9352.88 7304.37 5663.62 4388.32 3397.53 2623.23 2110.71 1575.4 1283.97 1019.85 812.476 648.928 519.219 414.941 331.689 264.275}} +set ::IQGraph(l,legendtext) "" +set ::IQGraph(e,ydata) "" set ::IQGraph(y,mapped) "1" set ::IQGraph(margin,top) "0" set ::IQGraph(l,borderwidth) "2" set ::IQGraph(e,errstipples) "hline1" -set ::IQGraph(e,symbol) "none" +set ::IQGraph(e,symbol) "" set ::IQGraph(y,tickfont) {Helvetica 10} set ::IQGraph(font) {Helvetica 10} set ::IQGraph(graph,bg) "white" set ::IQGraph(margin,bottom) "0" -set ::IQGraph(e,outline) "Black" -set ::IQGraph(e,resfill) "Black" +set ::IQGraph(e,outline) "" +set ::IQGraph(e,resfill) "" set ::IQGraph(plot,relief) "flat" -set ::IQGraph(e,resdash) "0" +set ::IQGraph(e,resdash) "" set ::IQGraph(x,showticks) "yes" set ::IQGraph(x,mapped) "1" set ::IQGraph(y,factor) "1.0" set ::IQGraph(stipples) {bdiagonal1 bdiagonal2 checker2 checker3 cross1 cross2 cross3 crossdiag dot1 dot2 dot3 dot4 fdiagonal1 fdiagonal2 hline1 hline2 lbottom ltop rbottom rtop vline1 vline2} set ::IQGraph(graph,borderwidth) "0" -set ::IQGraph(e,resdata) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0}} +set ::IQGraph(e,resdata) "" set ::IQGraph(x,titlecolor) "black" set ::IQGraph(c,dash) "0" set ::IQGraph(y,size) "12" set ::IQGraph(x,rot) "0" -set ::IQGraph(e,error) {{-1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0 -1.0}} +set ::IQGraph(e,error) "" set ::IQGraph(x,factor) "1.0" set ::IQGraph(x,stepsize) "0" set ::IQGraph(plot,background) "gray90" @@ -2451,7 +3145,7 @@ set ::IQGraph(upper,x) "" set ::IQGraph(width) "768" set ::IQGraph(g,minor) "no" set ::IQGraph(upper,y) "" -set ::IQGraph(e,reslinewidth) "1" +set ::IQGraph(e,reslinewidth) "" set ::IQGraph(y,stepsize) "0" set ::IQGraph(y,showticks) "yes" set ::IQGraph(lower,x) "" @@ -2466,7 +3160,7 @@ set ::GlobalFitIQGraph(e,linewidth) {2 2 2 2 2 2 2 2} set ::GlobalFitIQGraph(y,min) "" set ::GlobalFitIQGraph(l,hide) "no" set ::GlobalFitIQGraph(e,resoutline) {blue blue blue blue blue blue blue blue} -set ::GlobalFitIQGraph(e,xdata) {{0.01 0.0100437693782 0.0100877303323 0.0101318837008 0.0101762303257 0.0102207710532 0.0102655067326 0.0103104382173 0.0103555663643 0.0104008920344 0.0104464160921 0.0104921394058 0.0105380628476 0.0105841872935 0.0106305136232 0.0106770427203 0.0107237754725 0.0107707127709 0.0108178555111 0.010865204592 0.0109127609169 0.010960525393 0.0110084989311 0.0110566824465 0.0111050768581 0.011153683089 0.0112025020664 0.0112515347214 0.0113007819893 0.0113502448094 0.0113999241252 0.0114498208843 0.0114999360384 0.0115502705434 0.0116008253594 0.0116516014507 0.0117025997858 0.0117538213374 0.0118052670826 0.0118569380026 0.011908835083 0.0119609593137 0.012013311689 0.0120658932073 0.0121187048716 0.0121717476893 0.0122250226722 0.0122785308363 0.0123322732023 0.0123862507954 0.012440464645 0.0124949157852 0.0125496052547 0.0126045340966 0.0126597033586 0.0127151140931 0.0127707673569 0.0128266642116 0.0128828057233 0.012939192963 0.012995827006 0.0130527089328 0.0131098398282 0.013167220782 0.0132248528887 0.0132827372475 0.0133408749626 0.0133992671428 0.013457914902 0.0135168193587 0.0135759816366 0.0136354028641 0.0136950841747 0.0137550267066 0.0138152316032 0.013875700013 0.0139364330892 0.0139974319903 0.0140586978798 0.0141202319263 0.0141820353035 0.0142441091902 0.0143064547705 0.0143690732335 0.0144319657736 0.0144951335905 0.0145585778889 0.0146222998792 0.0146863007766 0.0147505818019 0.0148151441813 0.0148799891462 0.0149451179335 0.0150105317855 0.0150762319498 0.0151422196797 0.0152084962337 0.0152750628761 0.0153419208766 0.0154090715103 0.0154765160583 0.0155442558068 0.0156122920479 0.0156806260795 0.0157492592049 0.0158181927332 0.0158874279793 0.0159569662637 0.0160268089129 0.016096957259 0.0161674126401 0.0162381764 0.0163092498884 0.0163806344611 0.0164523314797 0.0165243423116 0.0165966683305 0.0166693109158 0.0167422714533 0.0168155513344 0.0168891519571 0.0169630747251 0.0170373210485 0.0171118923434 0.0171867900322 0.0172620155435 0.0173375703123 0.0174134557795 0.0174896733928 0.0175662246058 0.0176431108787 0.017720333678 0.0177978944767 0.0178757947542 0.0179540359964 0.0180326196956 0.0181115473508 0.0181908204675 0.0182704405576 0.0183504091399 0.0184307277398 0.0185113978891 0.0185924211267 0.018673798998 0.0187555330551 0.0188376248571 0.0189200759699 0.019002887966 0.0190860624251 0.0191696009336 0.019253505085 0.0193377764796 0.0194224167249 0.0195074274353 0.0195928102323 0.0196785667445 0.0197646986075 0.0198512074644 0.0199380949652 0.0200253627672 0.0201130125349 0.0202010459402 0.0202894646623 0.0203782703876 0.02046746481 0.0205570496309 0.0206470265589 0.0207373973104 0.0208281636091 0.0209193271862 0.0210108897806 0.0211028531387 0.0211952190148 0.0212879891706 0.0213811653756 0.021474749407 0.02156874305 0.0216631480972 0.0217579663495 0.0218531996154 0.0219488497113 0.0220449184618 0.0221414076992 0.022238319264 0.0223356550048 0.022433416778 0.0225316064484 0.0226302258888 0.0227292769805 0.0228287616126 0.0229286816828 0.0230290390968 0.0231298357691 0.0232310736221 0.0233327545869 0.023434880603 0.0235374536183 0.0236404755893 0.0237439484811 0.0238478742673 0.0239522549302 0.0240570924607 0.0241623888586 0.0242681461323 0.024374366299 0.0244810513848 0.0245882034246 0.0246958244621 0.0248039165503 0.0249124817508 0.0250215221345 0.0251310397811 0.0252410367796 0.0253515152282 0.0254624772341 0.0255739249138 0.025685860393 0.0257982858069 0.0259112032998 0.0260246150256 0.0261385231474 0.026252929838 0.0263678372796 0.0264832476639 0.0265991631923 0.0267155860758 0.0268325185349 0.0269499628002 0.0270679211117 0.0271863957194 0.0273053888831 0.0274249028725 0.0275449399672 0.0276655024568 0.0277865926409 0.0279082128292 0.0280303653415 0.0281530525078 0.0282762766681 0.028400040173 0.028524345383 0.0286491946692 0.0287745904129 0.0289005350061 0.0290270308508 0.0291540803601 0.0292816859571 0.0294098500759 0.0295385751611 0.0296678636679 0.0297977180626 0.0299281408218 0.0300591344333 0.0301907013958 0.0303228442186 0.0304555654224 0.0305888675386 0.0307227531099 0.0308572246901 0.0309922848439 0.0311279361477 0.0312641811888 0.0314010225659 0.0315384628893 0.0316765047804 0.0318151508723 0.0319544038095 0.0320942662481 0.032234740856 0.0323758303125 0.0325175373087 0.0326598645477 0.0328028147441 0.0329463906247 0.033090594928 0.0332354304045 0.0333808998169 0.0335270059399 0.0336737515603 0.0338211394771 0.0339691725018 0.0341178534577 0.0342671851809 0.0344171705199 0.0345678123353 0.0347191135006 0.0348710769016 0.0350237054371 0.0351770020181 0.0353309695687 0.0354856110258 0.0356409293389 0.0357969274705 0.0359536083963 0.0361109751048 0.0362690305976 0.0364277778894 0.0365872200083 0.0367473599954 0.0369082009053 0.0370697458058 0.0372319977783 0.0373949599176 0.0375586353321 0.0377230271437 0.037888138488 0.0380539725144 0.038220532386 0.0383878212798 0.0385558423867 0.0387245989116 0.0388940940733 0.0390643311047 0.0392353132531 0.0394070437797 0.0395795259601 0.0397527630843 0.0399267584566 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6.30342328054 6.38655515951 6.47078341246 6.55612249878 6.64258706856 6.73019196508 6.81895222739 6.90888309289 6.99999999993}} set ::GlobalFitIQGraph(e,element) "8" set ::GlobalFitIQGraph(y,max) "" set ::GlobalFitIQGraph(x,linewidth) "2" @@ -2511,10 +3205,10 @@ set ::GlobalFitIQGraph(l,pady) {0 0} set ::GlobalFitIQGraph(y,titlefont) {Helvetica 10} set ::GlobalFitIQGraph(x,loose) "no" set ::GlobalFitIQGraph(x,type) "log10(x)" -set ::GlobalFitIQGraph(c,x) "56" +set ::GlobalFitIQGraph(c,x) "260" set ::GlobalFitIQGraph(y,logscale) "1" +set ::GlobalFitIQGraph(c,y) "51" set ::GlobalFitIQGraph(e.errstipples) "" -set ::GlobalFitIQGraph(c,y) "8" set ::GlobalFitIQGraph(e,restags) "" set ::GlobalFitIQGraph(title) "unknown" set ::GlobalFitIQGraph(l,anchor) "n" @@ -2545,7 +3239,7 @@ set ::GlobalFitIQGraph(x,max) "" set ::GlobalFitIQGraph(g,linewidth) "1" set ::GlobalFitIQGraph(x,color) "Black" set ::GlobalFitIQGraph(l,legendtext) {{Sim.: 1} {Sim.: 1t} {Sim.: 2} {Sim.: 2t} {Sim.: 3} {Sim.: 3t} 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504932 480766 456988 433642 410763 388390 366570 345358 324812 304984 285910 267604 250056 233237 217111 201652 186863 172790 159528 147214 136013 126087 117558 110483 104825 100445 97116.6 94552.7 92444 90503.4 88502.4 86293.3 83812.1 81064.2 78098.7 74979.9 71764 68489.1 65175.5 61836.1 58486.3 55149.4 51853.6 48623.7 45472.2 42398.5 39398.4 36481.7 33688.1 31092.6 28791.7 26874.6 25387.9 24311.6 23557.9 22995.9 22491.1 21942.9 21303.1 20570.2 19766.5 18914.9 18027.5 17109.3 16167.1 15213.7 14262.3 13318.3 12380.6 11455.3 10571.7 9783.91 9149.86 8697.24 8402.2 8198.21 8010.47 7790.39 7526.16 7227.53 6904.8 6561.4 6200.18 5828.28 5451.95 5071.73 4690.83 4330.44 4029.14 3817.1 3688.08 3600.94 3511.16 3398.57 3265.47 3117.78 2957.01 2785.8 2608.66 2426.6 2242.45 2074.23 1949.15 1875.42 1830 1782.46 1721 1648.46 1567 1477.72 1383.44 1284.91 1186.3 1104.88 1055.54 1028.51 1001.56 965.759 923.006 874.175 820.711 763.792 705.404 657.692 631.152 618.805 610.447 572.87 544.059 488.983 476.137 439.772 412.317 398.918 388.774 374.62 363.44 336.19 313.226 289.377 272.512 264.978 257.193 246.549 233.407 218.302 202.28 189.232 183.672 174.944 170.574 160.998 149.906 138.777 133.665 130.542 124.22 115.041 109.755 104.673 96.3091 94.5746 90.6448 83.8243 77.828 75.7297 71.5565 67.9807 64.2208 60.4596 57.1333 54.2487 53.15 49.6493 47.4791 43.4235 42.804 42.5031 39.8173 36.1509 34.186 33.6447 31.598 28.2933 28.3191 27.2333 25.4636 23.6714 22.5907 21.9325 20.7388 19.2141 18.6653 16.59 16.4931 15.3661 15.1645 14.4219 13.6063 12.8385}} set ::GlobalFitIQGraph(y,mapped) "1" set ::GlobalFitIQGraph(margin,top) "0" set ::GlobalFitIQGraph(l,borderwidth) "2" @@ -2564,12 +3258,12 @@ set ::GlobalFitIQGraph(x,mapped) "1" set ::GlobalFitIQGraph(y,factor) "1.0" set ::GlobalFitIQGraph(stipples) {bdiagonal1 bdiagonal2 checker2 checker3 cross1 cross2 cross3 crossdiag dot1 dot2 dot3 dot4 fdiagonal1 fdiagonal2 hline1 hline2 lbottom ltop rbottom rtop vline1 vline2} set ::GlobalFitIQGraph(graph,borderwidth) "0" -set ::GlobalFitIQGraph(e,resdata) {{0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 0.0 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::ResIQGraph(e.errstipples) "" set ::ResIQGraph(e,restags) "" set ::ResIQGraph(title) "unknown" diff --git a/doc/images/form_factor/Ellipsoid/RotationsEllipsoid.opj b/doc/images/form_factor/Ellipsoid/RotationsEllipsoid.opj index 6bee9781..cb601c7f 100644 Binary files a/doc/images/form_factor/Ellipsoid/RotationsEllipsoid.opj and b/doc/images/form_factor/Ellipsoid/RotationsEllipsoid.opj differ diff --git a/doc/images/form_factor/Ellipsoid/Triaxial_Ellipsoid.jpg b/doc/images/form_factor/Ellipsoid/Triaxial_Ellipsoid.jpg new file mode 100644 index 00000000..60a9f852 Binary files /dev/null and b/doc/images/form_factor/Ellipsoid/Triaxial_Ellipsoid.jpg differ diff --git a/doc/images/form_factor/Ellipsoid/spheroid_core_shell.png b/doc/images/form_factor/Ellipsoid/spheroid_core_shell.png new file mode 100644 index 00000000..3215f058 Binary files /dev/null and b/doc/images/form_factor/Ellipsoid/spheroid_core_shell.png differ diff --git a/doc/images/form_factor/Ellipsoid/triaxEllSh.opj b/doc/images/form_factor/Ellipsoid/triaxEllSh.opj index c5d86bb4..a69584fc 100644 Binary files a/doc/images/form_factor/Ellipsoid/triaxEllSh.opj and b/doc/images/form_factor/Ellipsoid/triaxEllSh.opj differ diff --git a/doc/images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell_1.png b/doc/images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell_1.png new file mode 100644 index 00000000..6e3dd75c Binary files /dev/null and b/doc/images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell_1.png differ diff --git a/doc/images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell_2.png b/doc/images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell_2.png new file mode 100644 index 00000000..0501fe7c Binary files /dev/null and b/doc/images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell_2.png differ diff --git a/doc/manual/SASfit_history.tex b/doc/manual/SASfit_history.tex index aad12f4c..a3e35aba 100644 --- a/doc/manual/SASfit_history.tex +++ b/doc/manual/SASfit_history.tex @@ -1,9 +1,14 @@ \appendix{History} \begin{description} -\item[201x-xx-xx] \SASfit 0.94.10 +\item[2018-xx-xx] \SASfit 0.94.10 \begin{itemize} - \item bug fix in the algorithm for calculating the resolution parameter in case of averaging neighbouring data points - \item plugin implementation of several variants of helices + \item The form factors \texttt{"EllipsoidalCoreShell"}, \texttt{"Ellipsoid i"}, \texttt{"Ellipsoid ii"}, and \texttt{"triaxEllShell1"} have been disabled and replaced by a series of plug-in functions. Those replacements make use of a faster routine for multidimensional integrals (pcubature). Because of this an optional size distribution became part of the supplied plug-in form factors. + \item bug fix of unit conversion via clipboard + \item added a plug-in for a random flight structure factor + \item bug fix in the algorithm for calculating the resolution parameter in case of averaging neighboring data points + \item plug-in implementation of several variants of helices + \item plug-in for rectangular parallelepipeds have been extended so that it can have a size distribution of one, two or all three axis. The multiple integration is done by using the pcubature code from Steven G. Johnson + \item multi dimensional integration package "cubature" from Steven G. Johnson becomes generally available also in plug-ins (\href{https://github.com/stevengj/cubature}{cubature}) \end{itemize} \item[2017-08-16] \SASfit 0.94.9 \begin{itemize} @@ -41,7 +46,7 @@ \begin{itemize} \item implementation of another cumulant formula for DLS \item bug-fix in the unit conversion routine - \item implementation of GMRES, Bi-CGStab, TFQMR and Andersen Accelarion + \item implementation of GMRES, Bi-CGStab, TFQMR and Andersen Acceleration for solving efficiently the Ornstein Zernicke fixpoint problem \item bug fix: since version 0.94.4 the new interrupt option suppressed a proper error reporting to the GUI for undefined input values @@ -89,8 +94,8 @@ \item[2014-07-02] \SASfit 0.94.3 \begin{itemize} \item bug fix in the plugin for parallel epiped - \item spelling errors in the menue interface - \item in case of slow convergence the OZ solver can be interupted now + \item spelling errors in the menu interface + \item in case of slow convergence the OZ solver can be interrupted now \end{itemize} \item[2014-02-06] \SASfit 0.94.2 \begin{itemize} @@ -206,8 +211,8 @@ \item optical (layout) GUI improvements: \begin{itemize} \item removed thick margin around text boxes for ISP/analyt results - \item added resizeable file list in \texttt{ISP} window - \item added resizeable 'merge files' list when loading data files + \item added resizable file list in \texttt{ISP} window + \item added resizable 'merge files' list when loading data files \end{itemize} \item added menu->tools->toggle console to show the console, it is hidden by default now \item added \texttt{OPTIM} parameter to \texttt{src/CMakeLists.txt} for optimized binary generation on the underlying hardware, use: '\texttt{cmake -DOPTIM=TRUE}' diff --git a/doc/manual/SASfit_pluginsFF_elliptical_obj.tex b/doc/manual/SASfit_pluginsFF_elliptical_obj.tex index ee0c2837..d7a0a38a 100644 --- a/doc/manual/SASfit_pluginsFF_elliptical_obj.tex +++ b/doc/manual/SASfit_pluginsFF_elliptical_obj.tex @@ -5,7 +5,7 @@ \section{Ellipsoidal Objects} \begin{center} \includegraphics[width=0.85\textwidth]{../images/form_factor/Ellipsoid/Ellipsoide.png} \end{center} -\caption{Ellipse of revolution or spheroid and triaxial ellipse} +\caption{Ellipse of revolution (spheroid) and triaxial ellipse} \label{fig:EllipsoidalObjects} \end{figure} @@ -147,7 +147,7 @@ \subsection{Ellipsoid with two equal equatorial semi-axis $R$ and volume $V$} \clearpage \subsection{Ellipsoidal core shell structure} \label{sect:EllipsoidalCoreShell} ~\\ -For these form factor plugins a size distribution parameter has been included directly in the form factor to avoid apply nested numerical integration routines. A routine for multi-dimensional integration routines (\texttt{pcubature} \cite{Johnson}) has been used instead. +For these form factor plugins a size distribution parameter has been included directly in the form factor to avoid applying nested numerical integration routines. A routine for multi-dimensional integration (\texttt{pcubature} \cite{Johnson}) has been used instead. \begin{figure}[htb] \begin{center} \includegraphics[width=0.5\textwidth,height=0.28855\textwidth]{../images/form_factor/Ellipsoid/ellipsoidalShell.png} @@ -155,13 +155,14 @@ \subsection{Ellipsoidal core shell structure} \caption{Ellipsoid of revolution with an outer shell of constant thickness $t$} \label{ellipsoidalShell} \end{figure} \begin{align} -I_\text{ECSh}(Q) = \left\langle F^2(Q,\mu) \right\rangle -& = \int_0^1 \left[F(Q,\mu)\right]^2 d\mu \\ -\left\langle F(Q,\mu) \right\rangle^2 & = \left[\int_0^1 F(Q,\mu) -d\mu \right]^2 +I_\text{ECSh}(Q,R_\mathrm{p},R_\mathrm{e},t) = \left\langle F^2(Q,R_\mathrm{p},R_\mathrm{e},t) \right\rangle +& = \int_0^1 \left[F(Q,R_\mathrm{p},R_\mathrm{e},t,\mu)\right]^2 d\mu \\ +\left\langle F(Q,R_\mathrm{p},R_\mathrm{e},t) \right\rangle & = \int_0^1 F(Q,R_\mathrm{p},R_\mathrm{e},t,\mu) +d\mu \end{align} +with \begin{align} -F(Q,\mu) &= \left(\eta_\text{core}-\eta_\text{shell}\right) V_c\left[ +F(Q,R_\mathrm{p},R_\mathrm{e},t,\mu) &= \left(\eta_\text{core}-\eta_\text{shell}\right) V_c\left[ \frac{3j_1(x_c)}{x_c}\right] +\left(\eta_\text{shell}-\eta_\text{sol}\right) V_t\left[ \frac{3j_1(x_t)}{x_t}\right] \nonumber \\ @@ -175,16 +176,45 @@ \subsection{Ellipsoidal core shell structure} \eta_\text{core} &: \text{scattering length density of core} \nonumber \\ \eta_\text{shell} &: \text{scattering length density of shell} \nonumber \\ \eta_\text{sol} &: \text{scattering length density of solvent} \nonumber \\ -R_\mathrm{p} &: \text{semi-principal axes of elliptical core} \nonumber \\ +R_\mathrm{p} &: \text{polar semi-axes of elliptical core} \nonumber \\ R_\mathrm{e} &: \text{equatorial semi-axis of elliptical core} \nonumber \\ t &: \text{thickness of shell} \nonumber \\ V_c &: \text{volume of core} \nonumber \\ V_t &: \text{total volume of core along with shell} \nonumber \end{align} +Several variants including a size distribution have been implemented which just differ if only none, one or both axis scale with the same size distribution and if additionally also scales with that distribution. +\begin{align*} +\text{\texttt{Ellipsoidal Shell}} &: \left\langle F^n(Q,R_\mathrm{p},R_\mathrm{e},t)\right\rangle\\ +\text{\texttt{Ellipsoidal Shell (t)}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,R_\mathrm{p},R_\mathrm{e},\nu t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{Ellipsoidal Shell (Rp)}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu R_\mathrm{p},R_\mathrm{e}, t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{Ellipsoidal Shell (Rp t)}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu R_\mathrm{p},R_\mathrm{e},\nu t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{Ellipsoidal Shell (Re)}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,R_\mathrm{p},\nu R_\mathrm{e},t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{Ellipsoidal Shell (Re t)}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,R_\mathrm{p},\nu R_\mathrm{e},\nu t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{Ellipsoidal Shell (Re Rp)}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu R_\mathrm{p},\nu R_\mathrm{e},t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{Ellipsoidal Shell (Re Rp t)}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu R_\mathrm{p},\nu R_\mathrm{e},\nu t)\right\rangle \mathrm{d}\nu +\end{align*} +with $n$ being either 1 or 2 depending if the size averaged amplitude or the size averaged intensity needs to be calculated. As a size distribution a lognormal distribution is assumed where all parameters are scaled simultaneously. The used lognormal distribution is defined as +$$ +\mathrm{LogNorm}(x,\sigma) = \frac{1}{\sqrt{2\pi}x} \exp\left(-\frac{\ln^2(x)}{2\sigma^2}\right) +$$ \vspace{0.5cm} - -\underline{Input Parameters for model \texttt{EllipsoidalCoreShell}:} +~\\ +\underline{Input Parameters for model \texttt{Ellipsoidal Shell}:} +\begin{description} +\item[\texttt{R\_p}] semi-principal polar axes of elliptical core $R_\mathrm{p}$ +\item[\texttt{R\_e}] equatorial semi-axis axes of elliptical core $R_\mathrm{e}$ +\item[\texttt{dummy}] not used +\item[\texttt{t}] thickness of shell $t$ +\item[\texttt{dummy}] not used +\item[\texttt{eta\_core}] scattering length density of core $\eta_\text{c}$ +\item[\texttt{eta\_shell}] scattering length density of shell $\eta_\text{sh}$ +\item[\texttt{eta\_sol}] scattering length density of solvent $\eta_\text{sol}$ +\end{description} +~\\ +\underline{Input Parameters for model \texttt{Ellipsoidal Shell (t)}, \texttt{Ellipsoidal Shell (Rp)},} +\underline{\texttt{Ellipsoidal Shell (Rp t)}, \texttt{Ellipsoidal Shell (Re)}, \texttt{Ellipsoidal Shell (Re t)},} +\underline{\texttt{Ellipsoidal Shell (Re Rp)}, \texttt{Ellipsoidal Shell (Re Rp t)}:} \begin{description} \item[\texttt{R\_p}] semi-principal polar axes of elliptical core $R_\mathrm{p}$ \item[\texttt{R\_e}] equatorial semi-axis axes of elliptical core $R_\mathrm{e}$ @@ -198,10 +228,9 @@ \subsection{Ellipsoidal core shell structure} \begin{figure}[htb] \begin{center} -\includegraphics[width=0.768\textwidth,height=0.588\textwidth]{../images/form_factor/Ellipsoid/ellipsoidal_core_shell.png} +\includegraphics[width=0.768\textwidth,height=0.588\textwidth]{../images/form_factor/Ellipsoid/spheroid_core_shell.png} \end{center} -\caption{form factor of an ellipsoidal core shell $a$, $b$, $b$ and -$t$.} \label{fig:I_ellipsoidal_core_shell} +\caption{Form factor of an ellipsoidal core shell structure including a lognormal size distribution.} \label{fig:I_ellipsoidal_core_shell} \end{figure} @@ -209,6 +238,7 @@ \subsection{Ellipsoidal core shell structure} \clearpage \subsection{triaxial ellipsoidal core shell structure} \label{sect:triaxEllShell1} ~\\ +Also for these form factor plugins a size distribution parameter has been included directly in the form factor similar to the ellipsoidal shell of revolution to avoid applying nested numerical integration routines. As for the triaxial ellipsoid already a double integration for the orientational averaging is required it becomes even more important to have an optimized integration routine for including an additional size distribution, i.e an additional integration. The routine for multi-dimensional integration (\texttt{pcubature} \cite{Johnson}) has been used. \begin{figure}[htb] \begin{center} @@ -220,7 +250,11 @@ \subsection{triaxial ellipsoidal core shell structure} \end{figure} \begin{align} -I_\text{triaxEllSh}(Q) &= \int^1_0 \int ^1_0 dx\,dy\, K_\text{sh}^2(Q,R,R_t)\\ +I_\text{triaxEllSh}(Q) = \left\langle F^2(Q,a,b,c,t) \right\rangle &= \int^1_0 \int ^1_0 dx\,dy\, K_\text{sh}^2(Q,R,R_t)\\ +\left\langle F(Q,a,b,c,t) \right\rangle & = \int^1_0 \int ^1_0 dx\,dy\, K_\text{sh}(Q,R,R_t) +\end{align} +with +\begin{align} K(QR) &= 3 \frac{\sin QR - QR\cos QR}{(QR)^3} \\ K_\text{sh}(Q,R,R_t) &= \left(\eta_\text{c}-\eta_\text{sh}\right)K(QR)+\left(\eta_\text{sh}-\eta_\text{sol}\right)K(QR_t) \\ R^2 &= \left[a^2\cos^2\left(\pi x/2\right) + b^2\sin^2\left(\pi x/2\right)\right](1-y^2)+c^2y^2 \nonumber \\ @@ -241,13 +275,44 @@ \subsection{triaxial ellipsoidal core shell structure} V_t &: \text{total volume of core along with shell} \nonumber \end{align} +Several variants including a size distribution have been implemented which just differ if only none, one or both axis scale with the same size distribution and if additionally also scales with that distribution. +\begin{align*} +\text{\texttt{triax ellip shell}} &: \left\langle F^n(Q, a, b, c, t)\right\rangle\\ +\text{\texttt{triax ellip shell t}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q, a, b, c,\nu t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{triax ellip shell 1}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu a, b, c, t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{triax ellip shell 1t}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu a, b, c,\nu t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{triax ellip shell 2}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu a,\nu b, c, t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{triax ellip shell 2t}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu a,\nu b, c,\nu t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{triax ellip shell 3}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu a,\nu b,\nu c, t)\right\rangle \mathrm{d}\nu\\ +\text{\texttt{triax ellip shell 3t}} &: \int_0^\infty \mathrm{LogNorm}(\nu,\sigma) \left\langle F^n(Q,\nu a,\nu b,\nu c,\nu t)\right\rangle \mathrm{d}\nu +\end{align*} +with $n$ being either 1 or 2 depending if the size averaged amplitude or the size averaged intensity needs to be calculated. As a size distribution a lognormal distribution is assumed where all parameters are scaled simultaneously. The used lognormal distribution is defined as +$$ +\mathrm{LogNorm}(x,\sigma) = \frac{1}{\sqrt{2\pi}x} \exp\left(-\frac{\ln^2(x)}{2\sigma^2}\right) +$$ + \vspace{3cm} -\underline{Input Parameters for model \texttt{triaxEllShell1}:} +\noindent \underline{Input Parameters for model \texttt{triax ellip shell}:} +\begin{description} +\item[\texttt{a}] semi-axes of elliptical core $a$ +\item[\texttt{b}] semi-axes of elliptical core $b$ +\item[\texttt{c}] semi-axes of elliptical core $c$ +\item[\texttt{t}] thickness of shell $t$ +\item[\texttt{dummy}] not used +\item[\texttt{eta\_c}] scattering length density of core $\eta_\text{c}$ +\item[\texttt{eta\_sh}] scattering length density of shell $\eta_\text{sh}$ +\item[\texttt{eta\_sol}] scattering length density of solvent $\eta_\text{sol}$ +\end{description} +~\\ +\underline{Input Parameters for model \texttt{triax ellip shell t}, \texttt{triax ellip shell 1},} +\underline{\texttt{triax ellip shell 1t}, \texttt{triax ellip shell 2}, \texttt{triax ellip shell 2t},} +\underline{\texttt{triax ellip shell 3}, \texttt{triax ellip shell 3t}}: \begin{description} \item[\texttt{a}] semi-axes of elliptical core $a$ \item[\texttt{b}] semi-axes of elliptical core $b$ \item[\texttt{c}] semi-axes of elliptical core $c$ \item[\texttt{t}] thickness of shell $t$ +\item[\texttt{sigma}] width of the LogNorm size distribution $\sigma$ \item[\texttt{eta\_c}] scattering length density of core $\eta_\text{c}$ \item[\texttt{eta\_sh}] scattering length density of shell $\eta_\text{sh}$ \item[\texttt{eta\_sol}] scattering length density of solvent $\eta_\text{sol}$ @@ -255,9 +320,10 @@ \subsection{triaxial ellipsoidal core shell structure} \begin{figure}[htb] \begin{center} -\includegraphics[width=0.768\textwidth,height=0.588\textwidth]{../images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell.png} +\includegraphics[width=0.48\textwidth]{../images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell_1.png} +\includegraphics[width=0.48\textwidth]{../images/form_factor/Ellipsoid/triax_ellipsoidal_core_shell_2.png} \end{center} \caption{Form factor of a triaxial ellipsoidal core shell with semi -axis $a$, $b$ and $c$ and a shell thickness $t$.} +axis $a$, $b$ and $c$, with and without a shell thickness $t$ plus an additional size distribution.} \label{fig:I_triax_ellipsoidal_core_shell} \end{figure} \ No newline at end of file diff --git a/doc/manual/sasfit.aux b/doc/manual/sasfit.aux index 339077d3..ac2153c3 100644 --- a/doc/manual/sasfit.aux +++ b/doc/manual/sasfit.aux @@ -1534,14 +1534,15 @@ \@writefile{toc}{\contentsline {subsection}{\tocsubsection {}{8.4.3}{Ellipsoidal core shell structure}}{416}{subsection.1712}} \@writefile{lof}{\contentsline {figure}{\numberline {8.41}{\ignorespaces Ellipsoid of revolution with an outer shell of constant thickness $t$}}{416}{figure.1713}} \newlabel{ellipsoidalShell}{{8.41}{416}{Ellipsoid of revolution with an outer shell of constant thickness 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\bibcite{Bevington2003}{17} \bibcite{Blaurock1982}{18} -\@writefile{toc}{\contentsline {chapter}{\tocappendix {Appendix}{}{Bibliography}}{529}{appendix*.2213}} +\@writefile{toc}{\contentsline {chapter}{\tocappendix {Appendix}{}{Bibliography}}{531}{appendix*.2214}} \@writefile{lof}{\addvspace {10\p@ }} \@writefile{lot}{\addvspace {10\p@ }} \bibcite{Bohren1983}{19} diff --git a/doc/manual/sasfit.bib.bak b/doc/manual/sasfit.bib.bak deleted file mode 100644 index 7670fbda..00000000 --- a/doc/manual/sasfit.bib.bak +++ /dev/null @@ -1,4840 +0,0 @@ -% Encoding: windows-1252 - -@MISC{Rfactor, - author = {Online Dictionary of crystallography}, - title = {R factor}, - howpublished = {\href{http://reference.iucr.org/dictionary/R_factor}{http://reference.iucr.org/dictionary/R\_factor}}, - url = {http://reference.iucr.org/dictionary/R_factor}, - owner = {kohlbrecher}, - timestamp = {2013.04.26} -} - -@ARTICLE{Agarwal2007, - author = {R. P. Agarwal and Donal O'Regan and D. R. Sahu}, - title = {Iterative construction of fixed points of nearly asymptotically nonexpansive - mappings}, - year = {2007}, - volume = {8}, - number = {1}, - pages = {61--79}, - url = {http://www.ybook.co.jp/online2/jncav8-1.html}, - journal = {Journal of Nonlinear and - - Covnex Analysis}, - owner = {kohlbrecher}, - timestamp = {2014.06.09} -} - -@ARTICLE{Alexander1984, - author = {Alexander, S. and Chaikin, P. M. and Grant, P. and Morales, G. J. - and Pincus, P. and Hone, D.}, - title = {Charge renormalization, osmotic pressure, and bulk modulus of colloidal - crystals: Theory}, - year = {1984}, - volume = {80}, - number = {11}, - pages = {5776-5781}, - doi = {http://dx.doi.org/10.1063/1.446600}, - url = {http://scitation.aip.org/content/aip/journal/jcp/80/11/10.1063/1.446600}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.20} -} - -@ARTICLE{Anderson1965, - author = {Anderson, Donald G.}, - title = {Iterative Procedures for Nonlinear Integral Equations}, - year = {1965}, - volume = {12}, - number = {4}, - month = oct, - pages = {547--560}, - issn = {0004-5411}, - doi = {10.1145/321296.321305}, - url = {http://doi.acm.org/10.1145/321296.321305}, - acmid = {321305}, - address = {New York, NY, USA}, - issue_date = {Oct. 1965}, - journal = {J. ACM}, - numpages = {14}, - owner = {kohlbrecher}, - publisher = {ACM}, - timestamp = {2015.12.16} -} - -@ARTICLE{Asakura1958, - author = {Asakura, Sho and Oosawa, Fumio}, - title = {Interaction between particles suspended in solutions of macromolecules}, - year = {1958}, - volume = {33}, - number = {126}, - pages = {183--192}, - issn = {1542-6238}, - doi = {10.1002/pol.1958.1203312618}, - url = {http://dx.doi.org/10.1002/pol.1958.1203312618}, - abstract = {An attractive force appears between particles suspended in solutions - of macromolecules when there is neither direct interaction between - two particles nor energetic interaction between particles and solute - macromolecules. The magnitude of this force is of the order of the - osmotic pressure of the solution of macromolecules and the range - is of the order of the diameter of macromolecules. This force is - calculated as a function of concentration, shape, and charge of macromolecules, - and it is shown that it becomes stronger in solutions of chain macromolecules - or of macromolecules of dissymmetrical shape than in solutions of - rigid spherical macromolecules at the same net concentration. If - macromolecules have charge, the force can be greatly intensified. - In every case numerical estimation is made, and it is found that - actually this kind of force can have a remarkable influence on the - state of suspended particles. Numerical examples of the critical - concentration of particles at their macroscopic aggregation are given. - Finally a short description is added on the effect of energetic interaction - between particles and macromolecules.}, - journal = {Journal of Polymer Science}, - owner = {kohlbrecher}, - publisher = {Interscience Publishers, Inc.}, - timestamp = {2013.11.21} -} - -@ARTICLE{scatt97, - author = {N. W. Ashcroft and L. Lenker}, - title = {Structure and resistivity of liquid metals}, - year = {1966}, - volume = {145}, - number = {1}, - month = {May}, - pages = {83-90}, - journal = {Physical Review}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Ballone1986, - author = {Ballone, P. and Pastore, G. and Galli, G. and Gazzillo, D.}, - title = {Additive and non-additive hard sphere mixtures}, - year = {1986}, - volume = {59}, - number = {2}, - pages = {275-290}, - doi = {10.1080/00268978600102071}, - eprint = {http://www.tandfonline.com/doi/pdf/10.1080/00268978600102071}, - url = {http://www.tandfonline.com/doi/abs/10.1080/00268978600102071}, - journal = {Molecular Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.08} -} - -@ARTICLE{Barboy1974, - author = {B. Barboy}, - title = {On a representation of the equation of state of - - fluids in terms of the adhesive hard-sphere model}, - year = {1974}, - volume = {61}, - number = {8}, - pages = {3194-3196}, - journal = {J. Chem. Phys.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Barker:gl0350, - author = {Barker, J. G. and Pedersen, J. S.}, - title = {Instrumental Smearing Effects in Radially Symmetric Small-Angle Neutron - Scattering by Numerical and Analytical Methods}, - year = {1995}, - volume = {28}, - number = {2}, - month = {Apr}, - pages = {105--114}, - doi = {10.1107/S0021889894010095}, - url = {http://dx.doi.org/10.1107/S0021889894010095}, - journal = {Journal of Applied Crystallography}, - owner = {kohlbrecher}, - timestamp = {2010.05.08} -} - -@ARTICLE{Baxter1968, - author = {R.J. Baxter}, - title = {Percus-Yevick equation for hard spheres with - - surface adhesion}, - year = {1968}, - volume = {49}, - number = {6}, - pages = {2770-2774}, - doi = {10.1063/1.1673684}, - url = {http://scitation.aip.org/content/aip/journal/jcp/52/9/10.1063/1.1673684}, - journal = {J. Chem. Phys.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{beaucage96, - author = {G. Beaucage}, - title = {Small-Angle Scattering from Polymeric Mass Fractals of Arbitrary - Mass-Fractal Dimension}, - year = {1996}, - volume = {29}, - pages = {134-146}, - journal = {J. Appl. Cryst.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{beaucage95, - author = {G. Beaucage}, - title = {Approximations Leading to a Unified Exponential/Power-Law Approach - to Small-Angle Scattering}, - year = {1995}, - volume = {28}, - pages = {717-728}, - journal = {J. Appl. Cryst.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Benoit53, - author = {H. Benoit}, - title = {On the effect of branching and polydispersity on the angular distribution - of the light scattered by gaussian coils}, - year = {1953}, - volume = {11}, - pages = {507-510}, - journal = {J. Polym. Sci.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Berndt2006, - author = {Berndt, Ingo and Pedersen, Jan Skov and Lindner, Peter and Richtering, - Walter}, - title = {Influence of Shell Thickness and Cross-Link Density on the Structure - of Temperature-Sensitive Poly-N-Isopropylacrylamide−Poly-N-Isopropylmethacrylamide - Core−Shell Microgels Investigated by Small-Angle Neutron Scattering}, - year = {2006}, - volume = {22}, - number = {1}, - pages = {459-468}, - note = {PMID: 16378460}, - doi = {10.1021/la052463u}, - eprint = {http://pubs.acs.org/doi/pdf/10.1021/la052463u}, - url = {http://pubs.acs.org/doi/abs/10.1021/la052463u}, - abstract = {Swelling properties of doubly temperature sensitive core−shell microgels - consisting of two thermosensitive polymers with lower critical solution - temperatures (LCTS) at, respectively, 34 °C in the core and 44 °C - in the shell have been investigated by small-angle neutron scattering - (SANS). A core−shell form factor has been employed to evaluate - the structure, and the real space particle structure is expressed - by radial density profiles. By this means, the influences of both - shell/core mass composition and shell cross-linker content on the - internal structure have been revealed at temperatures above, between, - and below the LCSTs. Higher shell/core mass ratios lead to an increased - expansion of the core at temperatures between the LCSTs, whereas - a variation of cross-linker in the shell mainly effects the dimensions - of the shell. The influence on the core structure was interpreted - as resulting from an elastic force developed from the swollen shell. - At temperatures below the core LCST, the core cannot swell to its - native size (i.e., in the absence of a shell), because the maximum - expanded shell network prohibits further swelling. Thus, depending - on temperature, the shell either expands or compresses the core.}, - journal = {Langmuir}, - owner = {Kohlbrecher}, - timestamp = {2012.04.02} -} - -@ARTICLE{Berndt2006a, - author = {Berndt, Ingo and Pedersen, Jan Skov and Richtering, Walter}, - title = {Temperature-Sensitive Core–Shell Microgel Particles with Dense - Shell}, - year = {2006}, - volume = {118}, - number = {11}, - pages = {1769--1773}, - issn = {1521-3757}, - doi = {10.1002/ange.200503888}, - url = {http://dx.doi.org/10.1002/ange.200503888}, - journal = {Angewandte Chemie}, - keywords = {Blockcopolymere, Kern-Schale-Nanopartikel, Mikrogele, Neutronenbeugung}, - owner = {Kohlbrecher}, - publisher = {WILEY-VCH Verlag}, - timestamp = {2012.04.02} -} - -@ARTICLE{Berndt2005, - author = {Berndt, Ingo and Pedersen, Jan Skov and Richtering, Walter}, - title = {Structure of Multiresponsive “Intelligentâ€? Core−Shell Microgels}, - year = {2005}, - volume = {127}, - number = {26}, - pages = {9372-9373}, - note = {PMID: 15984856}, - doi = {10.1021/ja051825h}, - eprint = {http://pubs.acs.org/doi/pdf/10.1021/ja051825h}, - url = {http://pubs.acs.org/doi/abs/10.1021/ja051825h}, - abstract = {A doubly temperature-sensitive core−shell microgel composed of two - temperature-sensitive polymers with different lower critical solution - temperatures (LCSTs) in the core and shell has been studied by small-angle - neutron scattering (SANS). The application of a novel universal form - factor model in the analysis of the SANS data reveals that the radial - density profile at temperatures above the LCSTs of both polymers - can be well described by a two-box profile with narrow interfaces. - At temperatures between the LCSTs, the radial density profile reveals - that the core in the core−shell microgel has larger dimensions - than the naked core. Thus the swollen shell pulls the core apart. - At temperatures below both LCSTs, however, the shell restricts the - core swelling, and the core is found to be smaller than in its native - state. This clearly demonstrates the mutual influence of core and - shell swelling.}, - journal = {Journal of the American Chemical Society}, - owner = {Kohlbrecher}, - timestamp = {2012.04.02} -} - -@ARTICLE{scatt151, - author = {P. van Beurten and A. Vrij}, - title = {Polydispersity effects in the small-angle scattering of concentrated - solutions of colloidal spheres}, - year = {1981}, - volume = {74}, - number = {5}, - month = {March}, - pages = {2744-2748}, - journal = {J. Chem. Phys.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@BOOK{Bevington2003, - author = {Philip Bevington and D. Keith Robinson}, - title = {Data Reduction and Error Analysis for the Physical Sciences}, - year = {2002}, - edition = {3rd}, - note = {ISBN-10: 0072472278, ISBN-13: 978-0072472271}, - publisher = {McGraw-Hill}, - url = {http://catalogs.mhhe.com/mhhe/viewProductDetails.do?isbn=0072472278}, - abstract = {The purpose of this book is to provide an introduction to the concepts - of statistical analysis of data for students at the undergraduate - and graduate level, and to provide tools for data reduction and error - analysis commonly required in the physical sciences. The presentation - is developed from a practical point of view, including enough derivation - to justify the results, but emphasizing methods of handling data - more than theory. The text provides a variety of numerical and graphical - techniques. Computer programs that support these techniques will - be available on an accompanying website in both Fortran and C++.}, - month = {23 July}, - owner = {kohlbrecher}, - timestamp = {2013.04.26} -} - -@ARTICLE{Blaurock1982, - author = {A. E. Blaurock}, - title = {Evidence of bilayer structure and of membrane interactions from X-ray - diffraction analysis}, - year = {1982}, - volume = {650}, - number = {4}, - pages = {167 - 207}, - doi = {10.1016/0304-4157(82)90016-8}, - url = {http://www.sciencedirect.com/science/article/B6T22-47T348J-3W/2/6bece612b691d434da265844aa3e86eb}, - journal = {Biochimica et Biophysica Acta (BBA) - Reviews on Biomembranes}, - owner = {kohlbrecher}, - timestamp = {2010.06.04} -} - -@BOOK{Bohren1983, - author = {C.F. Bohren and D.R. Huffman}, - title = {Absorption and Scattering of Light by Small Particles}, - year = {1983}, - publisher = {Wiley, New York}, - pages = {82–129}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@INBOOK{Bomont2008, - author = {Bomont, Jean-Marc}, - title = {Recent Advances in the Field of Integral Equation Theories: Bridge - Functions and Applications to Classical Fluids}, - booktitle = {Advances in Chemical Physics}, - year = {2008}, - publisher = {John Wiley \& Sons, Inc.}, - isbn = {9780470259498}, - chapter = {Chapter 1}, - pages = {1--84}, - doi = {10.1002/9780470259498.ch1}, - url = {http://dx.doi.org/10.1002/9780470259498.ch1}, - keywords = {statistical mechanics, liquid state, thermodynamics quantities, nonconsistent - integral equations, thermodynamic properties}, - owner = {kohlbrecher}, - timestamp = {2013.11.02} -} - -@ARTICLE{Bomont2003, - author = {Bomont, J. M. and Bretonnet, J. L.}, - title = {A self-consistent integral equation: Bridge function and thermodynamic - properties for the Lennard-Jones fluid}, - year = {2003}, - volume = {119}, - number = {4}, - pages = {2188-2191}, - doi = {http://dx.doi.org/10.1063/1.1583675}, - url = {http://scitation.aip.org/content/aip/journal/jcp/119/4/10.1063/1.1583675}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.11} -} - -@ARTICLE{Bomont2004, - author = {Bomont, Jean-Marc and Bretonnet, Jean-Louis}, - title = {A consistent integral equation theory for hard spheres}, - year = {2004}, - volume = {121}, - number = {3}, - pages = {1548-1552}, - doi = {http://dx.doi.org/10.1063/1.1764772}, - url = {http://scitation.aip.org/content/aip/journal/jcp/121/3/10.1063/1.1764772}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.11} -} - -@ARTICLE{Booth1999, - author = {Michael J. Booth and A.G. Schlijper and L.E. Scales and A.D.J. Haymet}, - title = {Efficient solution of liquid state integral equations using the Newton-GMRES - algorithm}, - year = {1999}, - volume = {119}, - number = {2–3}, - pages = {122 - 134}, - issn = {0010-4655}, - doi = {http://dx.doi.org/10.1016/S0010-4655(99)00186-1}, - url = {http://www.sciencedirect.com/science/article/pii/S0010465599001861}, - journal = {Computer Physics Communications }, - keywords = {Newton}, - owner = {kohlbrecher}, - timestamp = {2013.12.03} -} - -@ARTICLE{scatt144, - author = {M. Born and H. S. Green}, - title = {A general kinetic theory of liquids}, - year = {1947}, - volume = {A190}, - pages = {455-474}, - journal = {Proc. Roy. Soc.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{scatt145, - author = {M. Born and H. S. Green}, - title = {A general kinetic theory of liquids. {IV. Quantum} mechanics of fluids}, - year = {1947}, - volume = {A191}, - pages = {168-181}, - journal = {Proc. Roy. Soc.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{scatt142, - author = {M. Born and H. S. Green}, - title = {A general kinetic theory of liquids {I. The} molecular distribution - functions}, - year = {1946}, - volume = {A188}, - pages = {10-18}, - journal = {Proc. Roy. Soc.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Boucher1983, - author = {B Boucher and P Chieux and P Convert and M Tournarie}, - title = {Small-angle neutron scattering determination of medium and long range - order in the amorphous metallic alloy TbCu 3.54}, - year = {1983}, - volume = {13}, - number = {7}, - pages = {1339}, - url = {http://stacks.iop.org/0305-4608/13/i=7/a=006}, - abstract = {Small-angle neutron scattering measurements have been performed on - the amorphous metallic alloy TbCu 3.54 in its as-prepared state and - after annealing for 5 h at 240 degrees C. The sample impurity atoms - such as hydrogen, argon and oxygen were identified and their concentrations - determined. At very small momentum transfer values a very strong - scattering is observed which decreases as q -3 in an oscillatory - fashion. A well defined weak ring is observed at about 0.2 AA -1 - . Annealing doubles the intensity of the whole pattern. In a model - description of the observed small-angle scattering, the alloy is - composed of domains several thousand of angstroms wide, in which - the impurities tend to accumulate near the walls. The impurities - might be diluted in the alloy or concentrated such as in small bubbles. - In any case, their distribution within the domains is characteristic. - The annealing purifies the centres of the domains and repels the - impurities to the periphery.}, - journal = {Journal of Physics F: Metal Physics}, - owner = {kohlbrecher}, - timestamp = {2016.01.20} -} - -@ARTICLE{Burchard1996, - author = {W. Burchard and E. Michel and V. Trappe}, - title = {Conformational Properties of Multiply Twisted Ring Systems and Daisy-Like - Structures}, - year = {1996}, - volume = {29}, - number = {18}, - pages = {5934-5939}, - doi = {10.1021/ma9603286}, - url = {http://dx.doi.org/10.1021/ma9603286}, - abstract = {Two multiple ring systems are considered and relationships are derived - for the angular dependence of the scattered light (P(q)), the radius - of gyration (Rg) and the hydrodynamic radius (Rh). The two models - of consideration are (i) the multiply twisted ring system and (ii) - the daisy-like ring structure. The derivations are made on the basis - of the Wang?Uhlenbeck theorem on Gaussian distributions for the static - properties and the Kirkwood?Riseman preaverage approximation for - the hydrodynamics. The derived particle scattering factors show significant - differences for the two different ring systems. To distinguish the - multiply twisted ring system from a linear open chain, it is necessary - to measure the scattering intensity over a large q range. The daisy-like - structures resemble star-branched macromolecules but with numbers - of subrings 4 to 5 times smaller than the arm numbers in a star. - Differences between the shrinking factors and the ? parameter of - the various systems are noticeable and can be used to discern these - systems.}, - journal = {Macromolecules}, - owner = {Kohlbrecher}, - timestamp = {2009.07.01} -} - -@Article{Caccamo1996, - author = {C. Caccamo}, - title = {Integral equation theory description of phase equilibria in classical fluids}, - year = {1996}, - journal = {Physics Reports}, - volume = {274}, - number = {1-2}, - pages = {1 - 105}, - issn = {0370-1573}, - doi = {http://dx.doi.org/10.1016/0370-1573(96)00011-7}, - url = {http://www.sciencedirect.com/science/article/pii/0370157396000117}, - abstract = {We review the present status of applications of integral equation - theories (IETs) for the radial distribution function g(r), to the - determination of phase diagrams and stability conditions of simple - and charged classical fluids. After having recalled some basic concepts - and definitions in the structural description of fluid systems, a - number of \{IETs\} are examined by reporting the constituting equations - and solution procedures; these last are discussed also in relationship - with the actual calculation of coexistence lines and description - of the critical behavior of each envisaged theory. In this context, - the crucial role played by the fulfilment of thermodynamic consistency - in the improvement of the performances of the various approximations, - is highlighted. Then, a number of results of phase diagram determinations, - phase stability investigations, and estimates of critical exponents, - are reported for several neutral and charged model fluids (and their - mixtures) such as the hard sphere fluid, the square-well fluid, the - hard-core Yukawa fluid, the Lennard-Jones fluid, and charged hard - spheres in different regimes of density, sizes and charges. Calculations - of the phase diagram of a rigid molecule model of \{C60\} are also - reported. Besides their theoretical interest, these models are investigated - by many authors also because they can reasonably mimic real systems - like rare gas liquids, electrolyte solutions, molten salts, neutral - and charged micellar systems, and colloidal solutions. The related - experimental evidence is therefore frequently referred, and comparison - with experimental results is also performed in some case. Theoretical - results are usually presented in parallel with the available computer - simulation data, which are extensively quoted both with the aim of - a systematic assessment of the theories, and in order to offer a - more complete scenario of phase behavior calculations in classical - fluids. Perspectives and advantages of future extensions and applications - of \{IETs\} in different physical contexts in which phase coexistence - conditions seem worth of a timely investigation, are also discussed. - }, - keywords = {Integral equation theories}, - owner = {kohlbrecher}, - timestamp = {2013.11.02}, -} - -@ARTICLE{Caille1972, - author = {A. Caille}, - title = {X-ray scattering in smectic A}, - year = {1972}, - volume = {274}, - pages = {891-893}, - abstract = {The x-ray intensity, I(q), scattered by a smectic A single crystal, - was analyzed for q close to the Bragg wave vector |qz| = 2p/density - Expressions of the I(q) function was obtained for the 2 main directions - (z and x). The laws describing this process are different from those - for scattering by a solid. The characteristic exponent of the derived - function is dependent on temperature}, - journal = {Comptes Rendus des Seances de l'Academie des Sciences, Serie B: Sciences - Physiques}, - owner = {kohlbrecher}, - timestamp = {2010.06.04} -} - -@ARTICLE{Charpentier2001, - author = {Charpentier, I. and Jakse, N.}, - title = {Exact numerical derivatives of the pair-correlation function of simple - liquids using the tangent linear method}, - year = {2001}, - volume = {114}, - number = {5}, - pages = {2284-2292}, - doi = {http://dx.doi.org/10.1063/1.1332808}, - url = {http://scitation.aip.org/content/aip/journal/jcp/114/5/10.1063/1.1332808}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.12} -} - -@ARTICLE{Chihara1973, - author = {Chihara, Junzo}, - title = {Integral Euqations for Fluids with Long-Range and Short-Range Potentials: - Application to a Charged Particle System}, - year = {1973}, - volume = {50}, - number = {2}, - pages = {409-423}, - doi = {10.1143/PTP.50.409}, - eprint = {http://ptp.oxfordjournals.org/content/50/2/409.full.pdf+html}, - url = {http://ptp.oxfordjournals.org/content/50/2/409.abstract}, - journal = {Progress of Theoretical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.11} -} - -@ARTICLE{Choudhury2002, - author = {Choudhury, Niharendu and Ghosh, Swapan K.}, - title = {Integral equation theory of Lennard-Jones fluids: A modified Verlet - bridge function approach}, - year = {2002}, - volume = {116}, - number = {19}, - pages = {8517-8522}, - doi = {http://dx.doi.org/10.1063/1.1467894}, - url = {http://scitation.aip.org/content/aip/journal/jcp/116/19/10.1063/1.1467894}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.08} -} - -@ARTICLE{Chugh2012, - author = {R. Chugh and V. Kumar and S. Kumar}, - title = {Strong Convergence of a New Three Step Iterative Scheme in Banach - Spaces}, - year = {2012}, - volume = {2}, - number = {4}, - pages = {345--357}, - doi = {10.4236/ajcm.2012.24048}, - url = {http://www.scirp.org/journal/PaperInformation.aspx?paperID=26176#.U5WZoCjc2M8}, - journal = {American Journal of Computational Mathematics}, - owner = {kohlbrecher}, - timestamp = {2014.06.09} -} - -@ARTICLE{Damaschun1971, - author = {Damaschun, G. and P{\"{u}}rschel, H.-V.}, - title = {{R{\"{o}}ntgen-Kleinwinkelstreuung von isotropen Proben ohne Fernordnung. - I. Allgemeine Theorie}}, - year = {1971}, - volume = {27}, - number = {3}, - month = {May}, - pages = {193--197}, - doi = {10.1107/S0567739471000457}, - url = {http://dx.doi.org/10.1107/S0567739471000457}, - journal = {Acta Crystallographica Section A}, - owner = {kohlbrecher}, - timestamp = {2010.05.07} -} - -@ARTICLE{Damaschun1969, - author = {G. Damaschun and H.-V. Porschel and G. Sommer}, - title = {{Bestimmung der Gestalt gel\"oster Makromolek\"ule aus R\"ontgen-Kleinwinkeldiagrammen - mit Hilfe von Gleichungssystemen}}, - year = {1969}, - volume = {A25}, - pages = {708}, - journal = {Acta Cryst.}, - owner = {Kohlbrecher}, - timestamp = {2009.03.20} -} - -@ARTICLE{DaoudCotton82, - author = {M. Daoud and J.P. Cotton}, - title = {Star shaped polymers - A model for the conformation and its concentration-dependence}, - year = {1982}, - volume = {43}, - pages = {531}, - journal = {Journal de Physique (Paris)}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{David1986, - author = {W. I. F. David}, - title = {Powder diffraction peak shapes. Parameterization of the pseudo-Voigt - as a Voigt function}, - year = {1986}, - volume = {19}, - number = {1}, - month = {Feb}, - pages = {63-64}, - doi = {doi:10.1107/S0021889886089999}, - url = {http://dx.doi.org/10.1107/S0021889886089999}, - abstract = {The Voigt function is now recognized to be one of the best mathematical - descriptions of the symmetrical component of the peak shape in constant-wavelength - X-ray and neutron powder diffraction. The simpler pseudo-Voigt function - has been used previously to provide an empirical fit to observed - peak shapes. In this paper, a parameterization of this function is - obtained to make it, to a very good approximation, equivalent to - a Voigt function, and, additionally, it is described by the half-width - parameters of the Gaussian and Lorentzian components of that Voigt - function. This new construction allows for greater flexibility in - peak-shape description and, in particular, allows for a more straightforward - convolution of additional functional contributions into the `Voigt' - component of a peak shape description.}, - journal = {Journal of Applied Crystallography}, - owner = {Kohlbrecher}, - timestamp = {2008.11.21} -} - -@ARTICLE{Debye1947, - author = {P. Debye}, - title = {Mollecular-weight determination by Light Scattering}, - year = {1947}, - volume = {51}, - pages = {18-32}, - journal = {Journal of Physical and Colloid Chemistry}, - owner = {Kohlbrecher}, - timestamp = {2009.04.13} -} - -@ARTICLE{scatt186, - author = {P. Debye}, - title = {{\"Uber die Zerstreuung von R\"ontgenstrahlen an amorphen K\"orpern}}, - year = {1927}, - volume = {28}, - pages = {135-141}, - journal = {Physik. Z.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{DAB1957, - author = {Debye, P. and Anderson, H. R. and Brumberger, H.}, - title = {Scattering by an Inhomogeneous Solid. II. The Correlation Function - and Its Application}, - year = {1957}, - volume = {28}, - number = {6}, - pages = {679-683}, - doi = {http://dx.doi.org/10.1063/1.1722830}, - url = {http://scitation.aip.org/content/aip/journal/jap/28/6/10.1063/1.1722830}, - journal = {Journal of Applied Physics}, - owner = {kohlbrecher}, - timestamp = {2015.04.24} -} - -@ARTICLE{DebyeBueche1949, - author = {Debye, P. and Bueche, A. M.}, - title = {Scattering by an Inhomogeneous Solid}, - year = {1949}, - volume = {20}, - number = {6}, - pages = {518-525}, - doi = {http://dx.doi.org/10.1063/1.1698419}, - url = {http://scitation.aip.org/content/aip/journal/jap/20/6/10.1063/1.1698419}, - journal = {Journal of Applied Physics}, - owner = {kohlbrecher}, - timestamp = {2015.04.24} -} - -@ARTICLE{dozier91, - author = {W. D. Dozier and J. S. Huang and L. J. Fetters}, - title = {Colloidal nature of star polymer dilute and semidilute solutions}, - year = {1991}, - volume = {24}, - number = {10}, - pages = {2810-2814}, - journal = {Macromolecules}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Duh1995, - author = {Duh, Der-Ming and Haymet, A. D. J.}, - title = {Integral equation theory for uncharged liquids: The Lennard-Jones - fluid and the bridge function}, - year = {1995}, - volume = {103}, - number = {7}, - pages = {2625-2633}, - doi = {http://dx.doi.org/10.1063/1.470724}, - url = {http://scitation.aip.org/content/aip/journal/jcp/103/7/10.1063/1.470724}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.08} -} - -@ARTICLE{Dzubiella2001, - author = {Dzubiella, J. and Jusufi, A. and Likos, C. N. and von Ferber, C. - and L\"owen, H. and Stellbrink, J. and Allgaier, J. and Richter, - D. and Schofield, A. B. and Smith, P. A. and Poon, W. C. K. and Pusey, - P. N.}, - title = {Phase separation in star-polymer\char21{}colloid mixtures}, - year = {2001}, - volume = {64}, - issue = {1}, - month = {Jun}, - pages = {010401}, - doi = {10.1103/PhysRevE.64.010401}, - url = {http://link.aps.org/doi/10.1103/PhysRevE.64.010401}, - journal = {Phys. Rev. E}, - numpages = {4}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2013.11.19} -} - -@Article{Forster2010, - author = {F{\"{o}}rster, S. and Apostol, L. and Bras, W.}, - title = {{Scatter: software for the analysis of nano- and mesoscale small-angle scattering}}, - journal = {Journal of Applied Crystallography}, - year = {2010}, - volume = {43}, - number = {3}, - month = {Jun}, - pages = {639--646}, - doi = {10.1107/S0021889810008289}, - url = {http://dx.doi.org/10.1107/S0021889810008289}, - abstract = {{\it Scatter} is a new software for analysis, modeling and fitting - of one- and two-dimensional small-angle scattering data of non-ordered, - partially ordered or fully ordered nano- and mesoscale structures. - The calculations are based on closed analytical expressions for the - scattering intensity, enabling efficient evaluation of form factors - and structure factors. The software allows one to sequentially fit - large series of scattering curves and scattering patterns automatically. - It provides further tools for data loading, beam centering, calibration, - zooming, binning, lattice identification, calculation of density - profiles and size distributions, and visualization of real-space - structures. Presentations of experimental and calculated data can - be saved as is for presentations or exported for further graphical - or mathematical treatment.}, - keywords = {small-angle scattering, SAS, computer programs}, - owner = {kohlbrecher}, - timestamp = {2016.02.12}, -} - -@Article{Forster2005, - author = {S. F\"orster and A. Timmann and M. Konrad and C. Schellbach and A. Meyer and S. S. Funari and P. Mulvaney and R. Knott}, - title = {Scattering Curves of Ordered Mesoscopic Materials}, - year = {2005}, - journal = {The Journal of Physical Chemistry B}, - volume = {109}, - number = {4}, - pages = {1347-1360}, - note = {PMID: 16851102}, - doi = {10.1021/jp0467494}, - eprint = { http://dx.doi.org/10.1021/jp0467494 }, - url = { http://dx.doi.org/10.1021/jp0467494 -}, - abstract = { Analytical expressions for the scattering functions of ordered mesoscopic - materials are derived and compared to experimentally determined scattering - curves. Ordered structures comprising spheres (fcc, bcc, hcp, sc), - cylinders (hex, sq), and lamellar structures are considered. The - expressions take into account particle size distributions and lattice - point deviations, domain size, core/shell structures, as well as - peak shapes varying analytically between Lorentzian and Gaussian - functions. The expressions allow one to quantitatively describe high-resolution - synchrotron small-angle X-ray (SAXS) and neutron scattering (SANS) - curves from lipid and block copolymer lyotropic phases, core/shell - nanoparticle superstructures, ordered nanocomposites, and ordered - mesoporous materials. In addition, the diffuse out-of-plane scattering - of grazing incidence GISAXS and GISANS experiments of laterally ordered - thin films can be quantitatively analyzed. }, - owner = {kohlbrecher}, - timestamp = {2016.02.12}, -} - -@ARTICLE{Forster1998, - author = {Stephan F\"orster and and Christian Burger}, - title = {Scattering Functions of Polymeric Core-Shell Structures and Excluded - Volume Chains}, - year = {1998}, - volume = {31}, - number = {3}, - pages = {879-891}, - doi = {10.1021/ma970761v}, - eprint = { http://dx.doi.org/10.1021/ma970761v }, - url = {http://dx.doi.org/10.1021/ma970761v}, - journal = {Macromolecules}, - owner = {kohlbrecher}, - timestamp = {2016.02.14} -} - -@ARTICLE{Forster2011, - author = {S. F\"orster and S. Fischer and K. Zielske and C. Schellbach and - M. Sztucki and P. Lindner and J. Perlich}, - title = {Calculation of scattering-patterns of ordered nano- and mesoscale - materials }, - year = {2011}, - volume = {163}, - number = {1}, - pages = {53 - 83}, - issn = {0001-8686}, - doi = {http://dx.doi.org/10.1016/j.cis.2010.12.003}, - url = {http://www.sciencedirect.com/science/article/pii/S0001868611000029}, - abstract = {Analytical expressions for the scattering patterns of ordered nano- - and mesoscopic materials are derived and compared to measured scattering - patterns. Ordered structures comprising spheres (fcc, bcc, hcp, sc, - and bct), cylinders (hex and sq), lamellae (lam) and vesicles, as - well as bicontinuous cubic structures (Ia3d, Pn3m, and Im3m) are - considered. The expressions take into account unit cell dimensions, - particle sizes and size distributions, lattice point deviations, - finite domain sizes, orientational distributions, core/shell-structures - as well a variety of peak shapes. The expressions allow to quantitatively - describe, model and even fit measured \{SAXS\} and SANS-patterns - of ordered or oriented micellar solutions, lyotropic phases, block - copolymers, colloidal solutions, nanocomposites, photonic crystals, - as well as mesoporous materials. }, - journal = {Advances in Colloid and Interface Science }, - keywords = {Scattering}, - owner = {kohlbrecher}, - timestamp = {2016.02.12} -} - -@ARTICLE{FoersterHermsdorf2002, - author = {S. F\"orster and N. Hermsdorf and C. B\"ottcher and P. Lindner}, - title = {Structure of Polyelectrolyte Block Copolymer Micelles, - - Macromolecules}, - year = {2002}, - volume = {35}, - pages = {4096-4105}, - journal = {Macromolecules}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Forster1999, - author = {S. F\"orster and N. Hermsdorf and W. Leube and H. Schnablegger and - M. Regenbrecht and S. Akari and P. - - Lindner and C. B\"ottcher}, - title = {Fusion of Charged Block - - Copolymer Micelles into Toroid Networks}, - year = {1999}, - volume = {103}, - pages = {6657-6668}, - journal = {J. Phys. Chem. B}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@BOOK{book:Feigin:Svergun, - author = {L. A. Feigin and D. I. Svergun}, - title = {Structure Analysis by Small-Angle X-ray and Neutron Scattering}, - year = {1987}, - publisher = {Plenum Press}, - file = {:http\://sans.web.psi.ch/sansstatus/SASbooks/structure_analysis_saxs_sans_feigin_svergun.pdf:PDF}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Fruhwirth2004, - author = {Fr{\"{u}}hwirth, Thomas and Fritz, Gerhard and Freiberger, Norbert - and Glatter, Otto}, - title = {{Structure and order in lamellar phases determined by small-angle - scattering}}, - year = {2004}, - volume = {37}, - number = {5}, - month = {Oct}, - pages = {703--710}, - doi = {10.1107/S0021889804012956}, - url = {http://dx.doi.org/10.1107/S0021889804012956}, - journal = {Journal of Applied Crystallography}, - owner = {kohlbrecher}, - timestamp = {2010.06.04} -} - -@ARTICLE{Fratzl1994, - author = {Peter Fratzl}, - title = {Statistical model of the habit and arrangement of mineral crystals - in the collagen of bone}, - year = {1994}, - volume = {77}, - number = {1-2}, - pages = {125-143}, - doi = {10.1007/BF02186835}, - file = {:http\://sans.web.psi.ch/sansstatus/papers/generalizedGuinier/E000547671_1.pdf:PDF}, - journal = {Journal of Statistical Physics}, - owner = {kohlbrecher}, - timestamp = {2008.02.05} -} - -@ARTICLE{Freund1993, - author = {Roland W. Freund}, - title = {A Transpose-Free Quasi-Minimal Residual Algorithm for Non-Hermitian - Linear Systems}, - year = {1993}, - volume = {14}, - number = {2}, - pages = {470-482}, - doi = {10.1137/0914029}, - eprint = { http://dx.doi.org/10.1137/0914029 }, - url = { http://dx.doi.org/10.1137/0914029 -}, - journal = {SIAM Journal on Scientific Computing}, - owner = {kohlbrecher}, - timestamp = {2015.12.16} -} - -@ARTICLE{FFTW05, - author = {Frigo, Matteo and Johnson, Steven~G.}, - title = {The Design and Implementation of {FFTW3}}, - year = {2005}, - volume = {93}, - number = {2}, - pages = {216--231}, - note = {Special issue on ``Program Generation, Optimization, and Platform - Adaptation''}, - journal = {Proceedings of the IEEE}, - owner = {kohlbrecher}, - timestamp = {2013.11.02} -} - -@TECHREPORT{FFTW97, - author = {Frigo, Matteo and Johnson, Steven~G.}, - title = {The Fastest {Fourier} Transform in the West}, - institution = {Massachusetts Institute of Technology}, - year = {1997}, - number = {MIT-LCS-TR-728}, - month = {September}, - owner = {kohlbrecher}, - timestamp = {2013.11.02} -} - -@ARTICLE{Furukawa1984, - author = {H. Furukawa}, - title = {Dynamics-scaling theory for phase-separating unmixing mixtures: Growth - rates of droplets and scaling properties of autocorrelation functions}, - year = {1984}, - volume = {123}, - pages = {497}, - doi = {10.1016/0378-4371(84)90168-7}, - journal = {Physica A}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Gursoy2014, - author = {{G{\"u}rsoy}, F. and {Karakaya}, V.}, - title = {{A Picard-S hybrid type iteration method for solving a differential - equation with retarded argument}}, - year = {2014}, - month = mar, - eprint = {1403.2546}, - adsnote = {Provided by the SAO/NASA Astrophysics Data System}, - adsurl = {http://adsabs.harvard.edu/abs/2014arXiv1403.2546G}, - archiveprefix = {arXiv}, - journal = {ArXiv e-prints}, - keywords = {Mathematics - Functional Analysis, 47H06, 54H25, 34L05}, - owner = {kohlbrecher}, - primaryclass = {math.FA}, - timestamp = {2014.06.09} -} - -@ARTICLE{Gazzillo1999, - author = {Domenico Gazzillo and Achille Giacometti and Raffaele Guido Della - Valle and Elisabetta Venuti and Flavio Carsughi}, - title = {A scaling approximation for structure factors in the integral equation - theory of polydisperse nonionic colloidal fluids}, - year = {1999}, - volume = {111}, - number = {16}, - pages = {7636-7645}, - doi = {10.1063/1.480089}, - url = {http://link.aip.org/link/?JCP/111/7636/1}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2008.01.25} -} - -@ARTICLE{Gillan1979, - author = {Gillan, M.J.}, - title = {A new method of solving the liquid structure integral equations}, - year = {1979}, - volume = {38}, - number = {6}, - pages = {1781-1794}, - doi = {10.1080/00268977900102861}, - eprint = {http://www.tandfonline.com/doi/pdf/10.1080/00268977900102861}, - url = {http://www.tandfonline.com/doi/abs/10.1080/00268977900102861}, - abstract = {We present a new method of obtaining numerical solutions to the Percus-Yevick - and hypernetted chain equations for liquid structure. The method, - which is rapidly convergent and very stable, is a hybrid of the traditional - iterative scheme and the Newton-Raphson technique. We show by numerical - tests for typical potentials that the method gives well-converged - solutions in 20 or 30 iterations even for very high densities. The - number of iterations needed is insensitive to the choice of initial - estimate, even if this is extremely inaccurate.}, - journal = {Molecular Physics}, - owner = {kohlbrecher}, - timestamp = {2013.12.03} -} - -@ARTICLE{scatt75, - author = {O. Glatter}, - title = {Data evaluation in small angle scattering: Calculation of the radial - electron density distribution by means of indirect {Fourier} transformation}, - year = {1977}, - volume = {47}, - pages = {83-102}, - journal = {Acta Physica Austriaca}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Greschner1973, - author = {Georg S. Greschner}, - title = {Mathematical properties of polydisperse systems, 2. Application to - light scattering}, - year = {1973}, - volume = {170}, - number = {1}, - pages = {203-229}, - doi = {10.1002/macp.1973.021700117}, - url = {http://dx.doi.org/10.1002/macp.1973.021700117}, - abstract = {The direct and the inverse problem of the light scattering from dilute - polymer solutions is solved for GAUssian coils at the theta point. - Theoretical scattering functions and their derivatives are analytically - calculated for the general gamma distribution of molecular weights - as a function of the non-uniformity and the weight average molecular - weight, and also for various ratios of the statistical segment length - of the coil to the wave length of the scattered light. The asymptote - and the tangent of P-1Theta are obtained by analysing the operator - in the ZIMM equation and their mutual position is compared in the - angle range 150° to 180°. The scattering envelopes of microgel systems - are analytically calculated and discussed. In order to obtain the - molecular weight distribution (MWD) from a given ZIMM diagram of - GAUssian coils at the theta point, the corresponding inverse problem - is solved analytically, the necessary zero approximation of the segment - length being taken from viscometric measurements. With the help of - the presented method the MWD and the correct statistical segment - length of the coil can theoretically be computed with any reasonable - accuracy. However, the calculation shows that for practical use extremely - high accuracy of the light scattering measurements is necessary.}, - journal = {Die Makromolekulare Chemie}, - owner = {Kohlbrecher}, - timestamp = {2009.04.13} -} - -@BOOK{Guinier1963, - author = {A. Guinier}, - title = {X-ray Diffraction}, - year = {1963}, - publisher = {San Francisco: Freeman}, - owner = {kohlbrecher}, - timestamp = {2010.06.04} -} - -@BOOK{book:Guinier:Fournet, - author = {A. Guinier and G. Fournet}, - title = {Small-Angle Scattering of X-Rays}, - year = {1955}, - publisher = {John Wiley \& Sons, Inc.}, - file = {:http\://sans.web.psi.ch/sansstatus/SASbooks/saxs_guinier_fournet.pdf:PDF}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Hamilton1965, - author = {Hamilton, W. C.}, - title = {{Significance tests on the crystallographic {\it R} factor}}, - year = {1965}, - volume = {18}, - number = {3}, - month = {Mar}, - pages = {502--510}, - doi = {10.1107/S0365110X65001081}, - url = {http://dx.doi.org/10.1107/S0365110X65001081}, - journal = {Acta Crystallographica}, - owner = {kohlbrecher}, - timestamp = {2013.04.26} -} - -@Electronic{Hammouda, - author = {B. Hammouda}, - editor = {B. Hammouda}, - title = {the SANS toolbox}, - url = {http://www.ncnr.nist.gov/staff/hammouda/the_SANS_toolbox.pdf}, - howpublished = {\href{http://www.ncnr.nist.gov/staff/hammouda/the\_SANS\_toolbox.pdf}{$\dots$/the\_SANS\_toolbox.pdf}}, - owner = {Kohlbrecher}, - timestamp = {2009.04.13}, -} - -@ARTICLE{Hammouda2012, - author = {Hammouda, Boualem}, - title = {Small-Angle Scattering From Branched Polymers}, - year = {2012}, - volume = {21}, - number = {6}, - pages = {372--381}, - issn = {1521-3919}, - doi = {10.1002/mats.201100111}, - url = {http://dx.doi.org/10.1002/mats.201100111}, - abstract = {The single-polymer form factor is determined for branched polymers - using a scaling argument in order to recover the low-Q Porod exponent - characteristic of the overall structure. The high-Q Porod exponent - characterizes the local branching structure. An alternative approach - based on a high-Q expansion contains information about functionality, - branch length and branch content. The specific case of a starburst - dendrimer for which the form factor is known is discussed. The model - predictions are compared to small-angle neutron scattering data from - a dilute solution of dendrimer in D2O.}, - journal = {Macromolecular Theory and Simulations}, - keywords = {branched polymers, dendrimers, small-angle scattering, structure, - Zimm plot}, - owner = {kohlbrecher}, - publisher = {WILEY-VCH Verlag}, - timestamp = {2014.12.06} -} - -@ARTICLE{Hammouda2010, - author = {Hammouda, Boualem}, - title = {{A new Guinier{--}Porod model}}, - year = {2010}, - volume = {43}, - number = {4}, - month = {Aug}, - pages = {716--719}, - doi = {10.1107/S0021889810015773}, - url = {http://dx.doi.org/10.1107/S0021889810015773}, - abstract = {Small-angle scattering (SAS) curves are characterized by two main - features: the Guinier region and the Porod region. Standard linear - plots are available to fit SAS data and obtain a radius of gyration - and a Porod exponent. A new Guinier{--}Porod empirical model is introduced - to fit SAS data from spherical as well as nonspherical objects such - as rods or platelets. It also applies to shapes intermediate between - spheres and rods or between rods and platelets. The new model is - used to fit SAS data from a Pluronic solution that sequentially forms - unimers, then spherical micelles, then cylindrical micelles, then - lamellar micelles upon heating. This single model can fit structures - associated with all four phases as well as the intermediate structures.}, - journal = {Journal of Applied Crystallography}, - keywords = {Guinier model, Porod model, small-angle scattering, empirical models, - Pluronic solutions, scattering from cylinders}, - owner = {kohlbrecher}, - timestamp = {2016.01.06} -} - -@ARTICLE{Hanley2003, - author = {Hanley, H. J. M. and Muzny, C. D. and Ho, D. L. and Glinka, C. J.}, - title = {A Small-Angle Neutron Scattering Study of a Commercial Organoclay - Dispersion}, - year = {2003}, - volume = {19}, - number = {14}, - pages = {5575-5580}, - doi = {10.1021/la026342v}, - eprint = {http://pubs.acs.org/doi/pdf/10.1021/la026342v}, - url = {http://pubs.acs.org/doi/abs/10.1021/la026342v}, - abstract = { The paper explores the capacity of small angle neutron neutron scattering - (SANS) to characterize the dispersion of an exchanged clay in an - organic solvent. As an illustration, results are reported for 1% - and 2% by mass suspensions of a representative commercial complex, - known as Cloisite, C15A in toluene. C15A is prepared from montmorillonite - and the cation ditallow (a naturally occurring variant of dimethydioctodecylammonium). - For this particular example, the SANS scattered intensity data suggest - that the complex is well dispersed into clusters which consist of - a stack of between three and six ditallow-coated montmorillonite - platelets. The size of the clusters, the amount of ditallow adsorbed - on a montmorillonite platelet, and an estimate of the thickness of - the adsorbed layer are evaluated. General comments on the fitting - of SANS data obtained from a cluster composed of stacked, coated - disks are given. }, - journal = {Langmuir}, - owner = {kohlbrecher}, - timestamp = {2010.12.12} -} - -@Article{Hansen1982, - author = {Jean-Pierre Hansen and John B. Hayter}, - title = {A rescaled MSA structure factor for dilute charged colloidal dispersions}, - year = {1982}, - journal = {Molecular Physics}, - volume = {46}, - number = {3}, - pages = {651-656}, - doi = {10.1080/00268978200101471}, - eprint = { http://dx.doi.org/10.1080/00268978200101471 }, - url = { http://dx.doi.org/10.1080/00268978200101471 -}, - abstract = { The structure of a dispersion of charged colloidal particles interacting - through a screened Coulomb potential is well described at moderate - to high densities by calculating the correlations in the mean spherical - approximation (MSA). In this paper we extend the validity of the - MSA calculation to arbitrarily low densities, using a physical rescaling - argument which preserves the analytic form of the MSA solution. Our - results are in excellent agreement with other numerical calculations - and with experimental low-density light scattering data. The method - may be viewed as a generalization of Gillan's prescription for one - component plasmas to systems interacting through a Yukawa potential. - An advantage of the present prescription is that it allows a smooth - transition from strong to weak coupling, and it implies no functional - relation between the experimentally independent parameters. }, - owner = {kohlbrecher}, - timestamp = {2007.12.18}, -} - -@BOOK{Hansen2013, - author = {Jean-Pierre Hansen and Ian R. McDonald}, - title = {Theory of Simple Liquids with Applications to Soft Matter}, - year = {2013}, - edition = {Fourth}, - publisher = {Academic Press}, - owner = {kohlbrecher}, - timestamp = {2013.10.18} -} - -@Article{Hayter1981, - author = {J.B. Hayter and J. Penfold}, - title = {An analytic structure factor for macroion solutions}, - year = {1981}, - journal = {Molecular Physics}, - volume = {42}, - pages = {109-118}, - doi = {10.1080/00268978100100091}, - eprint = { http://dx.doi.org/10.1080/00268978100100091 }, - url = { http://dx.doi.org/10.1080/00268978100100091 -}, - owner = {kohlbrecher}, - timestamp = {2007.12.18}, -} - -@ARTICLE{Hayter1984, - author = {J. B. Hayter and J. Penfold}, - title = {Use of Viscous Shear Alignment - - To Study Anisotropic Micellar Structure by Small-Angle Neutron - - Scattering}, - year = {1984}, - volume = {88}, - pages = {4589-4593}, - journal = {J. Phys. Chem.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@INBOOK{Henderson2000, - author = {Douglas Henderson and Stefan Soko{\l}owski and Malgorza{\l}a Bor\'{o}wko}, - title = {Computational Methods in Surface And Colloidal Science}, - year = {2000}, - editor = {Ma{\l}gorzata Bor\'{o}wko}, - publisher = {Marcel Dekker, Inc.}, - chapter = {Integral Equations in the Theory of Simple Fluids}, - pages = {135-166}, - owner = {kohlbrecher}, - timestamp = {2013.10.18} -} - -@ARTICLE{Hindmarsh2005, - author = {Alan C. Hindmarsh and Peter N. Brown and Keith E. Grant and Steven - L. Lee and Radu Serban and Dan E. Shumaker and Carol S. Woodward}, - title = {SUNDIALS: Suite of Nonlinear and Differential/Algebraic Equation - Solvers}, - year = {2005}, - volume = {31}, - number = {3}, - month = sep, - pages = {363--396}, - issn = {0098-3500}, - doi = {10.1145/1089014.1089020}, - url = {http://doi.acm.org/10.1145/1089014.1089020}, - acmid = {1089020}, - address = {New York, NY, USA}, - issue_date = {September 2005}, - journal = {ACM Trans. Math. Softw.}, - keywords = {DAEs, ODEs, nonlinear systems, sensitivity analysis}, - numpages = {34}, - owner = {kohlbrecher}, - publisher = {ACM}, - timestamp = {2015.12.16} -} - -@BOOK{hittmair, - author = {O. Hittmair}, - title = {{Lehrbuch der Quantentheorie}}, - year = {1972}, - publisher = {Verlag Karl Thiemig}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Hjelm1995, - author = {Rex P. Hjelm and Claudio Schteingart and Alan F. Hofmann and Devinderjit - S. Sivia}, - title = {Form and Structure of Self-Assembling Particles in Monoolein-Bile - Salt Mixtures}, - year = {1995}, - volume = {99}, - pages = {16395-16406}, - url = {http://pubs.acs.org/cgi-bin/searchRedirect.cgi/jpchax/1995/99/i44/pdf/j100044a030.pdf}, - file = {:http\://sans.web.psi.ch/sansstatus/papers/generalizedGuinier/j100200a080_generalizedGuinierApprox.pdf:PDF}, - journal = {J. Phys. Chem.}, - owner = {kohlbrecher}, - timestamp = {2008.02.06} -} - -@ARTICLE{Hjelm2000, - author = {Rex P. Hjelm and Claudio D. Schteingart and Alan F. Hofmann and P. - Thiyagarajan}, - title = {Structure of Conjugated Bile Salt-Fatty Acid-Monoglyceride Mixed - Colloids: Studies by Small-Angle Neutron Scattering}, - year = {2000}, - volume = {104}, - pages = {197-211}, - doi = {http://dx.doi.org/10.1021/jp992157n}, - url = {http://pubs.acs.org/cgi-bin/searchRedirect.cgi/jpcbfk/2000/104/i02/pdf/jp992157n.pdf}, - file = {:http\://sans.web.psi.ch/sansstatus/papers/generalizedGuinier/jp992157n_generalizedGuinierApprox.pdf:PDF}, - journal = {J. Phys. Chem. B}, - owner = {kohlbrecher}, - timestamp = {2008.02.05} -} - -@ARTICLE{Hjelm1992, - author = {Rex P. Hjelm and P. Thiyagarajan and Hayat Alkan-Onyuksel}, - title = {Organization of Phosphatidylcholine and Bile Salt in Rodlike Mixed - Micelles}, - year = {1992}, - volume = {96}, - pages = {8653-8661}, - url = {http://pubs.acs.org/cgi-bin/searchRedirect.cgi/jpchax/1992/96/i21/pdf/j100200a080.pdf}, - file = {:http\://sans.web.psi.ch/sansstatus/papers/generalizedGuinier/j100200a080_generalizedGuinierApprox.pdf:PDF}, - journal = {J. Phys. Chem}, - owner = {kohlbrecher}, - timestamp = {2008.02.05} -} - -@ARTICLE{Homeier1995, - author = {Herbert H.H Homeier and Sebastian Rast and Hartmut Krienke}, - title = {Iterative solution of the Ornstein-Zernike equation with various - closures using vector extrapolation }, - year = {1995}, - volume = {92}, - number = {2–3}, - pages = {188 - 202}, - issn = {0010-4655}, - doi = {http://dx.doi.org/10.1016/0010-4655(95)00116-0}, - url = {http://www.sciencedirect.com/science/article/pii/0010465595001160}, - abstract = {The solution of the Ornstein-Zernike equation with various closure - approximations is studied. This problem is rewritten as an integral - equation that can be solved iteratively on a grid. The convergence - of the fixed point iterations is relatively slow. We consider transformations - of the sequence of solution vectors using non-linear sequence transformations, - so-called vector extrapolation processes. An example is the vector - J transformation. The transformed vector sequences turn out to converge - considerably faster than the original sequences. }, - journal = {Computer Physics Communications }, - keywords = {Many-particle theory}, - owner = {kohlbrecher}, - timestamp = {2013.11.05} -} - -@ARTICLE{Homeier1995a, - author = {Herbert H.H Homeier and Sebastian Rast and Hartmut Krienke}, - title = {Iterative solution of the Ornstein-Zernike equation with various - closures using vector extrapolation}, - year = {1995}, - volume = {92}, - number = {2–3}, - pages = {188 - 202}, - issn = {0010-4655}, - doi = {http://dx.doi.org/10.1016/0010-4655(95)00116-0}, - url = {http://www.sciencedirect.com/science/article/pii/0010465595001160}, - abstract = {The solution of the Ornstein-Zernike equation with various closure - approximations is studied. This problem is rewritten as an integral - equation that can be solved iteratively on a grid. The convergence - of the fixed point iterations is relatively slow. We consider transformations - of the sequence of solution vectors using non-linear sequence transformations, - so-called vector extrapolation processes. An example is the vector - J transformation. The transformed vector sequences turn out to converge - considerably faster than the original sequences. }, - journal = {Computer Physics Communications }, - keywords = {Many-particle theory}, - owner = {kohlbrecher}, - timestamp = {2013.12.03} -} - -@BOOK{Hosemann1962, - author = {R. Hosemann and S.N. Bagchi}, - title = {Direct Analysis of Diffraction by Matter}, - year = {1962}, - publisher = {Amsterdam: North-Holland.}, - owner = {kohlbrecher}, - timestamp = {2010.06.04} -} - -@BOOK{Hulst1957, - author = {H.C. van de Hulst}, - title = {Light Scattering by Small Particles}, - year = {1957}, - publisher = {Wiley, New York}, - pages = {70ff}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Hurd1988, - author = {A.J. Hurd and W.L. Flower}, - title = {In Situ Growth and Structure of Fractal Silica Aggregates in a Flame}, - year = {1988}, - volume = {122}, - number = {1}, - pages = {178-192}, - journal = {Journal of Colloid and Interface Science}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Ida2000, - author = {T. Ida and M. Ando and H. Toraya}, - title = {Extended pseudo-Voigt function for approximating the Voigt profile}, - year = {2000}, - volume = {33}, - number = {6}, - month = {Dec}, - pages = {1311-1316}, - doi = {doi:10.1107/S0021889800010219}, - url = {http://dx.doi.org/10.1107/S0021889800010219}, - journal = {Journal of Applied Crystallography}, - owner = {Kohlbrecher}, - timestamp = {2008.11.21} -} - -@ARTICLE{Ishikawa1974, - author = {Shiro Ishikawa}, - title = {Fixed points by a new iteration method}, - year = {1974}, - volume = {44}, - pages = {147--150}, - doi = {10.1090/S0002-9939-1974-0336469-5}, - url = {http://dx.doi.org/10.1090/S0002-9939-1974-0336469-5}, - journal = {Proc. Amer. Math. Soc.}, - owner = {Kohlbrecher}, - timestamp = {2014.06.09} -} - -@ARTICLE{J.Moller1995, - author = {J. M\"oller, R. Kranold, J. Schmelzer and U. Lembke}, - title = {Small-Angle X-ray Scattering Size Parameters and Higher Moments of - the Particle-Size Distribution Function in the Asymptotic Stage of - Ostwald Ripening}, - year = {1995}, - volume = {28}, - pages = {553-560}, - journal = {J Appl. Cryst.}, - owner = {Kohlbrecher}, - timestamp = {2009.03.20} -} - -@ARTICLE{Jones1924, - author = {Jones, J. E.}, - title = {On the Determination of Molecular Fields. II. From the Equation of - State of a Gas}, - year = {1924}, - volume = {106}, - number = {738}, - pages = {463-477}, - doi = {10.1098/rspa.1924.0082}, - eprint = {http://rspa.royalsocietypublishing.org/content/106/738/463.full.pdf+html}, - url = {http://rspa.royalsocietypublishing.org/content/106/738/463.short}, - journal = {Proceedings of the Royal Society of London. Series A}, - owner = {kohlbrecher}, - timestamp = {2013.11.09} -} - -@ARTICLE{Jusufi2001, - author = {A Jusufi and J Dzubiella and C N Likos and C von Ferber and H Löwen}, - title = {Effective interactions between star polymers and colloidal particles}, - year = {2001}, - volume = {13}, - number = {28}, - pages = {6177}, - url = {http://stacks.iop.org/0953-8984/13/i=28/a=303}, - abstract = {Using monomer-resolved molecular dynamics simulations and theoretical - arguments based on the radial dependence of the osmotic pressure - in the interior of a star, we systematically investigate the effective - interactions between hard, colloidal particles and star polymers - in a good solvent. The relevant parameters are the size ratio q between - the stars and the colloids, as well as the number of polymeric arms - f (functionality) attached to the common centre of the star. By covering - a wide range of q 's ranging from zero (star against a flat wall) - up to about 0.75, we establish analytical forms for the star-colloid - interaction which are in excellent agreement with simulation results. - A modified expression for the star-star interaction for low functionalities, - f ##IMG## [http://ej.iop.org/icons/Entities/lesssim.gif] {lesssim} - 10 is also introduced.}, - journal = {Journal of Physics: Condensed Matter}, - owner = {kohlbrecher}, - timestamp = {2013.11.19} -} - -@ARTICLE{Karahan2013, - author = {Ibrahim Karahan and Murat Ozdemir}, - title = {A general iterative method for approximation of fixed points and - their applications}, - year = {2013}, - volume = {3}, - number = {3}, - pages = {510--526}, - url = {http://scik.org/index.php/afpt/article/view/1100/527}, - journal = {Advances in Fixed Point Theory}, - owner = {Kohlbrecher}, - timestamp = {2014.06.09} -} - -@ARTICLE{Karahan2013a, - author = {Karahan, Ibrahim and Ozdemir, Murat}, - title = {Fixed point problems of the Picard-Mann hybrid iterative process - for continuous functions on an arbitrary interval}, - year = {2013}, - volume = {2013}, - number = {1}, - pages = {244}, - issn = {1687-1812}, - doi = {10.1186/1687-1812-2013-244}, - url = {http://www.fixedpointtheoryandapplications.com/content/2013/1/244}, - abstract = {In this paper, we consider the iteration method called 'Picard-Mann - hybrid iterative process' for finding a fixed point of continuous - functions on an arbitrary interval. We give a necessary and sufficient - condition for convergence of this iteration for continuous functions - on an arbitrary interval. Also, we compare the rate of convergence - of the Picard-Mann hybrid iteration with the other iterations and - prove that it is better than the others under the same computational - cost. Moreover, we present numerical examples.MSC: 26A18, 47H10, - 54C05.}, - journal = {Fixed Point Theory and Applications}, - owner = {kohlbrecher}, - timestamp = {2014.06.10} -} - -@ARTICLE{Kawaguchi2001, - author = {Takeshi Kawaguchi}, - title = {Radii of gyration and scattering - - functions of a torus and its derivatives}, - year = {2001}, - volume = {34}, - pages = {580-584}, - journal = {J. Appl. Cryst.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Kaya:aj5008, - author = {Kaya, H{\aa}kon}, - title = {{Scattering from cylinders with globular end-caps}}, - year = {2004}, - volume = {37}, - number = {2}, - month = {Apr}, - pages = {223--230}, - doi = {10.1107/S0021889804000020}, - url = {http://dx.doi.org/10.1107/S0021889804000020}, - journal = {Journal of Applied Crystallography}, - owner = {Kohlbrecher}, - timestamp = {2009.02.09} -} - -@ARTICLE{Kaya:aj5016, - author = {Kaya, H{\aa}kon and de Souza, Nicolas-Rapha{\"{e}}l}, - title = {{Scattering from capped cylinders. Addendum}}, - year = {2004}, - volume = {37}, - number = {3}, - month = {Jun}, - pages = {508--509}, - doi = {10.1107/S0021889804005709}, - url = {http://dx.doi.org/10.1107/S0021889804005709}, - journal = {Journal of Applied Crystallography}, - owner = {Kohlbrecher}, - timestamp = {2009.02.09} -} - -@ARTICLE{Kelley2004, - author = {C.T. Kelley and B.Montgomery Pettitt}, - title = {A fast solver for the Ornstein–Zernike equations}, - year = {2004}, - volume = {197}, - number = {2}, - pages = {491 - 501}, - issn = {0021-9991}, - doi = {http://dx.doi.org/10.1016/j.jcp.2003.12.006}, - url = {http://www.sciencedirect.com/science/article/pii/S002199910300648X}, - abstract = {In this paper, we report on the design and analysis of a multilevel - method for the solution of the Ornstein–Zernike Equations and related - systems of integro-algebraic equations. Our approach is based on - an extension of the Atkinson–Brakhage method, with Newton-GMRES - used as the coarse mesh solver. We report on several numerical experiments - to illustrate the effectiveness of the method. The problems chosen - are related to simple short ranged fluids with continuous potentials. - Speedups over traditional methods for a given accuracy are reported. - The new multilevel method is roughly six times faster than Newton-GMRES - and 40 times faster than Picard.}, - journal = {Journal of Computational Physics }, - owner = {kohlbrecher}, - timestamp = {2013.12.03} -} - -@BOOK{doi:10.1137/1.9780898718898, - author = {C. T. Kelley}, - title = {Solving Nonlinear Equations with Newton's Method}, - year = {2003}, - publisher = {Society for Industrial and Applied Mathematics}, - doi = {10.1137/1.9780898718898}, - eprint = {http://epubs.siam.org/doi/pdf/10.1137/1.9780898718898}, - url = {http://epubs.siam.org/doi/abs/10.1137/1.9780898718898}, - owner = {kohlbrecher}, - timestamp = {2013.12.03} -} - -@BOOK{Kelley2003, - author = {C. T. Kelley}, - title = {Solving Nonlinear Equations with Newton's Method}, - year = {2003}, - publisher = {SIAM, Philadelphia}, - owner = {kohlbrecher}, - timestamp = {2015.12.16} -} - -@ARTICLE{Khan2013, - author = {Khan, Safeer}, - title = {A Picard-Mann hybrid iterative process}, - year = {2013}, - volume = {2013}, - number = {1}, - pages = {69}, - issn = {1687-1812}, - doi = {10.1186/1687-1812-2013-69}, - url = {http://www.fixedpointtheoryandapplications.com/content/2013/1/69}, - abstract = {We introduce a new iterative process which can be seen as a hybrid - of Picard and Mann iterative processes. We show that the new process - converges faster than all of Picard, Mann and Ishikawa iterative - processes in the sense of Berinde (Iterative Approximation of Fixed - Points, 2002) for contractions. We support our analytical proof by - a numerical example. We prove a strong convergence theorem with the - help of our process for the class of nonexpansive mappings in general - Banach spaces and apply it to get a result in uniformly convex Banach - spaces. Our weak convergence results are proved when the underlying - space satisfies Opial's condition or has Frechet differentiable norm - or its dual satisfies the Kadec-Klee property.MSC: 47H10, 54H25.}, - journal = {Fixed Point Theory and Applications}, - owner = {kohlbrecher}, - timestamp = {2014.06.10} -} - -@ARTICLE{kholodenko93, - author = {A. L. Kholodenko}, - title = {Analytical Calculation of the Scattering Function for Polymers of - Arbitrary Flexibility Using the Dirac Propagator}, - year = {1993}, - volume = {26}, - pages = {4179-4183}, - journal = {Macromolecules}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Kohlbrecher1997, - author = {J. Kohlbrecher and A. Wiedenmann and H. Wollenberger}, - title = {Magnetic coupling between the different phases in nanocrystalline - Fe-Si-B studied by small angle neutron scattering}, - year = {1997}, - volume = {104}, - number = {1}, - month = {August}, - pages = {1-4}, - doi = {10.1007/s002570050411}, - url = {http://www.springerlink.com/content/ryf4cquxpj9rkgje}, - abstract = {The magnetic coupling in the two-phase nanostructure of Fe$_{73.5}$Si$_{15.5}$B$_7$Nb$_3$Cu$_1$ - has been investigated by SANS technique. The scattering function - for partially aligned magnetic moments of ferromagnetic single domain - particles following the Langevin statistics of superparamagnetism - has been derived which describes the field and temperature dependency - of the SANS profiles. Above the Curie temperature of the amorphous - phase $T_ c^{am}$ the nanocrystals show superparamagnetic scattering - behaviour whereas below $T_c^{am}$ they interact by magnetostatic - forces only and not by exchange coupling via the amorphous matrix.}, - journal = {Zeitschrift für Physik B Condensed Matter}, - owner = {kohlbrecher}, - timestamp = {2008.02.10} -} - -@ARTICLE{Koppel1972, - author = {Dennis E. Koppel}, - title = {Analysis of Macromolecular Polydispersity in Intensity Correlation - Spectroscopy: The Method of Cumulants}, - year = {1972}, - volume = {57}, - number = {11}, - pages = {4814-4820}, - doi = {10.1063/1.1678153}, - url = {http://link.aip.org/link/?JCP/57/4814/1}, - file = {:http\://sans.web.psi.ch/sansstatus/DLS/E005665994.pdf:PDF}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2008.01.26} -} - -@ARTICLE{Kotlarchyk1983, - author = {M. Kotlarchyk and S.-H. Chen}, - title = {Analysis of small angle neutron scattering spectra from polydisperse - interacting colooids}, - year = {1983}, - volume = {79}, - number = {5}, - pages = {2461-2489}, - file = {:http\://sans.web.psi.ch/sansstatus/SQ/E001775346.pdf:PDF}, - journal = {J. Chem. Phys}, - owner = {kohlbrecher}, - timestamp = {2008.01.25} -} - -@ARTICLE{Krasnoselskij1955, - author = {M. A. Krasnoselskij}, - title = {Two remarks on the method of successive approximations, (Russian)}, - year = {1955}, - volume = {63}, - number = {1}, - pages = {123--127}, - journal = {Uspehi Mat. Nauk. 10}, - owner = {kohlbrecher}, - timestamp = {2014.06.10} -} - -@ARTICLE{Kratky194935, - author = {O. Kratky and G. Porod}, - title = {Diffuse small-angle scattering of x-rays in colloid systems}, - year = {1949}, - volume = {4}, - number = {1}, - pages = {35 - 70}, - issn = {0095-8522}, - doi = {DOI: 10.1016/0095-8522(49)90032-X}, - url = {http://www.sciencedirect.com/science/article/B759F-4CXCV60-TN/2/2f342262dbb7d1c2084706b447db7ee8}, - journal = {Journal of Colloid Science}, - owner = {kohlbrecher}, - timestamp = {2010.12.12} -} - -@ARTICLE{Kruif1989, - author = {C. G. de Kruif and P. W. Rouw and W. J. Briels and M. H. G. Duits - and A. Vrij and R. P. May}, - title = {Adhesive Hard-Sphere Colloidal Dispersions. A - - Small-Angle Neutron-Scattering Study of Stickiness and the - - Structure Factor}, - year = {1989}, - volume = {5}, - pages = {422-428}, - journal = {Langmuir}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Labik1985, - author = {Lab\'{i}k, Stanislav and Malijevsk\'{y}, Anatol and Vo\v{n}ka, Petr}, - title = {A rapidly convergent method of solving the OZ equation}, - year = {1985}, - volume = {56}, - number = {3}, - pages = {709-715}, - doi = {10.1080/00268978500102651}, - eprint = {http://www.tandfonline.com/doi/pdf/10.1080/00268978500102651}, - url = {http://www.tandfonline.com/doi/abs/10.1080/00268978500102651}, - abstract = {A new method is proposed for solving numerically the Ornstein-Zernike - equation for systems with a spherically symmetrical pair-potential. - The method is based on expansion of the function Γ(r)=r[h(r) - c(r)] - in suitable basis functions and on a combination of Newton-Raphson - and direct iterations. Tests on the PY and HNC approximations for - hard spheres and Lennard-Jones fluid have shown that the proposed - method is three to nine times as rapid as the related and so far - the most efficient method of Gillan. Other advantages besides the - speed are low sensitivity to the choice of initial estimate and a - relatively simple computational scheme.}, - journal = {Molecular Physics}, - owner = {kohlbrecher}, - timestamp = {2013.12.03} -} - -@INCOLLECTION{Lang2012, - author = {P.R. Lang and D. Vlassopoulos and W. Richtering}, - editor = {Matyjaszewski, Krzysztof and Möller, Martin }, - title = {1.12 - Polymer/Colloid Interactions and Soft Polymer Colloids }, - booktitle = {Polymer Science: A Comprehensive Reference }, - year = {2012}, - publisher = {Elsevier}, - isbn = {978-0-08-087862-1}, - pages = {315 - 338}, - doi = {http://dx.doi.org/10.1016/B978-0-444-53349-4.00007-8}, - url = {http://www.sciencedirect.com/science/article/pii/B9780444533494000078}, - abstract = {Abstract Polymer colloids are important model systems for investigating - fundamental aspects of colloid science. Traditionally rigid particles - that have rather "simple", for example, hard sphere-like or Yukawa, - interaction potentials have been employed. Such systems have been - reviewed frequently in the past. In this chapter we focus on recent - developments: depletion interaction and soft spheres. Concerning - the latter topic, two different types of materials are discussed: - star polymers and responsive microgels.}, - address = {Amsterdam}, - keywords = {Colloidal crystal}, - owner = {kohlbrecher}, - timestamp = {2013.11.21} -} - -@ARTICLE{Lebowitz1966, - author = {Lebowitz, J. L. and Percus, J. K.}, - title = {Mean Spherical Model for Lattice Gases with Extended Hard Cores and - Continuum Fluids}, - year = {1966}, - volume = {144}, - issue = {1}, - month = {Apr}, - pages = {251--258}, - doi = {10.1103/PhysRev.144.251}, - url = {http://link.aps.org/doi/10.1103/PhysRev.144.251}, - journal = {Phys. Rev.}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2013.11.11} -} - -@ARTICLE{Lee1995, - author = {Lee, Lloyd L.}, - title = {An accurate integral equation theory for hard spheres: Role of the - zero-separation theorems in the closure relation}, - year = {1995}, - volume = {103}, - number = {21}, - pages = {9388-9396}, - doi = {http://dx.doi.org/10.1063/1.469998}, - url = {http://scitation.aip.org/content/aip/journal/jcp/103/21/10.1063/1.469998}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.28} -} - -@ARTICLE{Lee1996, - author = {Lee, Lloyd L. and Ghonasgi, Dhananjay and Lomba, Enrique}, - title = {The fluid structures for soft-sphere potentials via the zero-separation - theorems on molecular distribution functions}, - year = {1996}, - volume = {104}, - number = {20}, - pages = {8058-8067}, - doi = {http://dx.doi.org/10.1063/1.471522}, - url = {http://scitation.aip.org/content/aip/journal/jcp/104/20/10.1063/1.471522}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.29} -} - -@BOOK{Lekkerkerker2011, - author = {Henk N.W. Lekkerkerker and Remco Tuinier}, - title = {Colloids and the Depletion Interaction}, - year = {2011}, - volume = {833}, - series = {Lecture Notes in Physics}, - publisher = {Springer Netherlands}, - doi = {10.1007/978-94-007-1223-2}, - url = {http://link.springer.com/book/10.1007%2F978-94-007-1223-2}, - owner = {kohlbrecher}, - timestamp = {2013.11.20} -} - -@INBOOK{Likos2011, - author = {Christos N. Likos}, - title = {Microgel Suspensions: Fundamentals and Applications}, - booktitle = {Microgel Suspensions}, - year = {2011}, - editor = {Alberto Fernandez-Nieves Hans M. Wyss and Johan Mattsson and David - A. Weitz}, - publisher = {Wiley-VCH Verlag GmbH \& Co. KGaA}, - isbn = {9783527632992}, - chapter = {Chapter 7. Structure and Thermodynamics of Ionic Microgels}, - pages = {163--193}, - doi = {10.1002/9783527632992.ch7}, - url = {http://dx.doi.org/10.1002/9783527632992.ch7}, - abstract = {This chapter contains sections titled: * Introduction * Effective - Interparticle Potentials * The Fluid Phase of Ionic Microgels * Genetic - Algorithms for the Crystal Structures * Phase Behavior * Summary - and Concluding Remarks * References}, - keywords = {degrees of freedom, effective Hamiltonian, effective interaction potential, - electroneutrality condition, ionic microgels, phase behavior}, - owner = {kohlbrecher}, - timestamp = {2013.11.20} -} - -@ARTICLE{Likos2006, - author = {Likos, Christos N.}, - title = {Soft matter with soft particles}, - year = {2006}, - volume = {2}, - issue = {6}, - pages = {478-498}, - doi = {10.1039/B601916C}, - url = {http://dx.doi.org/10.1039/B601916C}, - abstract = {In this review we present a summary of recent progress achieved in - examining the equilibrium and dynamical properties of concentrated - solutions of two novel kinds of soft matter systems: and starburst - molecules known as . The two systems share a host of interesting - properties. The both consist of highly branched polymers{,} they - allow for tuning of their properties through modification of the - macromolecular architecture and they are both representatives of - a quite novel class of colloidal particles{,} termed . On the other - hand there are also important differences{,} reflecting the fundamental - difference in their architecture. It will be shown that a combination - of scattering techniques and rheology with computer simulations and - analytical methods from the realm of theoretical physics can shed - light on the unusual properties of such systems. In this fashion{,} - new ways appear for the manipulation of soft matter systems under - external influences and promising perspectives for the fabrication - of new materials are opened up and the versatility in manipulating - soft matter is underlined.}, - journal = {Soft Matter}, - owner = {kohlbrecher}, - publisher = {The Royal Society of Chemistry}, - timestamp = {2015.06.10} -} - -@ARTICLE{Likos2001, - author = {Christos N. Likos}, - title = {Effective interactions in soft condensed matter physics }, - year = {2001}, - volume = {348}, - number = {4–5}, - pages = {267 - 439}, - issn = {0370-1573}, - doi = {http://dx.doi.org/10.1016/S0370-1573(00)00141-1}, - url = {http://www.sciencedirect.com/science/article/pii/S0370157300001411}, - abstract = {In this work, we present a review of recently achieved progress in - the field of soft condensed matter physics, and in particular on - the study of the static properties of solutions or suspensions of - colloidal particles. The latter are macromolecular entities with - typical sizes ranging from 1 nm to 1$\mu$m and their suspension typically - contain, in addition to the solvent, smaller components such as salt - ions or free polymer chains. The theoretical tool introduced is the - effective Hamiltonian which formally results by a canonical trace - over the smaller degrees of freedom for a fixed, "frozen" configuration - of the large ones. After presenting the formal definitions of this - effective Hamiltonian, we proceed with the applications to some common - soft matter systems having a variable softness and ranging from free - polymer chains to hard colloidal particles. We begin from the extreme - case of nondiverging effective interactions between ultrasoft polymer - chains and derive an exact criterion to determine the topology of - the phase diagrams of such systems. We use star polymers with a variable - arm number f as a hybrid system in order to interpolate between these - two extremes. By deriving an effective interaction between stars - we can monitor the change in the phase behavior of a system as the - steepness of the repulsion between its constituent particles increases. - We also review recent results on the nature and the effects of short-range - attractions on the phase diagrams of spherical, nonoverlapping colloidal - particles.}, - journal = {Physics Reports}, - keywords = {Soft matter}, - owner = {kohlbrecher}, - timestamp = {2013.11.18} -} - -@ARTICLE{Likos1998, - author = {Likos, C. N. and L\"owen, H. and Watzlawek, M. and Abbas, B. and - Jucknischke, O. and Allgaier, J. and Richter, D.}, - title = {Star Polymers Viewed as Ultrasoft Colloidal Particles}, - year = {1998}, - volume = {80}, - issue = {20}, - month = {May}, - pages = {4450--4453}, - doi = {10.1103/PhysRevLett.80.4450}, - url = {http://link.aps.org/doi/10.1103/PhysRevLett.80.4450}, - journal = {Phys. Rev. Lett.}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2013.11.19} -} - -@ARTICLE{Lin1990, - author = {M.Y. Lin and H.M. Lindsay and D.A. Weitz and R.C. Ball and R. Klein - and P. Meakin}, - title = {Universal reaction-limited colloidal aggregation}, - year = {1990}, - volume = {41}, - number = {4}, - pages = {2005-2020}, - journal = {Physical Review A}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Lin1990a, - author = {M.Y. Lin and H.M. Lindsay and D.A. Weitz and R.C. Ball and R. Klein - and P. Meakin}, - title = {Universal diffusion-limited colloid aggregation}, - year = {1990}, - volume = {2}, - pages = {3093-3113}, - journal = {J. Phys.: Condens. Matter}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Lin1989, - author = {M.Y. Lin and H.M. Lindsay and D.A. Weitz and R.C. Ball and R. Klein - and P. Meakin}, - title = {Universality of Fractal Aggregates as Probed by Light Scattering}, - year = {1989}, - volume = {423}, - pages = {71-87}, - doi = {10.1098/rspa.1989.0042}, - journal = {Proc. R. Soc. Lond. A}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Liu2001, - author = {Yuyan Liu and Jieli Lin and Guangming Huang and Yuanqing Guo and - Chuanxi Duan}, - title = {Simple empirical analytical approximation to the Voigt profile}, - year = {2001}, - volume = {18}, - number = {5}, - pages = {666--672}, - doi = {10.1364/JOSAB.18.000666}, - url = {http://josab.osa.org/abstract.cfm?URI=josab-18-5-666}, - journal = {J. Opt. Soc. Am. B}, - keywords = {Spectroscopy}, - owner = {Kohlbrecher}, - timestamp = {2008.11.21} -} - -@ARTICLE{Lomba1996, - author = {Lomba, E. and Lee, L.L.}, - title = {Consistency conditions for the integral equations of liquid structures}, - year = {1996}, - volume = {17}, - number = {3}, - pages = {663-672}, - issn = {0195-928X}, - doi = {10.1007/BF01441512}, - url = {http://dx.doi.org/10.1007/BF01441512}, - language = {English}, - journal = {International Journal of Thermophysics}, - keywords = {bridge function; chemical potential; closure relation; GibbsDuhem - relation; integral equations; Lennard Jones potential; pressure consistency; - thermodynamic consistency}, - owner = {kohlbrecher}, - publisher = {Kluwer Academic Publishers-Plenum Publishers}, - timestamp = {2013.11.28} -} - -@ARTICLE{Louis2000, - author = {Louis, A. A. and Bolhuis, P. G. and Hansen, J. P.}, - title = {Mean-field fluid behavior of the Gaussian core model}, - year = {2000}, - volume = {62}, - issue = {6}, - month = {Dec}, - pages = {7961--7972}, - doi = {10.1103/PhysRevE.62.7961}, - url = {http://link.aps.org/doi/10.1103/PhysRevE.62.7961}, - journal = {Phys. Rev. E}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2013.11.20} -} - -@ARTICLE{Lyatskaya2000, - author = {Lyatskaya, Yulia and Liu, Yufeng and Tristram-Nagle, Stephanie and - Katsaras, John and Nagle, John F.}, - title = {Method for obtaining structure and interactions from oriented lipid - bilayers}, - year = {2000}, - volume = {63}, - number = {1}, - month = {Dec}, - pages = {011907}, - doi = {10.1103/PhysRevE.63.011907}, - journal = {Phys. Rev. E}, - numpages = {9}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2010.06.04} -} - -@ARTICLE{Moller1995, - author = {M{\"{o}}ller, J. and Kranold, R. and Schmelzer, J. and Lembke, U.}, - title = {{Small-Angle X-ray Scattering Size Parameters and Higher Moments - of the Particle-Size Distribution Function in the Asymptotic Stage - of Ostwald Ripening}}, - year = {1995}, - volume = {28}, - number = {5}, - month = {Oct}, - pages = {553--560}, - doi = {10.1107/S0021889895003827}, - url = {http://dx.doi.org/10.1107/S0021889895003827}, - journal = {Journal of Applied Crystallography}, - owner = {kohlbrecher}, - timestamp = {2010.05.07} -} - -@ARTICLE{MuellerDelsanti2000, - author = {F. M\"uller and M. Delsanti and L. Auvray and J. Yang and Y.J. Chen - and J.W. Mays and - - B. Demé and M. Tirrell and and P. Guenoun}, - title = {Ordering of urchin-like charged - - copolymer micelles: Electrostatic, packing and polyelectrolyte - - correlations}, - year = {2000}, - volume = {3}, - pages = {45-53}, - journal = {Eur. Phys. J. E}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Madden1980, - author = {Madden, William G. and Rice, Stuart A.}, - title = {The mean spherical approximation and effective pair potentials in - liquids}, - year = {1980}, - volume = {72}, - number = {7}, - pages = {4208-4215}, - doi = {http://dx.doi.org/10.1063/1.439651}, - url = {http://scitation.aip.org/content/aip/journal/jcp/72/7/10.1063/1.439651}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.11} -} - -@ARTICLE{Mann1953, - author = {Mann, W. Robert}, - title = {Mean value methods in iteration}, - year = {1953}, - volume = {4}, - pages = {506--510}, - doi = {10.1090/S0002-9939-1953-0054846-3}, - url = {http://www.ams.org/journals/proc/1953-004-03/S0002-9939-1953-0054846-3/}, - journal = {Proc. Amer. Math. Soc.}, - owner = {Kohlbrecher}, - timestamp = {2014.06.09} -} - -@ARTICLE{Marquest1989, - author = {C. Marquest and T.A. Witten}, - title = {Simple cubic structure in copolymer mesophases}, - year = {1989}, - volume = {50}, - number = {10}, - pages = {1267-1277}, - doi = {10.1051/jphys:0198900500100126700}, - url = {http://dx.doi.org/10.1051/jphys:0198900500100126700}, - journal = {J. Phys. France}, - owner = {kohlbrecher}, - timestamp = {2013.11.10} -} - -@ARTICLE{Martynov1999, - author = {Martynov, G. A. and Sarkisov, G. N. and Vompe, A. G.}, - title = {New closure for the Ornstein-Zernike equation}, - year = {1999}, - volume = {110}, - number = {8}, - pages = {3961-3969}, - doi = {http://dx.doi.org/10.1063/1.478276}, - url = {http://scitation.aip.org/content/aip/journal/jcp/110/8/10.1063/1.478276}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.11} -} - -@ARTICLE{Martynov1993, - author = {Martynov, G. A. and Vompe, A. G.}, - title = {Differential condition of thermodynamic consistency as a closure - for the Ornstein-Zernike equation}, - year = {1993}, - volume = {47}, - issue = {2}, - month = {Feb}, - pages = {1012--1017}, - doi = {10.1103/PhysRevE.47.1012}, - url = {http://link.aps.org/doi/10.1103/PhysRevE.47.1012}, - journal = {Phys. Rev. E}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2013.12.01} -} - -@ARTICLE{Martynov1983, - author = {Martynov, G.A. and Sarkisov, G.N.}, - title = {Exact equations and the theory of liquids. V}, - year = {1983}, - volume = {49}, - number = {6}, - pages = {1495-1504}, - doi = {10.1080/00268978300102111}, - eprint = {http://www.tandfonline.com/doi/pdf/10.1080/00268978300102111}, - url = {http://www.tandfonline.com/doi/abs/10.1080/00268978300102111}, - journal = {Molecular Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.11} -} - -@ARTICLE{Mauritz2004, - author = {Mauritz, Kenneth A. and Moore, Robert B.}, - title = {State of Understanding of Nafion}, - year = {2004}, - volume = {104}, - number = {10}, - pages = {4535-4586}, - note = {PMID: 15669162}, - doi = {10.1021/cr0207123}, - eprint = { http://dx.doi.org/10.1021/cr0207123 }, - url = { http://dx.doi.org/10.1021/cr0207123 -}, - journal = {Chemical Reviews}, - owner = {kohlbrecher}, - timestamp = {2015.02.17} -} - -@ARTICLE{Menon1991, - author = {S.V.G. Menon and V.K. Kelkar and C. Monohar}, - title = {Application of - - Baxter´s model to the theory of cloud points of nonionic - - surfactant solutions}, - year = {1991}, - volume = {43}, - number = {2}, - pages = {1130-1133}, - journal = {Physical Review A}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Menon1991a, - author = {S.V.G. Menon and C. Manobar and K. Srinivasa Rao}, - title = {A new interpretation of a sticky hard sphere model}, - year = {1991}, - volume = {95}, - number = {12}, - pages = {9186-9190}, - journal = {J. Chem. Phys.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Michels2010, - author = {Michels, Andreas}, - title = {Correlation functions of the spin misalignment in magnetic small-angle - neutron scattering}, - year = {2010}, - volume = {82}, - issue = {2}, - month = {Jul}, - pages = {024433}, - doi = {10.1103/PhysRevB.82.024433}, - url = {http://link.aps.org/doi/10.1103/PhysRevB.82.024433}, - journal = {Phys. Rev. B}, - numpages = {12}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2013.05.25} -} - -@ARTICLE{Michels2013, - author = {Michels, Andreas and Bick, Jens-Peter}, - title = {{Autocorrelation function of the spin misalignment in magnetic small-angle - neutron scattering: application to nanocrystalline metals}}, - year = {2013}, - volume = {46}, - number = {3}, - month = {Jun}, - pages = {788--790}, - doi = {10.1107/S0021889813005402}, - url = {http://dx.doi.org/10.1107/S0021889813005402}, - journal = {Journal of Applied Crystallography}, - owner = {kohlbrecher}, - timestamp = {2013.05.25} -} - -@ARTICLE{Mie1908, - author = {G. Mie}, - title = {{Beitr\"age zur Optik tr\"uber Medien, speziell kolloidaler Metall\"osungen}}, - year = {1908}, - volume = {25}, - pages = {377-455}, - journal = {Annalen der Physik}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Mladek2005, - author = {B.M. Mladek and M.J. Fernaud and G. Kahl and M. Neumann}, - title = {On the thermodynamic properties of the generalized Gaussian core - model}, - year = {2005}, - volume = {8}, - pages = {135-148}, - doi = {10.5488/CMP.8.1.135}, - url = {http://www.icmp.lviv.ua/journal/zbirnyk.41/011/abstract.html}, - journal = {Condensed Matter Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.20} -} - -@ARTICLE{scatt91, - author = {R. M. Moon and T. Riste and W. C. Koehler}, - title = {Polarization analysis of thermal-neutron scattering}, - year = {1969}, - volume = {181}, - number = {2}, - month = {May}, - pages = {920-931}, - journal = {Physical Review}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Morita1960, - author = {Morita, Tohru and Hiroike, Kazuo}, - title = {A New Approach to the Theory of Classical Fluids. I}, - year = {1960}, - volume = {23}, - number = {6}, - pages = {1003-1027}, - doi = {10.1143/PTP.23.1003}, - eprint = {http://ptp.oxfordjournals.org/content/23/6/1003.full.pdf+html}, - url = {http://ptp.oxfordjournals.org/content/23/6/1003.abstract}, - abstract = {An exact integral equation is found for the pair distribution function. - The integral equation is of somewhat different nature from the usual - ones known in the theory of classical fluids, in the point that it - involves an infinite series. The Helmholtz free energy is expressed - as a series expansion which may be more rapidly convergent than the - usual one. It is shown that the integral equation can be derived - also by means of a variational principle from the expression for - the free energy. It is pointed out that the theory of classical fluids - may be constructed with the knowledge of the pair distribution function - alone, even if a form of the pair interaction potential is not known.}, - journal = {Progress of Theoretical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.12.01} -} - -@BOOK{Naegele2004, - author = {Gerhard N\"agele}, - title = {The Physics of Colloidal Soft Matter}, - year = {2004}, - editor = {Centre of Excellence for Advanced Materials and Structures}, - series = {Lecture Notes}, - number = {14}, - publisher = {Institute of Fundamental Technological Research - Polish Academy - of Sciences}, - url = {http://hera.physik.uni-konstanz.de/igk/news/workshops/Naegele.pdf}, - address = {Warsaw}, - owner = {kohlbrecher}, - timestamp = {2013.10.18} -} - -@ARTICLE{Naegele1996, - author = {Gerhard N\"agele}, - title = {On the dynamics and structure of charge-stabilized suspensions }, - year = {1996}, - volume = {272}, - number = {5-6}, - pages = {215 - 372}, - issn = {0370-1573}, - doi = {http://dx.doi.org/10.1016/0370-1573(95)00078-X}, - url = {http://www.sciencedirect.com/science/article/pii/037015739500078X}, - abstract = {Charge-stabilized suspensions of spherically shaped particles show - a variety of interesting properties. As a consequence, there has - been considerable interest in the investigation of the microstructure - and the dynamic properties of well characterized model systems, such - as polystyrene spheres dispersed in water and charged silica spheres - dispersed in an organic solvent. Among various experimental techniques, - static and dynamic light scattering have been the major tools for - the characterization of colloidal suspensions. Whereas there is an - essentially quantitative understanding of monodisperse suspensions, - only very recently good progress was achieved, both theoretically - and experimentally, in understanding certain properties of colloidal - mixtures and intrinsically polydisperse one-component suspensions. - Colloidal mixtures show additional phenomena, e.g., a variety of - microstructures and phase behaviour, tracer-diffusion and interdiffusion, - which do not exist in monodisperse systems. This article offers a - survey on our current knowledge of the dynamics and statics of charge-stabilized - suspensions in the fluid phase, with emphasis on the authors own - work. It further contains a summary of basic concepts, and of analytical - and numerical methods, which are relevant for the theoretical description - of charge-stabilized suspensions. Special effort is made to point - out the salient differences between colloidal mixtures and monodisperse - suspensions. The calculated or computer-simulated quantities characterizing - the suspensions are compared, whenever available, with the results - of light scattering experiments. The article is divided into two - major parts. The first part (chapters 2 and 3) is concerned with - static properties. It includes a discussion of the origin of the - repulsive and attractive forces between charged colloidal particles, - the concepts of the effective charge and global correlation functions, - the influence of the finite size of the counterions on the microstructure - of concentrated ionic micellar solutions, and the extension of the - rescaled mean spherical approximation to colloidal mixtures. The - central issue of the first part is, however, the theoretical modeling - of intrinsic polydispersity, and the calculation of static structure - factors and radial distribution functions by various integral equation - methods. The relative accuracy of these methods is assessed from - the comparisons with computer simulations and light scattering results. - The main body of this article is contained in the second part (chapter - 4), which is concerned with the dynamics of charge-stabilized suspensions. - A thorough discussion of the various levels of description of the - suspension dynamics is given in terms of the time scales characterizing - various relaxation processes associated with the colloidal particles - and the molecules of the host fluid. The description of the dynamics - of the colloidal particles, based on the generalized Smoluchowski - equation, is justified for the time interval accessible in dynamic - light scattering experiments. A summary of general properties of - the generalized Smoluchowski equation is provided, and various ordering - relations for diffusion coefficients are presented. The combined - influence of the electrostatic and solvent mediated hydrodynamic - interactions on the short-time dynamics of monodisperse and polydisperse - charge-stabilized suspensions is investigated in great detail. It - is shown that the effect of hydrodynamic interaction is strongly - enhanced by the presence of long-ranged electrostatic repulsion, - and its influence is more pronounced for collective diffusion than - for short-time self-diffusion. The additional influence of polydispersity - is found to be quite significant. Finally, a thorough study of tracer-diffusion - in charge-stabilized suspensions is presented. Mean square displacements - and long-time tracer-diffusion coefficients are calculated with two - alternative approximations, i.e., a mode-coupling scheme and a single - relaxation time ansatz. The range of validity of these approximations - is assessed by numerous comparisons with Brownian dynamics simulation - results, and with large-wavenumber dynamic light scattering and forced-Rayleigh - data. It is observed that tracer-diffusion is quite sensitive to - the amount of intrinsic polydispersity.}, - journal = {Physics Reports }, - keywords = {Charge-stabilized suspensions}, - owner = {kohlbrecher}, - timestamp = {2013.11.20} -} - -@ARTICLE{Neugebauer1943, - author = {Neugebauer, Th.}, - title = {Berechnung der Lichtzerstreuung von Fadenkettenlösungen}, - year = {1943}, - volume = {434}, - number = {7-8}, - pages = {509--533}, - issn = {1521-3889}, - url = {http://dx.doi.org/10.1002/andp.19434340702}, - abstract = {Abstract 10.1002/andp.19434340702.abs Die Methode der Messung der - Deporalisation des gestreuten Lichtes zur Erforschung der Molekülstruktur - ist bei Fadenketten unbrauchbar, weil die Anisotropie von diesen - mit zunehmender Kettengliederzahl sich kaum ändert; dagegen ändert - sich aber die Intensität des gestreuten Lichtes, aus der man dem - Gang der Polymerisation oder Depolymerisation im Ablaufe folgen kann, - die dazu benötigten Formeln (58), (59) und (61) werden hergeleitet. - Gleichzeitig wird eine Methode angegeben, mit Hilfe deren man die - Frage entscheiden kann, ob die Fadenketten gerade, verbogen oder - geknäuelt sind, und außerdem, wie man die Dichte- und Orientierungsstreuung - des Lösungsmittels von der Streuung der Fadenketten trennen kann - (§ 4). Der in dieser Arbeit erhaltene „diffusometrischeâ€?ï¸? - Mittelwert des Polymerisationsgrades ist mit dem Staudingerschen - „viskosimetrischenâ€?ï¸? identisch. Für den Fall, daß die Kettenlänge - nicht mehr klein im Verhältnis zur Wellenlänge des Lichtes ist, - werden ebenfalls Formeln (92), (93) und (94) hergeleitet (§ 5), - mit Hilfe deren man noch ein Verfahren zur Entscheidung der Frage, - ob die Ketten gerade sind, erhält. Besitzen die Ketten ein starkes - Assoziationsbestreben, so werden unsere Formeln ungültig, das ist - das Gebiet des Plotnikoweffektes.}, - journal = {Ann. Phys.}, - owner = {Kohlbrecher}, - publisher = {WILEY-VCH Verlag}, - timestamp = {2011.01.17} -} - -@ARTICLE{Noor2000, - author = {Muhammad Aslam Noor}, - title = {New Approximation Schemes for General Variational Inequalities }, - year = {2000}, - volume = {251}, - number = {1}, - pages = {217 - 229}, - issn = {0022-247X}, - doi = {http://dx.doi.org/10.1006/jmaa.2000.7042}, - url = {http://www.sciencedirect.com/science/article/pii/S0022247X00970422}, - abstract = {In this paper, we suggest and consider a class of new three-step approximation - schemes for general variational inequalities. Our results include - Ishikawa and Mann iterations as special cases. We also study the - convergence criteria of these schemes. }, - journal = {Journal of Mathematical Analysis and Applications }, - keywords = {variational inequalities}, - owner = {kohlbrecher}, - timestamp = {2014.06.09} -} - -@ARTICLE{Olivero1977, - author = {J. J. Olivero and R. L. Longbothum}, - title = {Empirical fits to the Voigt line width: A brief review.}, - year = {1977}, - volume = {17}, - number = {233-236}, - pages = {12–98}, - journal = {J. Quant. Spectrosc. Radiat. Transfer}, - owner = {Kohlbrecher}, - timestamp = {2008.11.21} -} - -@ARTICLE{Ornstein1914, - author = {L.S. Ornstein and F. Zernike}, - title = {Accidental deviations of density and opalescence at the critical - point of a single substance}, - year = {1914}, - volume = {17}, - pages = {793--806}, - url = {http://www.dwc.knaw.nl/DL/publications/PU00012727.pdf}, - journal = {Koninklijke Nederlandsche Akademie van Wetenschappen Proceedings}, - owner = {kohlbrecher}, - timestamp = {2013.11.12} -} - -@ARTICLE{Oversteegen2004, - author = {Oversteegen, S.M. and Lekkerkerker, H.N.W.}, - title = {On the accuracy of the Derjaguin approximation for depletion potentials}, - year = {2004}, - volume = {341}, - number = {1-4}, - pages = {23-39}, - note = {cited By (since 1996)12}, - doi = {http://dx.doi.org/10.1016/j.physa.2004.04.103}, - url = {http://www.sciencedirect.com/science/article/pii/S037843710400528X}, - abstract = {The accuracy of the Derjaguin expressions for the depletion potential - of large spheres due to small spheres, discs, and rods is analysed. - To that end, we subdivide the generalised Gibbs adsorption equation - into three contributions. We determine these contributions both in - first order of curvature of the large spheres as well as exact for - small spheres, discs, and rods up to first order in the number density - of the depletion agents. The gain of volume in the bulk when the - depletion zones of the large spheres overlap is the same for spheres, - discs, and rods of equally characteristic sizes. The Derjaguin approximation - underestimates the exact solution because of the neglected curvature. - The number of particles that fit in the gap between the two large - spheres as well as the amount that can enter a single depletion zone, - are both underestimated by the Derjaguin approximation for discs - and rods to relatively the same extent. Due to the intermediate excluded - volume of the discs, the correction of the last two contributions - just cancels the error in the first one. Small spheres only exhibit - the first contribution, whereas for rods the other parts overcompensate - the first. We can thus explain why the depletion potential of large - spheres due to small spheres is underestimated by the Derjaguin approximation, - is surprisingly accurate for discs, and is overestimated for rod-like - depletion agents.s}, - affiliation = {Van't Hoff Lab. Phys./Colloid Chem., Debye Research Institute, Utrecht - University, P.O. Box 80051, 3508 TB Utrecht, Netherlands}, - author_keywords = {Colloids; Depletion interaction}, - document_type = {Article}, - journal = {Physica A: Statistical Mechanics and its Applications}, - keywords = {Depletion interaction}, - owner = {kohlbrecher}, - source = {Scopus}, - timestamp = {2013.11.20} -} - -@ARTICLE{Pabst2003, - author = {G. Pabst and R. Koschuch and B. Pozo-Navas and M. Rappolt and K. - Lohner and P. Laggner}, - title = {Structural analysis of weakly ordered membrane stacks}, - year = {2003}, - volume = {36}, - number = {6}, - month = {Dec}, - pages = {1378-1388}, - doi = {10.1107/S0021889803017527}, - url = {http://dx.doi.org/10.1107/S0021889803017527}, - abstract = {The applicability of full-q-range models to fit low-resolution X-ray - diffraction data from multibilayers exhibiting only weak quasi-Bragg - peak scattering has been analysed. The models consider different - structure factors, accounting for different types of lattice disorder - caused by stacking faults or bending fluctuations. Numerical tests - of the models, considering instrumental influence of a line-focus - collimation system, demonstrated that Bragg peak line shapes given - by different lattice disorders cannot be discerned. However, line-shape - parameters can be determined for a particular sample, if the type - of disorder is known a priori. This has been verified by comparing - the experimental results for the fluctuation parameter of palmitoyl-oleoyl - phosphatidylcholine (POPC) as a function of temperature with high-resolution - data on the same lipid. Tests further show that the calculation of - structural parameters, such as the membrane thickness or the extent - of the interbilayer water region, is not obscured by the smearing - imposed by the instrument. The model was further applied successfully - to experimental data of lipid mixtures composed of sphingomyelin - (SM)/POPC/cholesterol and dipalmitoyl phosphatidylethanolamine (DPPE)/dipalmitoyl - phosphatidylglycerol (DPPG). The structural parameters determined - give valuable insight into the physical state of the membrane system, - which is not accessible when quasi-Bragg reflections only are considered.}, - journal = {Journal of Applied Crystallography}, - keywords = {biological model membranes; liquid crystals; diffuse scattering; instrumental - resolution; data modelling.}, - owner = {kohlbrecher}, - timestamp = {2010.06.04} -} - -@ARTICLE{Pabst2000, - author = {Pabst, Georg and Rappolt, Michael and Amenitsch, Heinz and Laggner, - Peter}, - title = {Structural information from multilamellar liposomes at full hydration: - Full \textit{q} -range fitting with high quality x-ray data}, - year = {2000}, - volume = {62}, - issue = {3}, - month = {Sep}, - pages = {4000--4009}, - doi = {10.1103/PhysRevE.62.4000}, - url = {http://link.aps.org/doi/10.1103/PhysRevE.62.4000}, - journal = {Phys. Rev. E}, - owner = {Kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2012.03.27} -} - -@ARTICLE{Pedersen1994, - author = {.S. Pedersen}, - title = {Determination of size distributions from small-angle scattering data - for systems with effective hard-sphere interactions}, - year = {1994}, - volume = {27}, - pages = {595-608}, - file = {:http\://sans.web.psi.ch/sansstatus/SQ/gl0327.pdf:PDF}, - journal = {J. Appl. Cryst.}, - owner = {kohlbrecher}, - timestamp = {2008.01.25} -} - -@ARTICLE{PedersenJApplCryst2000, - author = {J.S. Pedersen}, - title = {Form factors of block copolymer micelles with spherical, ellipsoidal - and cylindrical cores}, - year = {2000}, - volume = {33}, - number = {3 Part 1}, - month = {Jun}, - pages = {637-640}, - doi = {10.1107/S0021889899012248}, - url = {http://dx.doi.org/10.1107/S0021889899012248}, - journal = {Journal of Applied Crystallography}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@INBOOK{Pedersen2002, - author = {Jan Skov Pedersen}, - title = {Neutrons, X-Rays and Light}, - year = {2002}, - editor = {P. Lindner and Th. Zemb}, - publisher = {Elsevier Science}, - chapter = {Modelling of Small-Angle Scattering Data from Colloids and Polymer - Systems}, - pages = {391-420}, - owner = {Kohlbrecher}, - timestamp = {2009.04.13} -} - -@ARTICLE{pedersen:2839, - author = {Jan Skov Pedersen}, - title = {Structure factors effects in small-angle scattering from block copolymer - micelles and star polymers}, - year = {2001}, - volume = {114}, - number = {6}, - pages = {2839-2846}, - doi = {10.1063/1.1339221}, - url = {http://link.aip.org/link/?JCP/114/2839/1}, - journal = {The Journal of Chemical Physics}, - keywords = {polymers; polymer blends; colloids; liquid structure; polymer structure; - Monte Carlo methods; digital simulation}, - owner = {Kohlbrecher}, - publisher = {AIP}, - timestamp = {2012.03.30} -} - -@ARTICLE{Pedersen1997, - author = {Jan Skov Pedersen}, - title = {Analysis of small-angle scattering data from colloids and polymer - solutions: modeling and least-squares fitting}, - year = {1997}, - volume = {70}, - number = {0}, - pages = {171 - 210}, - issn = {0001-8686}, - doi = {10.1016/S0001-8686(97)00312-6}, - url = {http://www.sciencedirect.com/science/article/pii/S0001868697003126}, - abstract = {Analysis and modeling of small-angle scattering data from systems - consisting of colloidal particles or polymers in solution are discussed. - The analysis requires application of least-squares methods, and the - basic principles of linear and non-linear leastsquares methods are - summarized with emphasis on applications in the analysis of small-angle - scattering data. These include indirect Fourier transformation, square-root - deconvolution, size distribution determinations, and modeling. The - inclusion of corrections for instrumental smearing effects is also - discussed. The most common analytical expressions for model form - factors and structure factors are summarized. An example of analysis - of small-angle neutron and X-ray scattering data from block copolymer - micelles is given.}, - journal = {Advances in Colloid and Interface Science}, - owner = {Kohlbrecher}, - timestamp = {2012.03.30} -} - -@ARTICLE{PedersenGerstenberg96, - author = {Pedersen, Jan Skov and Gerstenberg, Michael C.}, - title = {Scattering Form Factor of Block Copolymer Micelles}, - year = {1996}, - volume = {29}, - number = {4}, - pages = {1363-1365}, - doi = {10.1021/ma9512115}, - eprint = {http://pubs.acs.org/doi/pdf/10.1021/ma9512115}, - url = {http://pubs.acs.org/doi/abs/10.1021/ma9512115}, - journal = {Macromolecules}, - owner = {Kohlbrecher}, - timestamp = {2012.03.30} -} - -@ARTICLE{Pedersen1990, - author = {Pedersen, J. S. and Posselt, D. and Mortensen, K.}, - title = {Analytical treatment of the resolution function for small-angle scattering}, - year = {1990}, - volume = {23}, - number = {4}, - month = {Aug}, - pages = {321--333}, - doi = {10.1107/S0021889890003946}, - url = {http://dx.doi.org/10.1107/S0021889890003946}, - journal = {Journal of Applied Crystallography}, - owner = {kohlbrecher}, - timestamp = {2010.05.08} -} - -@ARTICLE{Pedersen96Macrom, - author = {Pedersen, J. S. and P. Schurtenberger}, - title = {Scattering functions of semiflexible polymers with and without excluded - volume effects.}, - year = {1996}, - volume = {29}, - pages = {7602-7612}, - doi = {10.1021/ma9607630}, - url = {http://pubs.acs.org/doi/abs/10.1021/ma9607630}, - abstract = {Off-lattice Monte Carlo simulations on semiflexible polymer chains - with and without excluded volume interactions have been performed. - The model used in the simulations is a discrete representation of - the worm-like chain model of Kratky and Porod applied in the pseudocontinuous - limit. The ratio between the cross-section radius R of the chain - and the statistical segment length b was chosen to be R/b = 0.1 which - corresponds to the value found for polymer-like micelles. The ratio - R/b is equivalent to a reduced binary cluster integral of B = 0.30, - which is in accordance with the value for polystyrene in a good solvent. - The scattering functions of the semiflexible chains have been determined - with a precision of 1−2% for L/b = 0.3−640, where L is the contour - length of the chain. Numerical approximations to these functions - have been determined which interpolate between the simulated functions, - and these can be used in the analysis of experimental scattering - data. The approximations have been used in least-squares fitting - of experimental small-angle neutron scattering data from polystyrene - in a good solvent.}, - journal = {Macromolecules}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Pedersen2002a, - author = {Jan Skov Pedersen and Carsten Svaneborg}, - title = {Scattering from block copolymer micelles}, - year = {2002}, - volume = {7}, - number = {3–4}, - pages = {158 - 166}, - issn = {1359-0294}, - doi = {10.1016/S1359-0294(02)00044-4}, - url = {http://www.sciencedirect.com/science/article/pii/S1359029402000444}, - abstract = {Small-angle neutron and X-ray scattering are techniques, which are - frequently used for studying the structure and interactions of block - copolymer micelles. Recent developments of models for the analysis - of small-angle scattering data are reviewed. The most recent models, - based on Monte Carlo simulations, are able to provide information - on shape, aggregation number, polydispersity, core size, core solvation, - corona shape/size, and on the interactions between the chains in - the corona.}, - journal = {Current Opinion in Colloid \& Interface Science}, - keywords = {Block copolymer}, - owner = {Kohlbrecher}, - timestamp = {2012.03.30} -} - -@ARTICLE{Percus1958, - author = {J. K. Percus and G. J. Yevick}, - title = {Analysis of classical statistical mechanics by means of collective - coordinates}, - year = {1958}, - volume = {110}, - number = {1}, - pages = {1-13}, - journal = {Phys. Rev.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Petrache1998, - author = {Petrache, Horia I. and Gouliaev, Nikolai and Tristram-Nagle, Stephanie - and Zhang, Ruitian and Suter, Robert M. and Nagle, John F.}, - title = {Interbilayer interactions from high-resolution x-ray scattering}, - year = {1998}, - volume = {57}, - number = {6}, - month = {Jun}, - pages = {7014--7024}, - doi = {10.1103/PhysRevE.57.7014}, - journal = {Phys. Rev. E}, - numpages = {10}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2010.06.04} -} - -@ARTICLE{Phuengrattana2011, - author = {Withun Phuengrattana and Suthep Suantai}, - title = {On the rate of convergence of Mann, Ishikawa, Noor and SP-iterations - for continuous functions on an arbitrary interval }, - year = {2011}, - volume = {235}, - number = {9}, - pages = {3006 - 3014}, - issn = {0377-0427}, - doi = {http://dx.doi.org/10.1016/j.cam.2010.12.022}, - url = {http://www.sciencedirect.com/science/article/pii/S0377042710006722}, - abstract = {In this paper, we propose a new iteration, called the SP-iteration, - for approximating a fixed point of continuous functions on an arbitrary - interval. Then, a necessary and sufficient condition for the convergence - of the SP-iteration of continuous functions on an arbitrary interval - is given. We also compare the convergence speed of Mann, Ishikawa, - Noor and SP-iterations. It is proved that the SP-iteration is equivalent - to and converges faster than the others. Our results extend and improve - the corresponding results of Borwein and Borwein [D. Borwein, J. Borwein, - Fixed point iterations for real functions, J. Math. Anal. Appl. 157 - (1991) 112–126], Qing and Qihou [Y. Qing, L. Qihou, The necessary - and sufficient condition for the convergence of Ishikawa iteration - on an arbitrary interval, J. Math. Anal. Appl. 323 (2006) 1383–1386], - Rhoades [B.E. Rhoades, Comments on two fixed point iteration methods, - J. Math. Anal. Appl. 56 (1976) 741–750], and many others. Moreover, - we also present numerical examples for the SP-iteration to compare - with the Mann, Ishikawa and Noor iterations. }, - journal = {Journal of Computational and Applied Mathematics }, - keywords = {Continuous functions}, - owner = {kohlbrecher}, - timestamp = {2014.06.09} -} - -@ARTICLE{Picard1890, - author = {Emile Picard}, - title = {Mémoire sur la théorie des équations aux dérivées partielles et la - méthode des approximations successives}, - year = {1890}, - volume = {6}, - number = {4}, - pages = {145--210}, - url = {http://portail.mathdoc.fr/JMPA/PDF/JMPA_1890_4_6_A3_0.pdf}, - journal = {Journal de mathématiques pures et appliquées}, - owner = {Kohlbrecher}, - timestamp = {2014.06.09} -} - -@ARTICLE{Porod1948, - author = {G. Porod}, - title = {{Die Abh{\"a}ngigkeit der R{\"o}ntgenkleinwinkelstreuung von Form - und Gr{\"o}sse der Kolloiden Teilchen in verd{\"u}nnten Systemen, - IV}}, - year = {1948}, - volume = {2}, - pages = {255-292}, - journal = {Acta Physica Austriaca}, - owner = {Kohlbrecher}, - timestamp = {2009.12.15} -} - -@ARTICLE{Poeschke2000, - author = {Pöschke, Dominic and Hickl, Peter and Ballauff, Matthias and Ãstrand, - Per-Olof and Pedersen, Jan Skov}, - title = {Analysis of the conformation of worm-like chains by small-angle scattering: - Monte-Carlo simulations in comparison to analytical theory}, - year = {2000}, - volume = {9}, - number = {6}, - pages = {345--353}, - issn = {1521-3919}, - doi = {10.1002/1521-3919(20000701)9:6<345::AID-MATS345>3.0.CO;2-9}, - url = {http://dx.doi.org/10.1002/1521-3919(20000701)9:6<345::AID-MATS345>3.0.CO;2-9}, - abstract = {The analysis of the scattering intensity I0 (q) (q = (4 π/λ) sin (θ/2); - λ: wavelength of radiation; θ: scattering angle) of dissolved linear - polymers derived from static scattering experiments is considered. - The determination of I0 (q) and possible sources of experimental - uncertainties are discussed in detail. Moreover, a comprehensive - overview of current analytical models for the calculation of I0 (q) - of chains without excluded volume is given. These analytical theories - are compared to Monte-Carlo simulations of semiflexible chains without - excluded volume. It is shown that analytical expressions given by - Pedersen and Schurtenberger (Macromolecules 29, 7602 (1996); method - 2) provides the best description of the I0 (q) throughout the entire - range of stiffness. Among the analytical theories the expression - derived by Kholodenko (Macromolecules 26, 4179 (1993)) gives the - best description of the scattering function of worm-like chains.}, - journal = {Macromolecular Theory and Simulations}, - owner = {Kohlbrecher}, - publisher = {WILEY-VCH Verlag GmbH}, - timestamp = {2014.03.04} -} - -@BOOK{Press2007, - author = {William H. Press and Saul A. Teukolsky and William T. Vetterling - and Brian P. Flannery}, - title = {Numerical Recipes. The Art of Scientific Computing}, - year = {2007}, - edition = {3rd}, - publisher = {Cambridge University Press}, - owner = {kohlbrecher}, - timestamp = {2013.04.26} -} - -@ARTICLE{scatt188, - author = {C. V. Raman}, - title = {LXI. On the mean distance between neighbouring molecules in a fluid}, - year = {1924}, - volume = {47}, - pages = {671-679}, - doi = {http://dx.doi.org/10.1080/14786442408634406}, - url = {http://www.tandfonline.com/doi/abs/10.1080/14786442408634406}, - journal = {Phil. Mag.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Regnaut1990, - author = {C. Regnaut and J. C. Ravey}, - title = {Erratum: Application of the adhesive sphere model to the structure - of colloidal suspensions [J. Chem. Phys. 91, 1211 (1989)]}, - year = {1990}, - volume = {92}, - number = {5}, - pages = {3250-3250}, - doi = {10.1063/1.458616}, - url = {http://link.aip.org/link/?JCP/92/3250/1}, - journal = {The Journal of Chemical Physics}, - owner = {Kohlbrecher}, - publisher = {AIP}, - timestamp = {2009.12.18} -} - -@ARTICLE{Regnaut1989, - author = {C. Regnaut and J. C. Ravey}, - title = {Application of the adhesive sphere model to the structure of colloidal - suspensions}, - year = {1989}, - volume = {91}, - number = {2}, - pages = {1211-1221}, - doi = {10.1063/1.457194}, - url = {http://link.aip.org/link/?JCP/91/1211/1}, - journal = {The Journal of Chemical Physics}, - keywords = {COLLOIDS; SUSPENSIONS; LIQUID STRUCTURE; THERMODYNAMIC PROPERTIES; - PERCUSYEVICK EQUATION; HNC METHOD}, - owner = {Kohlbrecher}, - publisher = {AIP}, - timestamp = {2009.12.18} -} - -@ARTICLE{Richter1997, - author = {Richter, D. and Schneiders, D. and Monkenbusch, M. and Willner, L. - and Fetters, L. J. and Huang, J. S. and Lin, M. and Mortensen, K. - and Farago, B.}, - title = {Polymer Aggregates with Crystalline Cores:  The System Polyethylene−Poly(ethylenepropylene)}, - year = {1997}, - volume = {30}, - number = {4}, - pages = {1053-1068}, - doi = {10.1021/ma961039k}, - eprint = {http://pubs.acs.org/doi/pdf/10.1021/ma961039k}, - url = {http://pubs.acs.org/doi/abs/10.1021/ma961039k}, - abstract = { We have studied the aggregation behavior of polyethylene−poly(ethylenepropylene) - (PE−PEP) diblock copolymers dissolved in decane. For this purpose - PE−PEP diblock copolymers of various molecular weights, compositions, - and degrees of deuteration were synthesized via an anionic route. - The structure and morphology of the aggregates was studied by small - angle neutron scattering varying both the contrast as well as the - polymer labeling. We found a hierarchy of structures:  The PE component - crystallizes in lamellar sheets (thickness 40−80 Ã…) surrounded - on both sides by a PEP brush which exhibits a close to parabolic - density profile. Different aggregates form macroaggregates of needlelike - shape with the PE lamellar planes in the long direction. This macroaggregation - is well described by a paracrystalline structure factor. The structural - parameters depending on composition and molecular weights can be - well understood in terms of a free energy of formation based on a - scaling model. A quantitative evaluation of the different contributions - to the free energy reveals an important role of defect structures - resulting from the ethylene side branches in the polyethylene component. - Finally, we show in a semiquantitative approach that the van der - Waals energy between the brushes is large enough to facilitate macroaggregation. - }, - journal = {Macromolecules}, - owner = {Kohlbrecher}, - timestamp = {2012.03.30} -} - -@ARTICLE{Robertus1989, - author = {C. Robertus and W.H. Philipse and J.G.H. Joosten and Y.K. Levine}, - title = {Solution of the Percus-Yevick approximation of the multicomponent - - adhesive sphere system to the small angle x-ray scattering from - - microemulsions}, - year = {1989}, - volume = {90}, - number = {8}, - pages = {4482-4490}, - journal = {J. Chem. Phys.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Rogers1984, - author = {Rogers, Forrest J. and Young, David A.}, - title = {New, thermodynamically consistent, integral equation for simple fluids}, - year = {1984}, - volume = {30}, - issue = {2}, - month = {Aug}, - pages = {999--1007}, - doi = {10.1103/PhysRevA.30.999}, - url = {http://link.aps.org/doi/10.1103/PhysRevA.30.999}, - journal = {Phys. Rev. A}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2013.10.21} -} - -@ARTICLE{Roux1988, - author = {D. Roux and C.R. Safinya}, - title = {A synchrotron X-ray study of competing undulation and electrostatic - interlayer interactions in fluid multimembrane lyotropic phases}, - year = {1988}, - volume = {49}, - number = {2}, - pages = {307-318}, - doi = {10.1051/jphys:01988004902030700}, - url = {http://hal.archives-ouvertes.fr/docs/00/21/06/98/PDF/ajp-jphys_1988_49_2_307_0.pdf}, - journal = {J. Phys. France}, - owner = {kohlbrecher}, - timestamp = {2010.06.04} -} - -@ARTICLE{Sorensen1992, - author = {C. M. S{\o}rensen and J. Cai and N. Lu}, - title = {Test of Static Structure Factors for Describing Light Scattering - from Fractal Soot Aggregates}, - year = {1992}, - volume = {8}, - pages = {2064-2069}, - doi = {10.1021/la00044a029}, - url = {http://pubs.acs.org/doi/abs/10.1021/la00044a029}, - journal = {Langmuir}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Sorensen1999, - author = {C. M. S{\o}rensen and G. M. Wang}, - title = {Size distribution effect on the power law regime of the structure - factor of fractal aggregates}, - year = {1999}, - volume = {60}, - number = {6}, - pages = {7143-7148}, - doi = {10.1103/PhysRevE.60.7143}, - url = {http://link.aps.org/doi/10.1103/PhysRevE.60.7143}, - journal = {Physical Review E}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Saad1993, - author = {Youcef Saad}, - title = {A Flexible Inner-Outer Preconditioned GMRES Algorithm}, - year = {1993}, - volume = {14}, - number = {2}, - pages = {461-469}, - doi = {10.1137/0914028}, - eprint = { http://dx.doi.org/10.1137/0914028 }, - url = { http://dx.doi.org/10.1137/0914028 -}, - journal = {SIAM Journal on Scientific Computing}, - owner = {kohlbrecher}, - timestamp = {2015.12.16} -} - -@ARTICLE{Saad1986, - author = {Youcef Saad and Martin H. Schultz}, - title = {GMRES: A Generalized Minimal Residual Algorithm for Solving Nonsymmetric - Linear Systems}, - year = {1986}, - volume = {7}, - number = {3}, - pages = {856-869}, - doi = {10.1137/0907058}, - eprint = { http://dx.doi.org/10.1137/0907058 }, - url = { http://dx.doi.org/10.1137/0907058 -}, - journal = {SIAM Journal on Scientific and Statistical Computing}, - owner = {kohlbrecher}, - timestamp = {2015.12.16} -} - -@ARTICLE{StreyKlineKaler1994, - author = {K.-V. Schubert and R. Strey and S. R. Kline and E. W. Kaler}, - title = {Small angle neutron scattering near Lifshitz lines: Transition from - weakly structured mixtures to microemulsions}, - year = {1994}, - volume = {101}, - pages = {5343}, - doi = {10.1063/1.467387}, - journal = {J. Chem. Phys.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Schumacher2009, - author = {Manuela Schumacher and Markus Ruppel and Joachim Kohlbrecher and - Markus Burkhardt and Felix Plamper and Markus Drechsler and Axel - H.E. Müller}, - title = {Smart organic-inorganic nanohybrid stars based on star-shaped poly(acrylic - acid) and functional silsesquioxane nanoparticles}, - year = {2009}, - volume = {50}, - number = {8}, - pages = {1908 - 1917}, - issn = {0032-3861}, - doi = {DOI: 10.1016/j.polymer.2009.02.010}, - url = {http://www.sciencedirect.com/science/article/B6TXW-4VNH42B-2/2/681e3a8be5ecf579297bde4679bc481a}, - abstract = {pH- and salinity-responsive organic-inorganic nanohybrid stars based - on poly(acrylic acid) (PAA) stars and N,N-di(2,3-dihydroxypropyl)3-aminopropylfunctional - silsesquioxane nanoparticles are readily formed by mixing of aqueous - solutions of the components. The interaction between stars of two - different arm lengths, (PAA100)21, (PAA200)24, with water-soluble - silsesquioxane nanoparticles is studied according to changes in pH - and salt concentration. The original size of the stars is conserved - during complexation according to dynamic light scattering (DLS) measurements - and light scattering (LS) titration experiments, which exclude star-star - aggregation or crosslinking during the interaction. The proposed - interaction mechanism is based on hydrogen-bonding and Coulomb interactions. - Cryogenic transmission electron microscopy measurements demonstrate - the formation of nanohybrid stars. Small-angle neutron scattering - experiments enable a quantitative determination of the fraction of - bound nanoparticles and indicate an equilibrium between free and - bound nanoparticles.}, - journal = {Polymer}, - keywords = {Polyelectrolyte stars}, - owner = {Kohlbrecher}, - timestamp = {2009.03.25} -} - -@ARTICLE{Schwartz1975, - author = {S. Schwartz and J.E. Cain and E.A. Dratz and J.K. Blasie}, - title = {An analysis of lamellar x-ray diffraction from disordered membrane - multilayers with application to data from retinal rod}, - year = {1975}, - volume = {15}, - pages = {1201 - 1233}, - doi = {10.1016/S0006-3495(75)85895-4}, - url = {http://www.sciencedirect.com/science/article/B94RW-4V8RSSX-3/2/1b9b816948c363ebf75128d31846eca1}, - abstract = {Oriented multilayers containing a membrane pair within the unit cell - potentially possess both lattice disorder and substitution disorder. - Lattice disorder occurs when there is a lack of long-range order - in the lattice spacings produced by a variation in the nearest neighbor - distances between unit cells. A simple form of substitution disorder - can arise from a variation in the separation of the two membranes - within the unit cells in the multilayer. Lattice disorder produces - a monotonically increasing width for higher order lamellar "reflections" - while simple substitution disorder produces an incoherent intensity - underlying the coherent intensity. A generalized Patterson function - analysis has been developed for treating lamellar diffraction from - lattice disordered multilayers. This analysis allows the identification - of the autocorrelation function of the unit cell electron density - profile and its subsequent deconvolution to provide the unit cell - electron density profile. A recursive procedure has been developed - for separating the incoherent intensity from the coherent intensity - via a Gaussian probability model of the membrane intra-pair separation. - In cases studied so far both disorders can be quantitatively accounted - for and eliminated from interfering with the phasing of the coherent - intensity or distorting the derived electron density profile. Lamellar - X-ray diffraction data from intact retinal rods, using either film - or position sensitive detectors, shows severe effects of both forms - of disorder which have not been taken into account in past analysis - of such data. We have applied our analysis to the data on dark adapted - rod outer segments in electrophysiologically intact retinas of Chabre - and Cavaggioni (unpublished). An electron density profile is derived - at 25 A resolution. The lattice nearest neighbor spacing has a variation - of +/- 19 A out of a 295 A repeat. The intra-unit cell membrane pair - center to center distance of 88 A varies +/-8 A."}, - journal = {Biophysical Journal}, - owner = {kohlbrecher}, - timestamp = {2010.06.04} -} - -@ARTICLE{Sergiievskyi2011, - author = {Sergiievskyi, Volodymyr P. and Hackbusch, Wolfgang and Fedorov, Maxim - V.}, - title = {Multigrid solver for the reference interaction site model of molecular - liquids theory}, - year = {2011}, - volume = {32}, - number = {9}, - pages = {1982--1992}, - issn = {1096-987X}, - doi = {10.1002/jcc.21783}, - url = {http://dx.doi.org/10.1002/jcc.21783}, - journal = {Journal of Computational Chemistry}, - keywords = {multigrid, RISM, integral equation theory, hydration free energy}, - owner = {kohlbrecher}, - publisher = {Wiley Subscription Services, Inc., A Wiley Company}, - timestamp = {2013.12.03} -} - -@ARTICLE{Sharma1977, - author = {R. V. Sharma and K. C. Sharma}, - title = {The structure factor and the transport properties of dense fluids - having molecules with square well potential, a possible generalization}, - year = {1977}, - volume = {89}, - number = {1}, - pages = {213 - 218}, - issn = {0378-4371}, - doi = {DOI: 10.1016/0378-4371(77)90151-0}, - url = {http://www.sciencedirect.com/science/article/B6TVG-46D5KXJ-TB/2/a0c6ad232ccc1b7979ac2fefe23f9b02}, - abstract = {An analytical expression of the static structure factor S(k) has been - presented, treating the square well potential as a perturbation on - the hard sphere system incorporating the correct equation of state - given by Carnahan and Starling (CS). Reasonable values of potential - parameters are obtained from a fit with the experimental peak of - S(k). The present calculation of transport coefficients for liquid - sodium at 373 K, is found to be in closer agreement with the experimental - data. The role of back scattering correction is also discussed.}, - journal = {Physica A: Statistical and Theoretical Physics}, - owner = {Kohlbrecher}, - timestamp = {2009.12.18} -} - -@ARTICLE{Sjoberg1974, - author = {Sj{\"{o}}berg, B.}, - title = {{Small-angle X-ray investigation of the equilibria between copper(II) - and glycyl-{\sc l}-histidylglycine in water solution. A method for - analysing polydispersed systems}}, - year = {1974}, - volume = {7}, - number = {2}, - month = {Apr}, - pages = {192--199}, - doi = {10.1107/S0021889874009241}, - url = {http://dx.doi.org/10.1107/S0021889874009241}, - journal = {Journal of Applied Crystallography}, - owner = {kohlbrecher}, - timestamp = {2010.05.07} -} - -@ARTICLE{Smith1977, - author = {Smith, William R. and Henderson, Douglas and Tago, Yoshio}, - title = {Mean spherical approximation and optimized cluster theory for the - squar-well fluid}, - year = {1977}, - volume = {67}, - number = {11}, - pages = {5308-5316}, - doi = {http://dx.doi.org/10.1063/1.434709}, - url = {http://scitation.aip.org/content/aip/journal/jcp/67/11/10.1063/1.434709}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.12.01} -} - -@ARTICLE{Sottmann1997, - author = {Sottmann, T. and Strey, R. and Chen, S.-H.}, - title = {A small-angle neutron scattering study of nonionic surfactant molecules - at the water–oil interface: Area per molecule, microemulsion domain - size, and rigidity}, - year = {1997}, - volume = {106}, - number = {15}, - pages = {6483-6491}, - doi = {http://dx.doi.org/10.1063/1.473638}, - url = {http://scitation.aip.org/content/aip/journal/jcp/106/15/10.1063/1.473638}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2015.01.28} -} - -@BOOK{book:Squires, - author = {G. L. Squires}, - title = {Thermal Neutron Scattering}, - year = {1978}, - publisher = {Cambridge University Press}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Stieger2004, - author = {Stieger, Markus and Pedersen, Jan Skov and Lindner, Peter and Richtering, - Walter}, - title = {Are Thermoresponsive Microgels Model Systems for Concentrated Colloidal - Suspensions? A Rheology and Small-Angle Neutron Scattering Study}, - year = {2004}, - volume = {20}, - number = {17}, - pages = {7283-7292}, - note = {PMID: 15301516}, - doi = {10.1021/la049518x}, - eprint = {http://pubs.acs.org/doi/pdf/10.1021/la049518x}, - url = {http://pubs.acs.org/doi/abs/10.1021/la049518x}, - abstract = { The structure of concentrated temperature-sensitive poly(N-isopropylacrylamide) - (PNiPAM) microgel suspensions has been investigated employing rheology - and small-angle neutron scattering (SANS). A previously described - model expression for the particle form factor Pinho(q) is extended - by a model hard sphere structure factor S(q), and the average radial - density profiles φ(r) are calculated from the amplitude of the form - factor A(q) and the structure factor S(q). By this procedure, a direct - real space description of the spatial ordering in the neighborhood - of a single particle is obtained. The overall particle size and the - correlation length ξ of the concentration fluctuations of the internal - polymer network decrease with concentration, revealing the increasing - compression of the spheres. Thus, the particle form factor Pinho(q) - of the swollen PNiPAM microgels depends on concentration. The particle−particle - interaction potential does not change significantly between 25 and - 32 °C. Even approximately 1 K below the lower critical solution - temperature (LCST), the experimental scattering intensity distributions - I(q)/c are described very well by the hard sphere structure factor - when an equivalent hard sphere particle size RHS and volume fraction - ηHS are used. Microgels with different degrees of cross-linking - and particle size resemble true hard sphere behavior up to effective - volume fractions of φeff < 0.35. At higher effective volume fractions - φeff > 0.35 strong deviations from true hard spheres are observed. - Interpenetration of the outer, less cross-linked regions of the soft - spheres as well as particle compression occurred at higher concentrations. - In agreement with this, the equilibrium colloidal phase behavior - and rheology also has some features of soft sphere systems. At temperatures - well above the LCST, the interaction potential becomes strongly attractive - and the collapsed microgel spheres form aggregates consisting of - flocculated particles without significant long-range order. Hence, - an attractive interaction potential in concentrated suspensions of - PNiPAM microgels leads to distinctively different structures as compared - to attractive hard sphere colloids. When the peculiar structural - properties of the PNiPAM microgels are considered, they can be used - as model systems in colloidal science. }, - journal = {Langmuir}, - owner = {Kohlbrecher}, - timestamp = {2012.01.14} -} - -@ARTICLE{Strey1991, - author = {Strey, R. and Winkler, J. and Magid, L.}, - title = {Small-angle neutron scattering from diffuse interfaces. 1. Mono- - and bilayers in the water-octane-pentaoxyethylene monododecyl ether - (C12Es) system}, - year = {1991}, - volume = {95}, - number = {19}, - pages = {7502-7507}, - doi = {10.1021/j100172a070}, - eprint = { http://dx.doi.org/10.1021/j100172a070 }, - url = { http://dx.doi.org/10.1021/j100172a070 -}, - journal = {The Journal of Physical Chemistry}, - owner = {kohlbrecher}, - timestamp = {2015.01.28} -} - -@ARTICLE{Svaneborg2012, - author = {Carsten Svaneborg and Jan Skov Pedersen}, - title = {A formalism for scattering of complex composite structures. I. Applications - to branched structures of asymmetric sub-units}, - year = {2012}, - volume = {136}, - number = {10}, - eid = {104105}, - pages = {104105}, - doi = {10.1063/1.3682778}, - url = {http://link.aip.org/link/?JCP/136/104105/1}, - journal = {The Journal of Chemical Physics}, - keywords = {molecular configurations; polymers}, - numpages = {14}, - owner = {Kohlbrecher}, - publisher = {AIP}, - timestamp = {2012.03.30} -} - -@ARTICLE{SvaneborgPedersen2002, - author = {Svaneborg, Carsten and Pedersen, Jan Skov}, - title = {Form Factors of Block Copolymer Micelles with Excluded-Volume Interactions - of the Corona Chains Determined by Monte Carlo Simulations}, - year = {2002}, - volume = {35}, - number = {3}, - pages = {1028-1037}, - doi = {10.1021/ma011046v}, - eprint = {http://pubs.acs.org/doi/pdf/10.1021/ma011046v}, - url = {http://pubs.acs.org/doi/abs/10.1021/ma011046v}, - abstract = {The scattering of a diblock copolymer micelle has been simulated using - Monte Carlo techniques. The scattering is analyzed using a novel - model, where the corona is represented as a dilute/semidilute polymer - solution with a radial profile. This approach decouples the scattering - due to interaction and connectivity induced density fluctuations - and scattering due to the radial profile of the corona. Three different - profiles have been used to fit the simulated corona scattering:  - a box with a Gaussian tail and two maximum entropy (ME) profiles; - chain penetration into the core region is not allowed for any of - the profiles. Excellent fits are obtained, especially for a ME profile - with three parameters. An excluded-volume parameter and the corona - compressibility are obtained and show a strong dependence on surface - coverage. The derived expressions for the form factor provides a - new approach for analyzing experimental data obtained by neutron - or X-ray small-angle scattering for block copolymer micelles with - significant intra- and interchain excluded-volume interactions.}, - journal = {Macromolecules}, - owner = {Kohlbrecher}, - timestamp = {2012.03.30} -} - -@ARTICLE{Svaneborg2001, - author = {Svaneborg, Carsten and Pedersen, Jan Skov}, - title = {Block copolymer micelle coronas as quasi-two-dimensional dilute or - semidilute polymer solutions}, - year = {2001}, - volume = {64}, - issue = {1}, - month = {Jun}, - pages = {010802}, - doi = {10.1103/PhysRevE.64.010802}, - url = {http://link.aps.org/doi/10.1103/PhysRevE.64.010802}, - journal = {Phys. Rev. E}, - numpages = {4}, - owner = {Kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2012.03.30} -} - -@ARTICLE{Svaneborg2000, - author = {Carsten Svaneborg and Jan Skov Pedersen}, - title = {A Monte Carlo study on the effect of excluded volume interactions - on the scattering from block copolymer micelles}, - year = {2000}, - volume = {112}, - number = {21}, - pages = {9661-9670}, - doi = {10.1063/1.481586}, - url = {http://link.aip.org/link/?JCP/112/9661/1}, - journal = {The Journal of Chemical Physics}, - keywords = {polymer blends; colloids; scattering; Monte Carlo methods; digital - simulation; light scattering; polymer solutions}, - owner = {Kohlbrecher}, - publisher = {AIP}, - timestamp = {2012.03.30} -} - -@ARTICLE{TeubnerStrey87, - author = {M. Teubner and R. Strey}, - title = {Origin of the scattering peak in microemulsions}, - year = {1987}, - volume = {87}, - pages = {3195}, - doi = {10.1063/1.453006}, - journal = {J. Chem. Phys.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Toon1981, - author = {O. Toon and T. Ackerman}, - title = {Algorithms for the calculation of scattering by stratified spheres}, - year = {1981}, - volume = {20}, - number = {20}, - pages = {3657}, - journal = {Applied Optics}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Toth2015, - author = {A. Toth and C.T. Kelley}, - title = {Convergence analysis for Anderson acceleration}, - year = {2015}, - volume = {53}, - number = {2}, - pages = {805-819}, - note = {cited By 0}, - doi = {10.1137/130919398}, - url = {http://www.scopus.com/inward/record.url?eid=2-s2.0-84929440254&partnerID=40&md5=d51e4f335fb6b709974bb40be37ca09f}, - abstract = {Anderson(m) is a method for acceleration of fixed point iteration - which stores m+1 prior evaluations of the fixed point map and computes - the new iteration as a linear combination of those evaluations. Anderson(0) - is fixed point iteration. In this paper we show that Anderson(m) - is locally r-linearly convergent if the fixed point map is a contraction - and the coefficients in the linear combination remain bounded. Without - assumptions on the coefficients, we prove q-linear convergence of - Anderson(1) and, in the case of linear problems, Anderson(m). We - observe that the optimization problem for the coefficients can be - formulated and solved in nonstandard ways and report on numerical - experiments which illustrate the ideas. © 2015 Society for Industrial - and Applied Mathematics.}, - affiliation = {Department of Mathematics, North Carolina State University, Raleigh, - NC, United States}, - author_keywords = {Anderson acceleration; Local convergence; Nonlinear equations}, - document_type = {Article}, - journal = {SIAM Journal on Numerical Analysis}, - owner = {kohlbrecher}, - source = {Scopus}, - timestamp = {2015.12.16} -} - -@ARTICLE{Tuinier2003, - author = {R Tuinier and J Rieger and C.G de Kruif}, - title = {Depletion-induced phase separation in colloid-polymer mixtures}, - year = {2003}, - volume = {103}, - number = {1}, - pages = {1 - 31}, - issn = {0001-8686}, - doi = {http://dx.doi.org/10.1016/S0001-8686(02)00081-7}, - url = {http://www.sciencedirect.com/science/article/pii/S0001868602000817}, - abstract = {Phase separation can be induced in a colloidal dispersion by adding - non-adsorbing polymers. Depletion of polymer around the colloidal - particles induces an effective attraction, leading to demixing at - sufficient polymer concentration. This communication reviews theoretical - and experimental work carried out on the polymer-mediated attraction - between spherical colloids and the resulting phase separation of - the polymer-colloid mixture. Theoretical studies have mainly focused - on the limits where polymers are small or large as compared to the - colloidal size. Recently, however, theories are being developed that - cover a wider colloid-polymer size ratio range. In practical systems, - size polydispersity and polyelectrolytes (instead of neutral polymers) - and/or charges on the colloidal surfaces play a role in polymer-colloid - mixtures. The limited amount of theoretical work performed on this - is also discussed. Finally, an overview is given on experimental - investigations with respect to phase behavior and results obtained - with techniques enabling measurement of the depletion-induced interaction - potential, the structure factor, the depletion layer thickness and - the interfacial tension between the demixed phases of a colloid-polymer - mixture.}, - journal = {Advances in Colloid and Interface Science }, - keywords = {Depletion}, - owner = {kohlbrecher}, - timestamp = {2013.11.21} -} - -@ARTICLE{Ulander2001, - author = {Ulander, Johan and Greberg, Hans and Kjellander, Roland}, - title = {Primary and secondary effective charges for electrical double layer - systems with asymmetric electrolytes}, - year = {2001}, - volume = {115}, - number = {15}, - pages = {7144-7160}, - doi = {http://dx.doi.org/10.1063/1.1398587}, - url = {http://scitation.aip.org/content/aip/journal/jcp/115/15/10.1063/1.1398587}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.20} -} - -@ARTICLE{Verlet1981, - author = {Verlet, Loup}, - title = {Integral equations for classical fluids}, - year = {1981}, - volume = {42}, - number = {6}, - pages = {1291-1302}, - doi = {10.1080/00268978100100971}, - eprint = {http://www.tandfonline.com/doi/pdf/10.1080/00268978100100971}, - url = {http://www.tandfonline.com/doi/abs/10.1080/00268978100100971}, - journal = {Molecular Physics}, - owner = {kohlbrecher}, - timestamp = {2013.10.21} -} - -@ARTICLE{Verlet1980, - author = {Verlet, Loup}, - title = {Integral equations for classical fluids}, - year = {1980}, - volume = {41}, - number = {1}, - pages = {183-190}, - doi = {10.1080/00268978000102671}, - eprint = {http://www.tandfonline.com/doi/pdf/10.1080/00268978000102671}, - url = {http://www.tandfonline.com/doi/abs/10.1080/00268978000102671}, - journal = {Molecular Physics}, - owner = {kohlbrecher}, - timestamp = {2013.10.21} -} - -@ARTICLE{Viererblova2010, - author = {Viererblova, Linda and Kolafa, Jiri and Labik, Stanislav and Malijevsky, - Anatol}, - title = {Virial coefficients and equation of state of the penetrable sphere - model}, - year = {2010}, - volume = {12}, - issue = {1}, - pages = {254-262}, - doi = {10.1039/B917204A}, - url = {http://dx.doi.org/10.1039/B917204A}, - abstract = {We study the penetrable sphere (alias square mound) model in the fluid - phase by means of the virial expansion{,} molecular dynamics simulations{,} - and Ornstein-Zernike integral equation. The virial coefficients up - to B8 are expressed as polynomials in the Boltzmann factor with the - coefficients calculated by a Monte Carlo integration. New data for - pressure and internal energy are obtained by molecular dynamics simulations - with attention paid to finite-size errors and properties of the Andersen - thermostat. The data and virial coefficients are correlated by a - formula for the Helmholtz free energy. We also propose a new closure - for the Ornstein-Zernike equation and test several other closures.}, - journal = {Phys. Chem. Chem. Phys.}, - owner = {kohlbrecher}, - publisher = {The Royal Society of Chemistry}, - timestamp = {2013.11.10} -} - -@ARTICLE{Vompe1994, - author = {Vompe, A. G. and Martynov, G. A.}, - title = {The bridge function expansion and the self-consistency problem of - the Ornstein-Zernike equation solution}, - year = {1994}, - volume = {100}, - number = {7}, - pages = {5249-5258}, - doi = {http://dx.doi.org/10.1063/1.467189}, - url = {http://scitation.aip.org/content/aip/journal/jcp/100/7/10.1063/1.467189}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.11} -} - -@ARTICLE{scatt121, - author = {C. G. Vonk}, - title = {On two methods for determination of particle size distribution functions - by means of small-angle x-ray scattering}, - year = {1976}, - volume = {9}, - pages = {433-440}, - journal = {J. Appl. Cryst.}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Vorst1992, - author = {H. A. van der Vorst}, - title = {Bi-CGSTAB: A Fast and Smoothly Converging Variant of Bi-CG for the - Solution of Nonsymmetric Linear Systems}, - year = {1992}, - volume = {13}, - number = {2}, - pages = {631-644}, - doi = {10.1137/0913035}, - eprint = { http://dx.doi.org/10.1137/0913035 }, - url = { http://dx.doi.org/10.1137/0913035 -}, - journal = {SIAM Journal on Scientific and Statistical Computing}, - owner = {kohlbrecher}, - timestamp = {2015.12.16} -} - -@ARTICLE{Vrij1979, - author = {A. Vrij}, - title = {Mixtures of hard spheres in the Percus-Yevick approximation. Light - scattering at finite angles}, - year = {1979}, - volume = {71}, - number = {8}, - pages = {3267-3270}, - journal = {J. Chem. Phys.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Vrij1976, - author = {A. Vrij}, - title = {Polymers at Interfaces and the Interactions in Colloidal Dispersions}, - year = {1976}, - volume = {48}, - number = {4}, - pages = {471--483}, - doi = {10.1351/pac197648040471}, - url = {http://dx.doi.org/10.1351/pac197648040471}, - journal = {Pure Appl. Chem.}, - owner = {kohlbrecher}, - timestamp = {2013.11.21} -} - -@PHDTHESIS{Vyskocil1994, - author = {Pavel Vyskocil}, - title = {Decomposition and coarsening in Ni-Ti}, - year = {1994}, - doi = {http://dx.doi.org/10.3929/ethz-a-000937740}, - url = {http://e-collection.library.ethz.ch/view/eth:39304}, - abstract = {http://e-collection.library.ethz.ch/eserv/eth:39304/eth-39304-01.pdf}, - owner = {kohlbrecher}, - school = {ETH Zurich}, - timestamp = {2014.12.22} -} - -@INBOOK{Wagner2005, - author = {W. Wagner and J. Kohlbrecher}, - title = {Modern Techniques For Characterising Magnetic Materials:}, - year = {2005}, - editor = {Yimei Zhu}, - publisher = {Kluwer Academic Publishers}, - chapter = {Small-angle neutron scattering}, - pages = {65-104}, - url = {http://sans.web.psi.ch/sansstatus/SASbooks/KluwerBookch2.pdf}, - keywords = {magnetic materials - Analysis; - - magnetic materials - Microscopy; - - Electrons - Scattering;}, - owner = {Kohlbrecher}, - timestamp = {2008.05.10} -} - -@ARTICLE{Walker2011, - author = {Homer F. Walker and Peng Ni}, - title = {Anderson Acceleration for Fixed-Point Iterations}, - year = {2011}, - volume = {49}, - number = {4}, - pages = {1715-1735}, - doi = {10.1137/10078356X}, - eprint = { http://dx.doi.org/10.1137/10078356X }, - url = { http://dx.doi.org/10.1137/10078356X -}, - journal = {SIAM Journal on Numerical Analysis}, - owner = {kohlbrecher}, - timestamp = {2015.12.16} -} - -@ARTICLE{Walter1985, - author = {Walter, G. and Kranold, R. and Gerber, T. and Baldrian, J. and Steinhart, - M.}, - title = {{Particle size distribution from small-angle X-ray scattering data}}, - year = {1985}, - volume = {18}, - number = {4}, - month = {Aug}, - pages = {205--213}, - doi = {10.1107/S0021889885010160}, - url = {http://dx.doi.org/10.1107/S0021889885010160}, - journal = {Journal of Applied Crystallography}, - owner = {kohlbrecher}, - timestamp = {2010.05.07} -} - -@ARTICLE{Weeks1971, - author = {Weeks, John D. and Chandler, David and Andersen, Hans C.}, - title = {Role of Repulsive Forces in Determining the Equilibrium Structure - of Simple Liquids}, - year = {1971}, - volume = {54}, - number = {12}, - pages = {5237-5247}, - doi = {http://dx.doi.org/10.1063/1.1674820}, - url = {http://scitation.aip.org/content/aip/journal/jcp/54/12/10.1063/1.1674820}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.08} -} - -@ARTICLE{Wertheim1963, - author = {Wertheim, M. S.}, - title = {Exact Solution of the Percus-Yevick Integral Equation for Hard Spheres}, - year = {1963}, - volume = {10}, - issue = {8}, - month = {Apr}, - pages = {321--323}, - doi = {10.1103/PhysRevLett.10.321}, - url = {http://link.aps.org/doi/10.1103/PhysRevLett.10.321}, - journal = {Phys. Rev. Lett.}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2013.11.11} -} - -@ARTICLE{Wiedenmann2011, - author = {Wiedenmann, A. and G\"ahler, R. and Dewhurst, C. D. and Keiderling, - U. and Pr\'evost, S. and Kohlbrecher, J.}, - title = {Relaxation mechanisms in magnetic colloids studied by stroboscopic - spin-polarized small-angle neutron scattering}, - year = {2011}, - volume = {84}, - issue = {21}, - month = {Dec}, - pages = {214303}, - doi = {10.1103/PhysRevB.84.214303}, - url = {http://link.aps.org/doi/10.1103/PhysRevB.84.214303}, - abstract = {Stroboscopic small-angle neutron scattering by using polarized neutrons - is presented as a technique for investigations of relaxation phenomena - on a nanometer scale. Applying a cyclic perturbation to the sample - by an oscillating magnetic field allows the polarization-dependent - scattering cross-sections to be extracted as time-dependent response. - The potential of this special type of “physical” contrast variation - technique is demonstrated with three examples of ferrofluids of different - particle sizes and viscosities. The dynamics of magnetic moment reorientations - turned out to be governed by different time scales. For a temperature-dependent - fraction of individual mobile particles, a frequency-dependent phase - shift and damping of the intensity modulation have been precisely - determined and quantitatively explained using a Debye-like relaxation - model. The characteristic relaxation times, $\tau$, in the liquid - state of all samples scale with the particle volume and viscosity - confirming a Brownian-relaxation mechanism. For the remaining fraction - of particles that form locally ordered domains the orientation distribution - of the dynamically arrested static moments has been quantified by - an order parameter $S_1^\textrm{arr}$, which is not accessible with - nonpolarized neutrons. In a high viscous Co and a magnetite-based - ferrofluid, $S_1^\textrm{arr}$ corresponds to maximal alignment of - the static moments in the liquid state and to a gradual decrease - at lower temperatures when the solvent is frozen. In a low viscosity - Co-ferrofluid almost no preferred alignment of the arrested particle - moments was observed. In the magnetite-based ferrofluid with the - highest dipolar attraction energy an additional phase shift has been - detected which increases with frequency and magnitude of the magnetic - field. This indicates clearly that the set-up of local particle ordering - in distorted hexagonal arrangement is delayed with respect to the - moment alignment in the time varying magnetic field.}, - journal = {Phys. Rev. B}, - numpages = {13}, - owner = {Kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2011.12.07} -} - -@ARTICLE{Wijmans93, - author = {C. M. Wijmans and E. B. Zhulina}, - title = {Polymer Brushes at Curved Surfaces}, - year = {1993}, - volume = {26}, - pages = {1214-7224}, - journal = {Macromolecules}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Willner2000, - author = {L. Willner and A. Poppe and J. Allgaier and M. Monkenbusch and P. - Lindner and D. Richter}, - title = {Micellization of amphiphilic diblock copolymers: Corona shape and - mean-field to scaling crossover}, - year = {2000}, - volume = {51}, - number = {6}, - pages = {628}, - url = {http://stacks.iop.org/0295-5075/51/i=6/a=628}, - abstract = {The aggregation behaviour of six amphiphilic poly(ethylene-propylene)-block-polyethylene - oxide (PEP-PEO) copolymers in water was investigated with the aim - to study systematically the influence of a growing soluble block - on the structural properties of the micelle. The polymers were prepared - such that they differ in the PEO content over a large range of molecular - weights, while the PEP size was kept constant. The micelles were - characterized by small-angle neutron scattering (SANS) involving - contrast variation experiments. Data analysis was performed by a - spherical core/shell model with either constant or radial decreasing - density profile in the corona and constant density in the core for - both cases. The main new result is that we have observed a coronal - shape crossover from a micelle with homogeneous density distribution - for polymers of low PEO content to a starlike micelle with a hyperbolic - density profile for polymers of high PEO content. With respect to - the aggregation number this corresponds to a crossover from the mean-field - to the scaling behavior of a starlike micelle.}, - journal = {EPL (Europhysics Letters)}, - owner = {kohlbrecher}, - timestamp = {2010.10.03} -} - -@ARTICLE{Wiscombe1980, - author = {W. Wiscombe}, - title = {Improved Mie scattering algorithms}, - year = {1980}, - volume = {19}, - pages = {1505-1509}, - journal = {Appl. Opt.}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@TECHREPORT{Wiscombe1979, - author = {W. Wiscombe}, - title = {Mie Scattering Calculations--Advances in - - Technique And Fast, Vector-Speed Computer Codes, Ncar Tech Note - - TN-140+STR}, - institution = {National Center For Atmospheric Research, Boulder, - - Colorado}, - year = {1979}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@ARTICLE{Yoshizaki1980, - author = {Yoshizaki, Takenao and Yamakawa, Hiromi}, - title = {Scattering Functions of Wormlike and Helical Wormlike Chains}, - year = {1980}, - volume = {13}, - number = {6}, - pages = {1518-1525}, - doi = {10.1021/ma60078a030}, - eprint = {http://pubs.acs.org/doi/pdf/10.1021/ma60078a030}, - url = {http://pubs.acs.org/doi/abs/10.1021/ma60078a030}, - journal = {Macromolecules}, - owner = {Kohlbrecher}, - timestamp = {2014.03.04} -} - -@ARTICLE{Zerah1986, - author = {Zerah, Gilles and Hansen, Jean-Pierre}, - title = {Self-consistent integral equations for fluid pair distribution functions: - Another attempt}, - year = {1986}, - volume = {84}, - number = {4}, - pages = {2336-2343}, - doi = {http://dx.doi.org/10.1063/1.450397}, - url = {http://scitation.aip.org/content/aip/journal/jcp/84/4/10.1063/1.450397}, - journal = {The Journal of Chemical Physics}, - owner = {kohlbrecher}, - timestamp = {2013.11.08} -} - -@ARTICLE{scatt163, - author = {F. Zernike and J. A. Prins}, - title = {{Die Beugung von R\"ontgenstrahlen in Fl\"ussigkeiten als Effekt - der Molek\"ulanordnung}}, - year = {1927}, - volume = {XLI}, - pages = {184-194}, - journal = {Zeitschrift f\"ur Physik}, - owner = {kohlbrecher}, - timestamp = {2007.12.17} -} - -@ARTICLE{Zhang1994, - author = {Zhang, Ruitian and Suter, Robert M. and Nagle, John F.}, - title = {Theory of the structure factor of lipid bilayers}, - year = {1994}, - volume = {50}, - number = {6}, - month = {Dec}, - pages = {5047--5060}, - doi = {10.1103/PhysRevE.50.5047}, - journal = {Phys. Rev. E}, - numpages = {13}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2010.06.04} -} - -@ARTICLE{zimm:1093, - author = {Bruno H. Zimm}, - title = {The Scattering of Light and the Radial Distribution Function of High - Polymer Solutions}, - year = {1948}, - volume = {16}, - number = {12}, - pages = {1093-1099}, - doi = {10.1063/1.1746738}, - url = {http://link.aip.org/link/?JCP/16/1093/1}, - journal = {The Journal of Chemical Physics}, - owner = {Kohlbrecher}, - publisher = {AIP}, - timestamp = {2009.04.13} -} - -@BOOK{Glatter1982, - title = {Small Angle X-ray Scattering}, - year = {1982}, - editor = {O. Glatter and O. Kratky}, - publisher = {Academic Press}, - file = {:http\://sans.web.psi.ch/sansstatus/SASbooks/Glatter_Kratky_SAXS_1982.pdf:PDF}, - owner = {kohlbrecher}, - timestamp = {2007.12.18} -} - -@INBOOK{doi:10.1142/9789812814203_0010, - title = {Ionic Distributions: An Integral Equation Approach}, - booktitle = {Molecular Thermodynamics Of Electrolyte Solutions}, - chapter = {10}, - pages = {103-141}, - doi = {10.1142/9789812814203_0010}, - eprint = {http://www.worldscientific.com/doi/pdf/10.1142/9789812814203_0010}, - url = {http://www.worldscientific.com/doi/abs/10.1142/9789812814203_0010}, - owner = {kohlbrecher}, - timestamp = {2013.11.30} -} - -@Article{Frisken2001, - author = {Barbara J. Frisken}, - title = {Revisiting the method of cumulants for the analysis of dynamic light-scattering data}, - year = {2001}, - journal = {Appl. Opt.}, - volume = {40}, - number = {24}, - month = {Aug}, - pages = {4087--4091}, - doi = {10.1364/AO.40.004087}, - url = {http://ao.osa.org/abstract.cfm?URI=ao-40-24-4087}, - abstract = {The method of cumulants is a standard technique used to analyzedynamic - light-scattering data measured for polydispersesamples. These data, - from an intensity--intensity autocorrelationfunction of the scattered - light, can be described in terms of adistribution of decay rates. - The method of cumulants providesinformation about the cumulants and - the moments of thisdistribution. However, the method does not permit - independentdetermination of the long-time baseline of the intensity - correlationfunction and can lead to inconsistent results when different - numbers ofdata points are included in the fit. The method is reformulated - interms of the moments about the mean to permit more robust andsatisfactory - fits. The different versions of the method arecompared by analysis - of the data for polydisperse-vesiclesamples.}, - keywords = {Scattering measurements; Scattering, Rayleigh}, - owner = {kohlbrecher}, - publisher = {OSA}, - timestamp = {2016.04.18}, -} - -@Book{Dhont1996, - author = {Dhont, J.K.G.}, - title = {An Introduction to Dynamics of Colloids}, - year = {1996}, - series = {Studies in Interface Science}, - publisher = {Elsevier Science}, - isbn = {9780080535074}, - url = {https://books.google.ch/books?id=mmArTF5SJ9oC}, - owner = {kohlbrecher}, - timestamp = {2016.04.18}, -} - -@Article{Pusey1974, - author = {Peter N. Pusey and Dennis E. Koppel and Dale E. Schaefer and Rafael D. Camerini-Otero and Seymour H. Koenig}, - title = {Intensity fluctuation spectroscopy of laser light scattered by solutions of spherical viruses. R17, Q.beta., BSV, PM2, and T7. I. Light-scattering technique}, - year = {1974}, - journal = {Biochemistry}, - volume = {13}, - number = {5}, - pages = {952-960}, - note = {PMID: 4591621}, - doi = {10.1021/bi00702a020}, - eprint = { http://dx.doi.org/10.1021/bi00702a020 }, - url = { http://dx.doi.org/10.1021/bi00702a020 -}, - owner = {kohlbrecher}, - timestamp = {2016.04.16}, -} - -@Article{Mailer2015, - author = {Alastair G Mailer and Paul S Clegg and Peter N Pusey}, - title = {Particle sizing by dynamic light scattering: non-linear cumulant analysis}, - year = {2015}, - journal = {Journal of Physics: Condensed Matter}, - volume = {27}, - number = {14}, - month = {4}, - pages = {145102}, - issn = {0953-8984}, - doi = {10.1088/0953-8984/27/14/145102}, - url = {http://stacks.iop.org/0953-8984/27/i=14/a=145102}, - abstract = {We revisit the method of cumulants for analysing dynamic light scattering - data in particle sizing applications. Here the data, in the form - of the time correlation function of scattered light, is written as - a series involving the first few cumulants (or moments) of the distribution - of particle diffusion constants. Frisken (2001 Appl. Opt. 40 [http://dx.doi.org/10.1364/AO.40.004087] - 4087 ) has pointed out that, despite greater computational complexity, - a non-linear, iterative, analysis of the data has advantages over - the linear least-squares analysis used originally. In order to explore - further the potential and limitations of cumulant methods we analyse, - by both linear and non-linear methods, computer-generated data with - realistic noise, where the parameters of the distribution can be - set explicitly. We find that, with modern computers, non-linear analysis - is straightforward and robust. The mean and variance of the distribution - of diffusion constants can be obtained quite accurately for distributions - of width (standard deviation/mean) up to about 0.6, but there appears - to be little prospect of obtaining meaningful higher moments.}, - keywords = {photon correlation spectroscopy, colloids, polydispersity, CORRELATION SPECTROSCOPY, INTEGRAL-EQUATIONS, PHOTON-CORRELATION, POLYDISPERSITY, INVERSION}, - owner = {kohlbrecher}, - timestamp = {2016.04.16}, -} - -@Article{BURCHARD1979589, - author = {Walther Burchard}, - title = {Determination of type and width of a size distribution from the z-averages of the radii moments rnz}, - year = {1979}, - journal = {Polymer}, - volume = {20}, - number = {5}, - pages = {589 - 592}, - issn = {0032-3861}, - doi = {http://dx.doi.org/10.1016/0032-3861(79)90170-8}, - url = {http://www.sciencedirect.com/science/article/pii/0032386179901708}, - abstract = {Relationships are given between the z-average radii moments rÌ?nz and the common moments rÌ?n of a size distribution. Instructions are given for finding the type and width of a size distribution from measurements of the rÌ?nz moments.}, - owner = {kohlbrecher}, - timestamp = {2016.04.20}, -} - -@Article{Burchard1974, - author = {Walther Burchard}, - title = {Statistics of Star-Shaped Molecules. I. Stars with Polydisperse Side Chains}, - year = {1974}, - journal = {Macromolecules}, - volume = {7}, - number = {6}, - pages = {835-841}, - doi = {10.1021/ma60042a027}, - eprint = { http://dx.doi.org/10.1021/ma60042a027 }, - url = { http://dx.doi.org/10.1021/ma60042a027 -}, - owner = {kohlbrecher}, - timestamp = {2016.04.20}, -} - -@Article{Jakes1991, - author = {Jaromír Jakeš}, - title = {A simple method of estimation of the polydispersity index of narrow molecular weight distributions by using quasielastic light scattering data}, - year = {1991}, - journal = {Collect. Czech. Chem. Commun.}, - volume = {56}, - issue = {8}, - pages = {1642-1652}, - doi = {http://dx.doi.org/10.1135/cccc19911642}, - owner = {kohlbrecher}, - timestamp = {2016.05.06}, -} - -@Article{Jakes1986, - author = {Jakeš, Jaromir and Saudek, Vladimir}, - title = {Empirical molecular weight distribution functions as determined from gel permeation chromatography data}, - year = {1986}, - journal = {Makromol. Chem.}, - volume = {187}, - number = {9}, - month = sep, - pages = {2223--2234}, - issn = {0025-116X}, - url = {http://dx.doi.org/10.1002/macp.1986.021870919}, - abstract = {Two- and three-parameter functions commonly used for the description - of the molecular weight distribution of polymers were determined - from gel permeation chromatography data for 80 water-soluble samples - of polymers derived from glutamic acid. Two methods were applied: - the moment method in which two or three different molecular weight - averages are used, and a least squares adjustment method using the - whole chromatogram. Convergence difficulties observed in the past - were overcome, and a fully automated computer procedure was developed. - The moment method, although virtually the only one still in use, - often gives inexact results: sometimes the type of two-parameter - distribution is wrongly assigned, or the description of experimental - data cannot be improved by adding yet another parameter. On the other - hand, in all cases under study the least squares method gave a function - which describes the real distribution within the limits of experimental - error. Although the majority of samples could be described by employing - one of the common two-parameter functions, the more general three-parameter - function, encompassing all two-parameter ones as special cases, has - the advantage of wider applicability. It is shown that the standard - gel permeation chromatography data often cannot provide reliable - values of higher molecular weight moment averages, including Mz. - Hence, it may be inferred that in the description of the experimental - molecular weight distribution curves the least squares method should - be preferred over the moment method.}, - owner = {kohlbrecher}, - timestamp = {2016.05.06}, -} - -@Article{Miltz1972, - author = {Miltz, J. and Ram, A.}, - title = {A three-parameter equation for molecular weight distribution of low-density polyethylene}, - year = {1972}, - journal = {Journal of Applied Polymer Science}, - volume = {16}, - number = {8}, - pages = {2051--2056}, - issn = {1097-4628}, - doi = {10.1002/app.1972.070160816}, - url = {http://dx.doi.org/10.1002/app.1972.070160816}, - abstract = {A new three-parameter distribution function is proposed -\documentclass{article}\pagestyle{empty}\begin{document}$ W\left( M \right) = AM^a \exp {\rm }[ - {\rm }b{\rm }\ln ^c \left( M \right)] $\end{document} -which fits best the experimental molecular weight distribution curves of branched lowdensity polyethylenes. The data were interpreted from GPC measurements, and a special computer program was utilized in order to derive the best values of the empirical constants a, b, and c.}, - owner = {kohlbrecher}, - publisher = {Wiley Subscription Services, Inc., A Wiley Company}, - timestamp = {2016.05.11}, -} - -@Article{Wieder1999, - author = {Wieder, Thomas}, - title = {Algorithm 794: Numerical Hankel Transform by the Fortran Program HANKEL}, - year = {1999}, - journal = {ACM Trans. Math. Softw.}, - volume = {25}, - number = {2}, - month = jun, - pages = {240--250}, - issn = {0098-3500}, - doi = {10.1145/317275.317284}, - url = {http://doi.acm.org/10.1145/317275.317284}, - acmid = {317284}, - address = {New York, NY, USA}, - issue_date = {June 1999}, - keywords = {Hankel transform, numerical analysis}, - numpages = {11}, - owner = {kohlbrecher}, - publisher = {ACM}, - timestamp = {2016.06.22}, -} - -@Article{Ooura1991, - author = {Takuya Ooura and Masatake Mori}, - title = {The double exponential formula for oscillatory functions over the half infinite interval}, - year = {1991}, - journal = {Journal of Computational and Applied Mathematics}, - volume = {38}, - number = {1}, - pages = {353 - 360}, - issn = {0377-0427}, - doi = {http://dx.doi.org/10.1016/0377-0427(91)90181-I}, - url = {http://www.sciencedirect.com/science/article/pii/037704279190181I}, - abstract = {The double exponential formula is known to be very powerful for evaluation of various kinds of integrals, in particular integrals with end point singularities or integrals over the half infinite interval. It is also known that a weak point of this formula is the inefficiency when applied to a slowly decaying oscillatory integral over the half infinite interval such as I = Int_0^Infty f1(x) sin x dx, f1(x) is an algebraic function. In this paper we propose a new type of the double exponential formula which is quite efficient for evaluation of the integral mentioned above. It is based on such a transformation that makes the points of the formula after the transformation approach to the zeros of sin x double exponentially for large x.}, - keywords = {Numerical integration, variable transformation, double exponential formula, DE-transformation, oscillatory integral}, - owner = {kohlbrecher}, - timestamp = {2016.06.24}, -} - -@Misc{LourakisJul.2004, - author = {M.I.A. Lourakis}, - title = {levmar: Levenberg-Marquardt nonlinear least squares algorithms in {C}/{C}++}, - year = {Jul. 2004}, - howpublished = {[web page] \verb+http://www.ics.forth.gr/~lourakis/levmar/+}, - note = {[Accessed on 31 Jan. 2005.]}, - url = {http://users.ics.forth.gr/~lourakis/levmar/}, - owner = {kohlbrecher}, - timestamp = {2016.07.07}, -} - -@Article{Kovalenko1999, - author = {Kovalenko, Andriy and Hirata, Fumio}, - title = {Self-consistent description of a metal-water interface by the Kohn-Sham density functional theory and the three-dimensional reference interaction site model}, - year = {1999}, - journal = {The Journal of Chemical Physics}, - volume = {110}, - number = {20}, - pages = {10095-10112}, - doi = {http://dx.doi.org/10.1063/1.478883}, - url = {http://scitation.aip.org/content/aip/journal/jcp/110/20/10.1063/1.478883}, - owner = {kohlbrecher}, - timestamp = {2016.07.18}, -} - -@Article{Hus2013, - author = {Hu\u{s}, Matej and Zalar, Matja and Urbic, Tomaz}, - title = {Correctness of certain integral equation theories for core-softened fluids}, - year = {2013}, - journal = {The Journal of Chemical Physics}, - volume = {138}, - number = {22}, - eid = {224508}, - doi = {http://dx.doi.org/10.1063/1.4809744}, - url = {http://scitation.aip.org/content/aip/journal/jcp/138/22/10.1063/1.4809744}, - owner = {kohlbrecher}, - timestamp = {2016.07.18}, -} - -@Article{Rosenfeld1979, - author = {Rosenfeld, Yaakov and Ashcroft, N. W.}, - title = {Theory of simple classical fluids: Universality in the short-range structure}, - year = {1979}, - journal = {Phys. Rev. A}, - volume = {20}, - issue = {3}, - month = {Sep}, - pages = {1208--1235}, - doi = {10.1103/PhysRevA.20.1208}, - url = {http://link.aps.org/doi/10.1103/PhysRevA.20.1208}, - numpages = {0}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2016.07.21}, -} - -@Article{Trokhymchuk2005, - author = {Trokhymchuk, Andrij and Nezbeda, Ivo and Jirsák, Jan and Henderson, Douglas}, - title = {Hard-sphere radial distribution function again}, - year = {2005}, - journal = {The Journal of Chemical Physics}, - volume = {123}, - number = {2}, - eid = {024501}, - doi = {http://dx.doi.org/10.1063/1.1979488}, - url = {http://scitation.aip.org/content/aip/journal/jcp/123/2/10.1063/1.1979488}, - owner = {kohlbrecher}, - timestamp = {2016.07.21}, -} - -@Article{Trokhymchuk2006, - author = {Trokhymchuk, Andrij and Nezbeda, Ivo and Jirsák, Jan and Henderson, Douglas}, - title = {Erratum: "Hard sphere radial distribution function again" [J. Chem. Phys.123, 024501 (2005)]}, - year = {2006}, - journal = {The Journal of Chemical Physics}, - volume = {124}, - number = {14}, - eid = {149902}, - doi = {http://dx.doi.org/10.1063/1.2188941}, - url = {http://scitation.aip.org/content/aip/journal/jcp/124/14/10.1063/1.2188941}, - owner = {kohlbrecher}, - timestamp = {2016.07.21}, -} - -@Article{Hunter2006, - author = {Hunter, Martin and Backman, Vadim and Popescu, Gabriel and Kalashnikov, Maxim and Boone, Charles W. and Wax, Adam and Gopal, Venkatesh and Badizadegan, Kamran and Stoner, Gary D. and Feld, Michael S.}, - title = {Tissue Self-Affinity and Polarized Light Scattering in the Born Approximation: A New Model for Precancer Detection}, - year = {2006}, - journal = {Phys. Rev. Lett.}, - volume = {97}, - issue = {13}, - month = {Sep}, - pages = {138102}, - doi = {10.1103/PhysRevLett.97.138102}, - url = {http://link.aps.org/doi/10.1103/PhysRevLett.97.138102}, - numpages = {4}, - owner = {kohlbrecher}, - publisher = {American Physical Society}, - timestamp = {2016.09.08}, -} - -@Article{Andersson2008, - author = {Andersson, Robert and van Heijkamp, L{\'{e}}on F. and de Schepper, Ignatz M. and Bouwman, Wim G.}, - title = {{Analysis of spin-echo small-angle neutron scattering measurements}}, - year = {2008}, - journal = {Journal of Applied Crystallography}, - volume = {41}, - number = {5}, - month = {Oct}, - pages = {868--885}, - doi = {10.1107/S0021889808026770}, - url = {http://dx.doi.org/10.1107/S0021889808026770}, - abstract = {Spin-echo small-angle neutron scattering (SESANS) is, in contrast to conventional small-angle neutron scattering (SANS), a real-space technique. SESANS measures the projection of the density{--}density correlation function of a sample, rather than, as in SANS, its Fourier transform. This paper introduces a toolkit for interpretion and analysis of a SESANS measurement. Models that are used in SANS are discussed and translated into a SESANS formalism. These models can be used to analyse and fit the data obtained by SESANS. Dilute, concentrated, random, fractal and anisotropic density distributions are considered. Numerical methods used to calculate the projection from numerical data are presented, either by using Fourier transformation or {\it via} the real-space pair correlation function.}, - keywords = {spin-echo small-angle neutron scattering (SESANS), data analysis}, - owner = {kohlbrecher}, - timestamp = {2016.09.08}, -} - -@Article{Klimes2002, - author = {Klimeš, L.}, - title = {Correlation Functions of Random Media}, - year = {2002}, - journal = {pure and applied geophysics}, - volume = {159}, - number = {7}, - pages = {1811--1831}, - issn = {1420-9136}, - doi = {10.1007/s00024-002-8710-2}, - url = {http://dx.doi.org/10.1007/s00024-002-8710-2}, - abstract = {--- In geophysics, the correlation functions of random media are of principal importance for understanding and inverting the properties of seismic waves propagating in geological structures. Unfortunately, the kinds of correlation functions inappropriate for the description of geological structures are often assumed and applied. The most frequently used types of correlation functions are thus summarized and reviewed in this paper, together with an explanation of the physical meaning of their parameters.{\textparagraph}A stationary random medium is assumed to be realized in terms of a white noise filtered by a spectral filter. The spectral filter is considered isotropic, in a simple general form enabling the random media used in geophysics to be specified. The medium correlation functions, corresponding to the individual special cases of the general random medium (Gaussian, exponential, von K{\'a}rm{\'a}n, self-affine, Kummer), are then derived and briefly discussed. The corresponding elliptically anisotropic correlation functions can simply be obtained by linear coordinate transforms.}, - owner = {kohlbrecher}, - timestamp = {2016.09.08}, -} - -@InBook{Hammouda1993, - author = {Hammouda, Boualem}, - title = {SANS from homogeneous polymer mixtures: A unified overview}, - booktitle = {Polymer Characteristics}, - year = {1993}, - publisher = {Springer Berlin Heidelberg}, - isbn = {978-3-540-47477-7}, - pages = {87--133}, - doi = {10.1007/BFb0025862}, - url = {http://dx.doi.org/10.1007/BFb0025862}, - address = {Berlin, Heidelberg}, - owner = {kohlbrecher}, - timestamp = {2016.09.09}, -} - -@Article{Hammouda2016, - author = {Boualem Hammouda}, - title = {Form Factors for Branched Polymers with Excluded Volume}, - year = {2016}, - journal = {Journal of Research of NIST}, - volume = {121}, - pages = {139--164}, - issn = {2165-7254}, - doi = {10.6028/jres.121.006}, - url = {http://dx.doi.org/10.6028/jres.121.006}, - owner = {kohlbrecher}, - timestamp = {2016.09.09}, -} - -@InBook{Bracewell2003, - author = {Bracewell, Ronald}, - title = {The Projection-Slice Theorem}, - booktitle = {Fourier Analysis and Imaging}, - year = {2003}, - publisher = {Springer US}, - isbn = {978-1-4419-8963-5}, - pages = {493--504}, - doi = {10.1007/978-1-4419-8963-5_14}, - url = {http://dx.doi.org/10.1007/978-1-4419-8963-5_14}, - address = {Boston, MA}, - owner = {kohlbrecher}, - timestamp = {2016.09.13}, -} - -@Article{Bracewell1956, - author = {Bracewell, RN}, - title = {Strip Integration in Radio Astronomy}, - journal = {Australian Journal of Physics}, - year = {1956}, - volume = {9}, - number = {2}, - issue = {9}, - pages = {198-217}, - doi = {http://dx.doi.org/10.1071/PH560198}, - url = {http://dx.doi.org/10.1071/PH560198}, - abstract = {When a celestial source of radio waves is scanned with an aerial beam which is much longer than the source in one direction but suitably narrow in the other, the transformation from the true distribution to the measured value is referred to as strip integration. It is here treated as a special case of two-dimensional aerial smoothing in which the aerial beam is allowed to spin about its centre as it moves about the sky. It is shown that the resolution obtainable is set by the cross-sectional profile of the strip beam in the narrow dimension. Thus, when the strip reduces to a line, the resolution is complete and full reconstruction of the true distribution is possible; but scans must be made in all directions. In the general case it is shown that there is a principal solution, and that a finite number of scans suffices to determine it. A method is presented for reconstructing the principal solution from the observed data.}, - owner = {kohlbrecher}, - publisher = {{CSIRO} Publishing}, - timestamp = {2016.11.07}, -} - -@Book{Bracewell2000, - author = {Ronald N. Bracewell}, - title = {The Fourier Transform and its Applications.}, - year = {2000}, - publisher = {New York: McGraw-Hill}, - owner = {kohlbrecher}, - timestamp = {2016.10.24}, -} - -@InBook{Bracewell2007, - author = {Bracewell, Ronald N.}, - title = {Fourier and Other Transform Methods}, - booktitle = {The Optics Encyclopedia}, - year = {2007}, - publisher = {Wiley-VCH Verlag GmbH \& Co. KGaA}, - isbn = {9783527600441}, - chapter = {The Optics Encyclopedia}, - pages = {725--749}, - doi = {10.1002/9783527600441.oe023}, - url = {http://dx.doi.org/10.1002/9783527600441.oe023}, - abstract = {The Fourier transform is a basic tool for optical diffraction, interferometry, sky mapping, laser resonance, tomography, and other fields. Chemical analysis using Fourier transform spectroscopy and optical signal processing are traditional one-dimensional applications, while in fiber-optic transmission and optical analogue computing, the fractional Fourier transform is a new tool. Applications of other transforms (Abel, Hankel, Hartley, Radon) are also described. Mathematical definitions and properties are tabulated for reference.}, - keywords = {transforms, interferometry, coherence, fractional Fourier transform, tomography, projection-slice theorem, nulling interferometry, volume rendering, Abel transform, Hankel transform, Hartley transform, Radon transform}, - owner = {kohlbrecher}, - timestamp = {2016.11.07}, -} - -@Article{Bracewell1990, - author = {R. N. Bracewell}, - title = {Numerical Transforms}, - journal = {Science}, - year = {1990}, - volume = {248}, - number = {4956}, - pages = {697-704}, - issn = {00368075, 10959203}, - doi = {10.1126/science.248.4956.697}, - url = {http://www.jstor.org/stable/2874133}, - abstract = {Numerical computation of transforms is now widely practiced in science and industry and has been revolutionized by the development of fast transforms that make feasible computing projects that once could not be contemplated. The article discusses the significance of transforms in numerical work, defines the modern forms of several common transforms and their inverses, gives examples, and describes and gives references to methods of numerical evaluation.}, - owner = {kohlbrecher}, - publisher = {American Association for the Advancement of Science}, - timestamp = {2016.11.08}, -} - -@Article{Kohlbrecher2017, - author = {Kohlbrecher, J. and Studer, A.}, - title = {{Transformation cycle between the spherically symmetric correlation function, projected correlation function and differential cross section as implemented in {\it SASfit}}}, - journal = {Journal of Applied Crystallography}, - year = {2017}, - volume = {50}, - number = {5}, - month = {Oct}, - pages = {1395--1403}, - doi = {10.1107/S1600576717011979}, - url = {https://doi.org/10.1107/S1600576717011979}, - abstract = {Spin-echo-based small-angle neutron scattering techniques like spin-echo SANS (SESANS) or spin-echo modulated SANS (SEMSANS) as well as dark-field (DF) imaging are directly sensitive to \tilde{G}(\delta), which is the projection of the scattering length density autocorrelation function \tilde{\gamma}(r). Here, a simplified transformation cycle relating the spherically symmetric correlation function \tilde{\gamma}(r), the projected correlation function \tilde{G}(\delta) and the macroscopic small-angle scattering cross section d{$\Sigma$}/d{$\Omega$} is introduced. The suggested changes to the cycle make it easier to include size distribution on an absolute scale if the data from the different techniques are fitted simultaneously. As up to now only very few analytical expressions for the projected correlation function are known, a numerical transformation of known scattering functions into the projected correlation function in the {\it SASfit} software package is supplied. Furthermore, a new analytical expression for the projected correlation function for polymers that can be described by the generalized Gaussian coil model is provided. For this polymer model, the Hankel transform used to calculate \tilde{G}(0) from the SANS signal is divergent for a certain parameter range describing a polymer in a good solvent and finite in the case of a poor solvent. It is therefore a suitable example of how the experimentally available {\it q} range can strongly influence the obtained results.}, - keywords = {spin-echo small-angle neutron scattering, small-angle neutron scattering, data analysis}, -} - -@Article{Lebedev2003, - author = {Lebedev, D.V. and Baitin, D.M. and Islamov, A.Kh. and Kuklin, A.I. and Shalguev, V.Kh. and Lanzov, V.A. and Isaev-Ivanov, V.V.}, - title = {Analytical model for determination of parameters of helical structures in solution by small angle scattering: comparison of RecA structures by SANS}, - journal = {FEBS Letters}, - year = {2003}, - volume = {537}, - number = {1-3}, - pages = {182--186}, - issn = {1873-3468}, - doi = {10.1016/S0014-5793(03)00107-8}, - url = {http://dx.doi.org/10.1016/S0014-5793(03)00107-8}, - abstract = {The filament structures of the self-polymers of RecA proteins from Escherichia coli and Pseudomonas aeruginosa, their complexes with ATP?S, phage M13 single-stranded DNA (ssDNA) and the tertiary complexes RecA::ATP?S::ssDNA were compared by small angle neutron scattering. A model was developed that allowed for an analytical solution for small angle scattering on a long helical filament, making it possible to obtain the helical pitch and the mean diameter of the protein filament from the scattering curves. The results suggest that the structure of the filaments formed by these two RecA proteins, and particularly their complexes with ATP?S, is conservative.}, - keywords = {RecA protein, Small angle neutron scattering, Homologous recombination, Pseudomonas aeruginosa, SANS, small angle neutron scattering, ssDNA, single-stranded DNA, dsDNA, double-stranded DNA}, -} - -@Article{Pringle1971, - author = {Pringle, O. A. and Schmidt, P. W.}, - title = {{Small-angle X-ray scattering from helical macromolecules}}, - journal = {Journal of Applied Crystallography}, - year = {1971}, - volume = {4}, - number = {4}, - month = {Aug}, - pages = {290--293}, - doi = {10.1107/S002188987100699X}, - url = {https://doi.org/10.1107/S002188987100699X}, - abstract = {An earlier calculation of the intensity of small-angle X-ray scattering from helical filaments is extended to give an expression for the intensity from helical macromolecules with a finite cross section. The results are in quite good agreement with an experimental scattering curve for a solution of DNA molecules.}, -} - -@Article{Schmidt1970, - author = {Schmidt, P. W.}, - title = {{Small angle X-ray scattering from helical filaments}}, - journal = {Journal of Applied Crystallography}, - year = {1970}, - volume = {3}, - number = {4}, - month = {Aug}, - pages = {257--264}, - doi = {10.1107/S0021889870006155}, - url = {https://doi.org/10.1107/S0021889870006155}, - abstract = {The intensity of small angle X-ray scattering has been calculated for a dilute suspension of identical, randomly oriented particles composed of two rigid coaxial helical filaments with negligible cross section and uniform electron density. The scattering is also computed for particles consisting of a single helix. Numerical calculations have been made for several values of the helix parameters. A series of intensity curves illustrates the effect of these parameters on the scattered intensity. The calculated intensities can be used in analysis of scattering data from suspensions of helical macromolecules.}, -} - -@Article{Teixeira2010, - author = {Teixeira, Cil{\^{a}}ine V. and Amenitsch, Heinz and Fukushima, Takanori and Hill, Jonathan P. and Jin, Wusong and Aida, Takuso and Hotokka, Matti and Lind{\'{e}}n, Mika}, - title = {{Form factor of an {\it N}-layered helical tape and its application to nanotube formation of hexa-{\it peri}-hexabenzocoronene-based molecules}}, - journal = {Journal of Applied Crystallography}, - year = {2010}, - volume = {43}, - number = {4}, - month = {Aug}, - pages = {850--857}, - doi = {10.1107/S0021889810015736}, - url = {https://doi.org/10.1107/S0021889810015736}, - abstract = {Self-assembled helical supramolecular structures are widely found in nature and have also been observed in several systems based on synthetic amphiphiles. Such structures often exhibit interesting properties that can be utilized in different nanotechnological applications. Based on previous work concerning the form factor of helical filaments with a finite cross section, the present work gives the helical form factor generalized for a tape containing {\it N} layers. The presented form factor is applied to the characterization of an intermediate structure obtained during the formation of self-assembled graphitic nanotubes. The structure was modeled as a centrosymmetric bilayer containing five layers including a structure factor. These results have been compared with that obtained using a model based on polydisperse cylinders, and it is shown that the full description with helical model and structure factor is the superior one.}, - keywords = {small-angle scattering, helix form factor, hexagonal order structure factor, nanotubes}, -} - -@Article{Avdeev2013, - author = {Avdeev, Mikhail V. and Aksenov, Victor L. and Gazov{\'{a}}, Zuzana and Alm{\'{a}}sy, L{\'{a}}szl{\'{o}} and Petrenko, Viktor I. and Gojzewski, Hubert and Feoktystov, Artem V. and Siposova, Katarina and Antosova, Andrea and Timko, Milan and Kopcansky, Peter}, - title = {{On the determination of the helical structure parameters of amyloid protofilaments by small-angle neutron scattering and atomic force microscopy}}, - journal = {Journal of Applied Crystallography}, - year = {2013}, - volume = {46}, - number = {1}, - month = {Feb}, - pages = {224--233}, - doi = {10.1107/S0021889812050042}, - url = {https://doi.org/10.1107/S0021889812050042}, - abstract = {The helical structure of amyloid protofilaments of hen egg white lysozyme was analyzed by small-angle neutron scattering (SANS) and atomic force microscopy (AFM). The structure of these formations in bulk solutions was adequately described by SANS in terms of a simplified model of a helix with spherical structural units. The found main helix parameters (pitch and effective diameter) are consistent with the results of AFM analysis for amyloid fibrils adsorbed on a mica surface. Both methods reveal a strong isotope effect on the structure of amyloid fibrils with respect to the substitution of heavy for light water in the solvent. Specific details responsible for the structural differences when comparing SANS and AFM data are discussed from the viewpoint of methodological aspects, the influence of different (native and adsorbed) amyloid states and sample preparation.}, - keywords = {small-angle neutron scattering, atomic force microscopy, helical structures, amyloid fibrils, hen egg white lysozyme}, -} - -@Article{Fukuda2002, - author = {Hiroshi Fukuda and Ayako Goto and Toyoko Imae}, - title = {Structure Determination of Helical Fibers by Numerical Simulation for Small-Angle Neutron Scattering{\textdagger}}, - journal = {Langmuir}, - year = {2002}, - volume = {18}, - number = {19}, - month = {sep}, - pages = {7107--7114}, - doi = {10.1021/la025528r}, - url = {10.1021/la025528r}, - publisher = {American Chemical Society ({ACS})}, -} - -@Article{Franklin1956, - author = {Rosalind E. Franklin and A. Klug}, - title = {The nature of the helical groove on the tobacco mosaic virus particle X-ray diffraction studies}, - journal = {Biochimica et Biophysica Acta}, - year = {1956}, - volume = {19}, - number = {Supplement C}, - pages = {403 - 416}, - issn = {0006-3002}, - doi = {https://doi.org/10.1016/0006-3002(56)90463-2}, - url = {http://www.sciencedirect.com/science/article/pii/0006300256904632}, - abstract = {Abstract It is shown that various aspects of the X-ray fibre-diagrams of TMV can be explained by the presence of some form of helical groove (with its resulting helical ridge) on the surface of the virus particle. The groove follows the line of the main protein helix (pitch 23 A) and is approximately 30 A in depth. The form of the groove and ridge is such as to permit a high degree of interlocking between neighbouring particles, and it is suggested that the ridge may in fact consist of a series of protuberances, one corresponding to each protein sub-unit. As a result, the surface area of the virus particle must be considerably greater than that of a smooth cylinder of the same diameter, and this may be important in determining the chemical properties of the intact virus.Résumé Les auteurs montrent que différents aspects des diagrammes de fibre aux rayons X du TMV peuvent s'expliquer par la présence d'une certaine forme de rainure hélicoïdale (avec sa crête hélicoïdale résultante) à la surface de la particule de virus. La rainure suit la ligne de l'hélice protéique principale (pas 23 A) et a une profondeur de 30 A environ. La forme de la rainure et de la crête est telle qu'elle permet un degré élevé d'interpénétration entre particules voisines, et les auteurs suggèrent que la crête peut en fait être constituée d'une série de protubérances, chacune correspondant à une sub-unité protéique. Il en résulte que l'aire de la surface de la particule de virus doit être considérablement plus grande que celle d'un cylindre lisse de même diamètre; cette conformation oeut jouer un róle important dans la détermination des propriétés chimiques du virus intact.Zusammenfassung Es wird bewiesen, dass verschiedene Aspekte der TMV-Röntgen-Faserdiagramme durch die Anwesenheit einer Art von Schraubenrinne (mit der sich daraus ergebenden Schraubenkannte) auf der Viruspartikeloberfläche erklärt werden können. Die Rinne folgt der Linie der Haupt-proteinschraube (Steighöle 23 A); ihre Tiefe ist ungefähr 30 A. Die Form von Rinne und Kante ermöglicht einen hohen Verflechtungsgrad der Nachbarpartikeln; die Annahme wird befürwortet, dass die Kante aus einer Reihe von Auswüchsen bestehen könnte, deren jeder einer Proteinsubeinheit entsprechen würde. Die Viruspartikeloberfläche muss daher bedeutend grösser sein als diejenige eines glatten Zylinders mit dem gleichen Durchmesser. Dies kann bei Bestimmung der chemischen Eigenschaften des intakten Virus von Wichtigkeit sein.}, -} - -@Article{Cochran1952, - author = {Cochran, W. and Crick, F. H. and Vand, V.}, - title = {{The structure of synthetic polypeptides. I. The transform of atoms on a helix}}, - journal = {Acta Crystallographica}, - year = {1952}, - volume = {5}, - number = {5}, - month = {Sep}, - pages = {581--586}, - doi = {10.1107/S0365110X52001635}, - url = {https://doi.org/10.1107/S0365110X52001635}, -} - -@Article{Puigjaner1974, - author = {Puigjaner, L. C. and Subirana, J. A.}, - title = {{Low-angle X-ray scattering by disordered and partially ordered helical systems}}, - journal = {Journal of Applied Crystallography}, - year = {1974}, - volume = {7}, - number = {2}, - month = {Apr}, - pages = {169--173}, - doi = {10.1107/S002188987400906X}, - url = {https://doi.org/10.1107/S002188987400906X}, - abstract = {A model has been developed to calculate the diffraction given by a disordered set of thick coils of helical conformation. Double coils placed inside a cylinder of different density are considered. The cylinder accounts for the presence of substances which may interact with the double coil in a random manner. The thickness of each coil, pitch and radius of gyration, outer cylinder diameter and its density are the parameters that influence the diffraction maxima observed. It is demonstrated that when the parameter {\it Z} (pitch/radius) increases, the peaks tend to overlap. The relative position ({$\alpha$}) of the two coils is also studied. When they are diametrically opposed, only even layer-line peaks are detected. At intermediate positions, other peaks appear, the intensity of which depends strongly on the precise value of {$\alpha$}. An interesting result is that the relative position of the peaks for any single coil is constant and does not depend on the dimensions of the coil. The central scattering increases considerably if one of the two-component coils becomes a straight cylinder coaxial with the primitive coil. As a result the lower layer-line peaks do not show. On the other hand, the intensity due to the central equatorial peak diminishes when some packing order is introduced between coils. The model is suitable for interpreting the specific case of nucleohistone patterns.}, -} - -@Article{Benham1980, - author = {C.J. Benham and G.W. Brady and D.B. Fein}, - title = {X-ray scattering from randomly oriented superhelices. Circular superhelical {DNA}}, - journal = {Biophysical Journal}, - year = {1980}, - volume = {29}, - number = {3}, - month = {mar}, - pages = {351--366}, - doi = {10.1016/S0006-3495(80)85139-3}, - publisher = {Elsevier {BV}}, -} - -@Article{Crick1953, - author = {Crick, F. H. C.}, - title = {{The Fourier transform of a coiled-coil}}, - journal = {Acta Crystallographica}, - year = {1953}, - volume = {6}, - number = {8-9}, - month = {Sep}, - pages = {685--689}, - doi = {10.1107/S0365110X53001952}, - url = {https://doi.org/10.1107/S0365110X53001952}, -} - -@Article{Nayuk2012, - author = {Roman Nayuk and Klaus Huber}, - title = {Formfactors of Hollow and Massive Rectangular Parallelepipeds at Variable Degree of Anisometry}, - journal = {Zeitschrift für Physikalische Chemie}, - year = {2012}, - volume = {226}, - number = {7-8}, - month = {aug}, - pages = {837--854}, - doi = {10.1524/zpch.2012.0257}, - publisher = {Walter de Gruyter {GmbH}}, -} - -@Article{, - author = {P. Mittelbach and G. Porod}, - title = {Small-Angle X-Ray Scattering by Dilute Colloid Systems. The Calculation of Scattering Curves for Parallelepipeds}, - journal = {Acta Phys. Austriaca}, - year = {1961}, - volume = {14}, - pages = {185-211}, -} - -@Article{Burchard1970, - author = {W. Burchard and K. Kajiwara}, - title = {The statistics of stiff chain molecules I. The particle scattering factor}, - journal = {Proceedings of the Royal Society of London A: Mathematical, Physical and Engineering Sciences}, - year = {1970}, - volume = {316}, - number = {1525}, - month = {apr}, - pages = {185--199}, - issn = {0080-4630}, - doi = {10.1098/rspa.1970.0074}, - eprint = {http://rspa.royalsocietypublishing.org/content/316/1525/185.full.pdf}, - url = {http://rspa.royalsocietypublishing.org/content/316/1525/185}, - abstract = {Analytic expressions for the particle scattering factor of stiff chains have been derived, both for the wormlike and a discrete chain model with an axial symmetric potential of hindered rotation. The angular distribution functions agree well with the results of Monte Carlo calculations by Heine, Kratky \& Roeppert (1962), if the chains are longer than five persistence lengths. The particle scattering factor of short chains can be well represented by the simple Guinier approximation. A transition point from the behaviour of a coil to that of the rod-like short chain sections has been determined by graphical extrapolation and appears at Xa = 2.87 {\textpm} 0.05. The difference between the wormlike and the discrete chain models turned out to be smaller than 14\% even for an alkane type chain with free rotation of the chain elements and decreases with increasing chain stiffness. The influence of the cross-section has been taken into account by representing the chain by a pearl necklace. Comparison with X -ray small angle scattering measurements of a cellulosetricarbanilate reveals close similarities between calculated and experimental curves.}, - publisher = {The Royal Society}, - timestamp = {2017-12-21}, -} - -@Article{Schweins2004, - author = {Ralf Schweins and Klaus Huber}, - title = {Particle scattering factor of pearl necklace chains}, - journal = {Macromolecular Symposia}, - year = {2004}, - volume = {211}, - number = {1}, - month = {apr}, - pages = {25--42}, - doi = {10.1002/masy.200450702}, - publisher = {Wiley-Blackwell}, - timestamp = {2017-12-21}, -} - -@Article{Giehm2010, - author = {Lise Giehm and Cristiano Luis Pinto Oliveira and Gunna Christiansen and Jan Skov Pedersen and Daniel E. Otzen}, - title = {{SDS}-Induced Fibrillation of $\alpha$-Synuclein: An Alternative Fibrillation Pathway}, - journal = {Journal of Molecular Biology}, - year = {2010}, - volume = {401}, - number = {1}, - month = {aug}, - pages = {115--133}, - doi = {10.1016/j.jmb.2010.05.060}, - publisher = {Elsevier {BV}}, - timestamp = {2017-12-21}, -} - -@Article{Kuhn1934, - author = {Kuhn, Werner}, - title = {{\"U}ber die Gestalt fadenf{\"o}rmiger Molek{\"u}le in L{\"o}sungen}, - journal = {Kolloid-Zeitschrift}, - year = {1934}, - volume = {68}, - number = {1}, - month = {Feb}, - pages = {2--15}, - issn = {1435-1536}, - doi = {10.1007/BF01451681}, - url = {https://doi.org/10.1007/BF01451681}, - abstract = {Es werden statistische Betrachtungen angestellt betreffend die Form, welche kettenf{\"o}rmig gebaute Molek{\"u}le, welche in einer L{\"o}sung (oder im Gasraum) suspendiert sind, infolge der Valenzwinkelung und der freien Drehbarkeit annehmen k{\"o}nnen.}, - day = {01}, - timestamp = {2017-12-22}, -} - -@WWW{Johnson, - author = {Steven G. Johnson}, - title = {multi-dimensional adaptive integration (cubature) in C, https://github.com/stevengj/cubature}, - year = {2017}, - url = {https://github.com/stevengj/cubature}, - timestamp = {2018-03-05}, -} - -@Comment{jabref-meta: databaseType:biblatex;} diff --git a/doc/manual/sasfit.log b/doc/manual/sasfit.log index 3aca830f..d4806f2e 100644 --- a/doc/manual/sasfit.log +++ b/doc/manual/sasfit.log @@ -1,4 +1,4 @@ -This is pdfTeX, Version 3.1415926-2.3-1.40.12 (MiKTeX 2.9) (preloaded format=pdflatex 2011.6.14) 12 MAR 2018 10:19 +This is pdfTeX, Version 3.1415926-2.3-1.40.12 (MiKTeX 2.9) (preloaded format=pdflatex 2011.6.14) 19 MAR 2018 14:58 entering extended mode **sasfit.tex (C:\user\SASfitGit\doc\manual\sasfit.tex @@ -6498,70 +6498,97 @@ Package pdftex.def Info: ../images/form_factor/Ellipsoid/ellipsoidalShell.png u sed on input line 153. 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(pdftex.def) Requested size: 380.91402pt x 180.32927pt. -)) [476] [477 ] (C:\user\SAS -fitGit\doc\manual\SASfit_absInt.tex [478 +)) [478] [479 ] (C:\user\SAS +fitGit\doc\manual\SASfit_absInt.tex [480 @@ -7277,7 +7304,7 @@ Chapter 11 LaTeX Warning: Command \r invalid in math mode on input line 29. -[479] [480] +[481] [482] Underfull \hbox (badness 2277) in paragraph at lines 169--169 [][]\OT1/cmr/m/n/10 Definition of uni-fied atomic mass unit: $1u = \OML/cmm/m/i t/10 m[] \OT1/cmr/m/n/10 = \OML/cmm/m/it/10 m [] =\OT1/cmr/m/n/10 12 = 1\OML/cm @@ -7290,11 +7317,11 @@ Overfull \hbox (49.65741pt too wide) has occurred while \output is active VOLUME - ABSOLUTE SCALE [] [] -[481] [482] +[483] [484] Underfull \vbox (badness 10000) has occurred while \output is active [] - [483] - + [485] + File: QTintegralparameterGUI.png Graphic file (type png) @@ -7314,7 +7341,7 @@ Underfull \hbox (badness 10000) in paragraph at lines 301--302 [] -[484] +[486] File: QTmoments.png Graphic file (type png) Package pdftex.def Info: QTmoments.png used on input line 330. @@ -7322,16 +7349,16 @@ Package pdftex.def Info: QTmoments.png used on input line 330. Underfull \vbox (badness 1127) has occurred while \output is active [] - [485 ] [486 ]) [487] [488] + [487 ] [488 ]) [489] [490] (C:\user\SASfitGit\doc\manual\SASfit_DLS.tex Chapter 12 -[489 +[491 -] [490] [491] [492]) [493] (C:\user\SASfitGit\doc\manual\basics.tex -[494 +] [492] [493] [494]) [495] (C:\user\SASfitGit\doc\manual\basics.tex +[496 @@ -7340,13 +7367,13 @@ Chapter 13 LaTeX Warning: Command \b invalid in math mode on input line 12. - + File: EwaldSphereTeX.png Graphic file (type png) Package pdftex.def Info: EwaldSphereTeX.png used on input line 18. (pdftex.def) Requested size: 403.29497pt x 201.64969pt. - [495 ] + [497 ] LaTeX Warning: Command \b invalid in math mode on input line 68. @@ -7392,7 +7419,7 @@ LaTeX Warning: Command \b invalid in math mode on input line 94. 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(pdftex.def) Requested size: 215.1114pt x 268.88329pt. - [511 ] [512] [513]) (C:\user\SASfitGit\doc\manual\DatenRed.tex [514] + [513 ] [514] [515]) (C:\user\SASfitGit\doc\manual\DatenRed.tex [516] Chapter 14 - + File: SANSAN.png Graphic file (type png) Package pdftex.def Info: SANSAN.png used on input line 5. (pdftex.def) Requested size: 448.12378pt x 280.95203pt. - + File: CJUSIFA.png Graphic file (type png) Package pdftex.def Info: CJUSIFA.png used on input line 14. (pdftex.def) Requested size: 448.12239pt x 267.99065pt. - [515 + [517 - ] [516 ] [518 ] Chapter 15 -[517 +[519 -] [518]) [519] (C:\user\SASfitGit\doc\manual\SASfit_history.tex +] [520]) [521] (C:\user\SASfitGit\doc\manual\SASfit_history.tex Underfull \vbox (badness 10000) has occurred while \output is active [] - [520 + [522 ] Missing character: There is no à in font cmr12! Missing character: There is no ¶ in font cmr12! -[521] -Underfull \hbox (badness 1817) in paragraph at lines 142--144 +[523] [524] +Underfull \hbox (badness 1817) in paragraph at lines 147--149 []\OT1/cmr/m/n/12 new plu-gin for \OT1/cmtt/m/n/12 generalized Guinier law \OT1 /cmr/m/n/12 to be found un-der \OT1/cmtt/m/n/12 [by [] -[522] -Underfull \hbox (badness 4403) in paragraph at lines 160--162 + +Underfull \hbox (badness 4403) in paragraph at lines 165--167 []\OT1/cmr/m/n/12 included un-der peak func-tion the \OT1/cmtt/m/n/12 Maxwell \ OT1/cmr/m/n/12 dis-tri-bu-tion and the [] -Underfull \hbox (badness 1881) in paragraph at lines 177--179 +Underfull \hbox (badness 1881) in paragraph at lines 182--184 []\OT1/cmr/m/n/12 added con-fig-u-ra-tion file \OT1/cmtt/m/n/12 config.ini \OT1 /cmr/m/n/12 as re-place-ment for dep-re-cated [] -[523] [524] -Underfull \hbox (badness 1924) in paragraph at lines 243--250 + +Underfull \vbox (badness 10000) has occurred while \output is active [] + + [525] +[526] +Underfull \hbox (badness 1924) in paragraph at lines 248--255 \OT1/cmr/m/n/12 in Macro-molecules 1996, 29, 7602-7612. They have been im-ple- [] -[525] [526] -Underfull \hbox (badness 10000) in paragraph at lines 351--360 +[527] +Underfull \vbox (badness 10000) has occurred while \output is active [] + + [528] +Underfull \hbox (badness 10000) in paragraph at lines 356--365 []\OT1/cmr/m/n/12 (\OT1/cmtt/m/n/12 SASfit \OT1/cmr/m/n/12 ver-sion 0.84) Form fac-tor for worm-like mi-celles [] -Underfull \hbox (badness 4569) in paragraph at lines 351--360 +Underfull \hbox (badness 4569) in paragraph at lines 356--365 \OT1/cmr/m/n/12 clus-ter ag-gre-gates (\OT1/cmtt/m/n/12 Mass Fractal (Exp(-x) C ut-Off), Fisher-Burford, [] -Underfull \hbox (badness 10000) in paragraph at lines 351--360 +Underfull \hbox (badness 10000) in paragraph at lines 356--365 \OT1/cmtt/m/n/12 MassFractExp,MassFractGauss, Mass Fractal (Exp(-x$[]$a) Cut-Of f), [] -Underfull \hbox (badness 1552) in paragraph at lines 351--360 +Underfull \hbox (badness 1552) in paragraph at lines 356--365 \OT1/cmtt/m/n/12 DLCAggregation, RLCAggregation, MassFractOverlappingSph \OT1/c mr/m/n/12 have been [] -Underfull \hbox (badness 10000) in paragraph at lines 360--366 +Underfull \hbox (badness 10000) in paragraph at lines 365--371 []\OT1/cmr/m/n/12 (SPHERE+Chains(RW), SPHERE+Chains(RW)[]Rc, [] -Underfull \hbox (badness 1371) in paragraph at lines 360--366 +Underfull \hbox (badness 1371) in paragraph at lines 365--371 \OT1/cmr/m/n/12 SPHERE+Chains(RW)[]Nagg\OT1/cmtt/m/n/12 SASfit \OT1/cmr/m/n/12 ver-sion 0.80) Next to the cor-rec-tion [] -Underfull \hbox (badness 1199) in paragraph at lines 360--366 +Underfull \hbox (badness 1199) in paragraph at lines 365--371 \OT1/cmr/m/n/12 Fur-ther-more an op-tion has been im-ple-mented to sub-tract a the-o-ret-i-cal [] -Underfull \hbox (badness 10000) in paragraph at lines 366--380 +Underfull \hbox (badness 10000) in paragraph at lines 371--385 []\OT1/cmr/m/n/12 A cou-ple of form fac-tors for spher-i-cal, el-lip-ti-cal, cy lin- [] -Underfull \hbox (badness 5133) in paragraph at lines 366--380 +Underfull \hbox (badness 5133) in paragraph at lines 371--385 \OT1/cmr/m/n/12 dri-cal and very long rod-like mi-celles con-sist-ing of a ho-m o-ge-neous [] -Underfull \hbox (badness 3000) in paragraph at lines 366--380 +Underfull \hbox (badness 3000) in paragraph at lines 371--385 \OT1/cmr/m/n/12 core and which are ei-ther grafted with Gauss-ian chains \OT1/c mtt/m/n/12 *(RW)*\OT1/cmr/m/n/12 , or [] -Underfull \hbox (badness 2922) in paragraph at lines 366--380 +Underfull \hbox (badness 2922) in paragraph at lines 371--385 \OT1/cmr/m/n/12 grafted with semi-flexible self-avoiding and in-ter-act-ing cha ins \OT1/cmtt/m/n/12 *(SAW)* [] -Underfull \hbox (badness 4060) in paragraph at lines 366--380 +Underfull \hbox (badness 4060) in paragraph at lines 371--385 \OT1/cmr/m/n/12 or a corona with a power-law de-cay-ing pro-file $\OML/cmm/m/it /12 r[]$ \OT1/cmtt/m/n/12 *(R$[]$-a)* \OT1/cmr/m/n/12 have [] -Underfull \hbox (badness 10000) in paragraph at lines 366--380 +Underfull \hbox (badness 10000) in paragraph at lines 371--385 \OT1/cmr/m/n/12 been im-ple-mented: \OT1/cmtt/m/n/12 SPHERE+Chains(RW), SPHERE +Chains(RW)[]Rc, [] -Underfull \hbox (badness 10000) in paragraph at lines 366--380 +Underfull \hbox (badness 10000) in paragraph at lines 371--385 \OT1/cmtt/m/n/12 SPHERE+Chains(RW)[]Nagg, SPHERE+Chains(SAW), SPHERE+Chains(SAW )[]Rc, [] -Underfull \hbox (badness 10000) in paragraph at lines 366--380 +Underfull \hbox (badness 10000) in paragraph at lines 371--385 \OT1/cmtt/m/n/12 SPHERE+Chains(SAW)[]Nagg, SPHERE+R$[]$-a, SPHERE+R$[]$-a[]Rc, [] -Underfull \hbox (badness 10000) in paragraph at lines 366--380 +Underfull \hbox (badness 10000) in paragraph at lines 371--385 \OT1/cmtt/m/n/12 SPHERE+R$[]$-a[]Nagg, ELL+Chains(RW), ELL+Chains(RW)[]Rc, [] -Underfull \hbox (badness 10000) in paragraph at lines 366--380 +Underfull \hbox (badness 10000) in paragraph at lines 371--385 \OT1/cmtt/m/n/12 ELL+Chains(RW)[]Nagg, CYL+Chains(RW), CYL+Chains(RW)[]Rc, [] -Underfull \hbox (badness 10000) in paragraph at lines 366--380 +Underfull \hbox (badness 10000) in paragraph at lines 371--385 \OT1/cmtt/m/n/12 CYL+Chains(RW)[]Nagg, ROD+Chains(RW), ROD+Chains(RW)[]Rc, [] - -Underfull \hbox (badness 10000) in paragraph at lines 388--389 +[529] +Underfull \hbox (badness 10000) in paragraph at lines 393--394 []\OT1/cmr/m/n/12 Implementation of form fac-tors for bi-continuous sys-tems [] - -Underfull \vbox (badness 10000) has occurred while \output is active [] - - [527]) -(C:\user\SASfitGit\doc\manual\sasfit.bbl [528] +) (C:\user\SASfitGit\doc\manual\sasfit.bbl [530] Bibliography Missing character: There is no â in font cmr10! 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Ellipsoid with two equal equatorial semi-axis R and volume V}{section.1696}% 344 \BOOKMARK [2][-]{subsection.1712}{8.4.3. Ellipsoidal core shell structure}{section.1696}% 345 \BOOKMARK [2][-]{subsection.1717}{8.4.4. triaxial ellipsoidal core shell structure}{section.1696}% 346 -\BOOKMARK [1][-]{section.1723}{8.5. Cylindrical objects}{chapter.1472}% 347 -\BOOKMARK [2][-]{subsection.1724}{8.5.1. Helical structures}{section.1723}% 348 -\BOOKMARK [3][-]{subsubsection.1725}{8.5.1.1. Fanlike helix}{subsection.1724}% 349 -\BOOKMARK [3][-]{subsubsection.1735}{8.5.1.2. Helix with round cross-section}{subsection.1724}% 350 -\BOOKMARK [3][-]{subsubsection.1744}{8.5.1.3. Beads model of a single helical strand}{subsection.1724}% 351 -\BOOKMARK [3][-]{subsubsection.1755}{8.5.1.4. straight superhelix}{subsection.1724}% 352 -\BOOKMARK [3][-]{subsubsection.1763}{8.5.1.5. coiled superhelix}{subsection.1724}% 353 -\BOOKMARK [1][-]{section.1777}{8.6. 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LogNorm\137fp}{chapter.1936}% 374 -\BOOKMARK [0][-]{chapter.1949}{Chapter 10. Plugin functions for structure factors}{}% 375 -\BOOKMARK [1][-]{section.1950}{10.1. Structure factor of a random flight model}{chapter.1949}% 376 -\BOOKMARK [1][-]{section.1955}{10.2. ordered particle systems}{chapter.1949}% 377 -\BOOKMARK [2][-]{subsection.1968}{10.2.1. Domains of ordered particle systems isotropically oriented}{section.1955}% 378 -\BOOKMARK [2][-]{subsection.1996}{10.2.2. Domains of ordered particle systems with preferred orientation}{section.1955}% 379 -\BOOKMARK [0][-]{chapter.2001}{Chapter 11. Absolute intensities, moments and volume fractions}{}% 380 -\BOOKMARK [1][-]{section.2002}{11.1. Fitting absolute intensities}{chapter.2001}% 381 -\BOOKMARK [1][-]{section.2014}{11.2. Contrast - Concentration - Forward Scattering - Particle Volume - Absolute Scale}{chapter.2001}% 382 -\BOOKMARK [1][-]{section.2027}{11.3. 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Correction and normalization of SAXS raw data}{chapter.2188}% 422 -\BOOKMARK [0][-]{appendix*.2213}{Bibliography}{}% 423 +\BOOKMARK [1][-]{section.1724}{8.5. Cylindrical objects}{chapter.1472}% 347 +\BOOKMARK [2][-]{subsection.1725}{8.5.1. Helical structures}{section.1724}% 348 +\BOOKMARK [3][-]{subsubsection.1726}{8.5.1.1. Fanlike helix}{subsection.1725}% 349 +\BOOKMARK [3][-]{subsubsection.1736}{8.5.1.2. Helix with round cross-section}{subsection.1725}% 350 +\BOOKMARK [3][-]{subsubsection.1745}{8.5.1.3. Beads model of a single helical strand}{subsection.1725}% 351 +\BOOKMARK [3][-]{subsubsection.1756}{8.5.1.4. straight superhelix}{subsection.1725}% 352 +\BOOKMARK [3][-]{subsubsection.1764}{8.5.1.5. coiled superhelix}{subsection.1725}% 353 +\BOOKMARK [1][-]{section.1778}{8.6. Form factors of magnetic objects}{chapter.1472}% 354 +\BOOKMARK [2][-]{subsection.1779}{8.6.1. Magnetic spin misalignment}{section.1778}% 355 +\BOOKMARK [2][-]{subsection.1787}{8.6.2. Ferrofluids}{section.1778}% 356 +\BOOKMARK [2][-]{subsection.1802}{8.6.3. Langevin statistics for averages of the form factor and averages of the squared form factor}{section.1778}% 357 +\BOOKMARK [1][-]{section.1826}{8.7. Bi-continuous and non-particulate structures}{chapter.1472}% 358 +\BOOKMARK [2][-]{subsection.1827}{8.7.1. Teubner-Strey}{section.1826}% 359 +\BOOKMARK [2][-]{subsection.1845}{8.7.2. Debye-Anderson-Brumberger\(DAB\)}{section.1826}% 360 +\BOOKMARK [2][-]{subsection.1849}{8.7.3. Generalization of the Debye-Anderson-Brumberger model \(gDAB\)}{section.1826}% 361 +\BOOKMARK [2][-]{subsection.1853}{8.7.4. Spinodal}{section.1826}% 362 +\BOOKMARK [2][-]{subsection.1857}{8.7.5. OrnsteinZernike}{section.1826}% 363 +\BOOKMARK [2][-]{subsection.1860}{8.7.6. Broad-Peak}{section.1826}% 364 +\BOOKMARK [2][-]{subsection.1863}{8.7.7. generalized Guinier approximation Fratzl1994,Hjelm1992,Hjelm1995,Hjelm2000}{section.1826}% 365 +\BOOKMARK [2][-]{subsection.1867}{8.7.8. generalized Guinier-Porod law}{section.1826}% 366 +\BOOKMARK [1][-]{section.1874}{8.8. fractal size distribution of particles}{chapter.1472}% 367 +\BOOKMARK [1][-]{section.1894}{8.9. Plugin functions for SESANS}{chapter.1472}% 368 +\BOOKMARK [2][-]{subsection.1918}{8.9.1. G\(z\) of a sphere}{section.1894}% 369 +\BOOKMARK [1][-]{section.1922}{8.10. G\(z\) of a randomly distributed, two-phase system \(DAB\) }{chapter.1472}% 370 +\BOOKMARK [1][-]{section.1926}{8.11. G\(z\) of a self-affine random density distribution \(gDAB\) }{chapter.1472}% 371 +\BOOKMARK [1][-]{section.1930}{8.12. G\(z\) for a generalized Gaussian coil \(gGc\) }{chapter.1472}% 372 +\BOOKMARK [0][-]{chapter.1937}{Chapter 9. Plugin functions for size distributions}{}% 373 +\BOOKMARK [1][-]{section.1938}{9.1. LogNorm\137fp}{chapter.1937}% 374 +\BOOKMARK [0][-]{chapter.1950}{Chapter 10. Plugin functions for structure factors}{}% 375 +\BOOKMARK [1][-]{section.1951}{10.1. Structure factor of a random flight model}{chapter.1950}% 376 +\BOOKMARK [1][-]{section.1956}{10.2. ordered particle systems}{chapter.1950}% 377 +\BOOKMARK [2][-]{subsection.1969}{10.2.1. Domains of ordered particle systems isotropically oriented}{section.1956}% 378 +\BOOKMARK [2][-]{subsection.1997}{10.2.2. Domains of ordered particle systems with preferred orientation}{section.1956}% 379 +\BOOKMARK [0][-]{chapter.2002}{Chapter 11. Absolute intensities, moments and volume fractions}{}% 380 +\BOOKMARK [1][-]{section.2003}{11.1. Fitting absolute intensities}{chapter.2002}% 381 +\BOOKMARK [1][-]{section.2015}{11.2. Contrast - Concentration - Forward Scattering - Particle Volume - Absolute Scale}{chapter.2002}% 382 +\BOOKMARK [1][-]{section.2028}{11.3. Moments of scattering curves and size distribution}{chapter.2002}% 383 +\BOOKMARK [1][-]{section.2043}{11.4. Volume fractions}{chapter.2002}% 384 +\BOOKMARK [0][-]{chapter.2049}{Chapter 12. Basic Analysis of Dynamic Light Scattering Data}{}% 385 +\BOOKMARK [1][-]{section.2055}{12.1. Cumulant Analysis}{chapter.2049}% 386 +\BOOKMARK [1][-]{section.2060}{12.2. Double Decay Cumulant Analysis}{chapter.2049}% 387 +\BOOKMARK [1][-]{section.2062}{12.3. Fit of Double Stretched Exponentials}{chapter.2049}% 388 +\BOOKMARK [2][-]{subsection.2064}{12.3.1. The least squares minimiser and the robust least squares procedure}{section.2062}% 389 +\BOOKMARK [0][-]{chapter.2070}{Chapter 13. Scattering Theory}{}% 390 +\BOOKMARK [1][-]{section.2071}{13.1. Scattering Cross-Section}{chapter.2070}% 391 +\BOOKMARK [2][-]{subsection.2075}{13.1.1. Scattering of neutrons on atoms}{section.2071}% 392 +\BOOKMARK [3][-]{subsubsection.2085}{13.1.1.1. Nuclear scattering}{subsection.2075}% 393 +\BOOKMARK [3][-]{subsubsection.2090}{13.1.1.2. Magnetic Scattering}{subsection.2075}% 394 +\BOOKMARK [2][-]{subsection.2102}{13.1.2. Scattering of x-ray at atoms}{section.2071}% 395 +\BOOKMARK [3][-]{subsubsection.2110}{13.1.2.1. Anomalous scattering of x-rays}{subsection.2102}% 396 +\BOOKMARK [1][-]{section.2114}{13.2. Small angle scattering}{chapter.2070}% 397 +\BOOKMARK [2][-]{subsection.2121}{13.2.1. Autocorrelation function \(r\) and \(r\)}{section.2114}% 398 +\BOOKMARK [3][-]{subsubsection.2122}{13.2.1.1. Isotropic averages}{subsection.2121}% 399 +\BOOKMARK [3][-]{subsubsection.2126}{13.2.1.2. Absence of long range order}{subsection.2121}% 400 +\BOOKMARK [3][-]{subsubsection.2130}{13.2.1.3. Limits r=0 and r=}{subsection.2121}% 401 +\BOOKMARK [2][-]{subsection.2133}{13.2.2. Volume fraction}{section.2114}% 402 +\BOOKMARK [2][-]{subsection.2138}{13.2.3. Interparticle interferences}{section.2114}% 403 +\BOOKMARK [3][-]{subsubsection.2144}{13.2.3.1. Isotropic ensemble of particles}{subsection.2138}% 404 +\BOOKMARK [2][-]{subsection.2146}{13.2.4. Influence of the relative arrangement of scatterers on interparticle interferences}{section.2114}% 405 +\BOOKMARK [3][-]{subsubsection.2152}{13.2.4.1. Formula from Prins and Zernicke}{subsection.2146}% 406 +\BOOKMARK [3][-]{subsubsection.2157}{13.2.4.2. Isolate particles}{subsection.2146}% 407 +\BOOKMARK [3][-]{subsubsection.2159}{13.2.4.3. Polydisperse System of isolated particles}{subsection.2146}% 408 +\BOOKMARK [2][-]{subsection.2161}{13.2.5. Influence of N\(R\) and F\(Q,R\) on interparticle interferences}{section.2114}% 409 +\BOOKMARK [2][-]{subsection.2166}{13.2.6. Scattering laws and structural parameter}{section.2114}% 410 +\BOOKMARK [3][-]{subsubsection.2167}{13.2.6.1. Porod volume}{subsection.2166}% 411 +\BOOKMARK [3][-]{subsubsection.2169}{13.2.6.2. Radius of gyration and Guinier approximation}{subsection.2166}% 412 +\BOOKMARK [3][-]{subsubsection.2173}{13.2.6.3. Correlation length}{subsection.2166}% 413 +\BOOKMARK [3][-]{subsubsection.2176}{13.2.6.4. Porod law and specific surfaces}{subsection.2166}% 414 +\BOOKMARK [0][-]{chapter.2184}{Chapter 14. Experimental Setup of a Small Angle Scattering Instrument}{}% 415 +\BOOKMARK [1][-]{section.2185}{14.1. SANS-Camera}{chapter.2184}% 416 +\BOOKMARK [1][-]{section.2187}{14.2. SAXS-Camera}{chapter.2184}% 417 +\BOOKMARK [0][-]{chapter.2189}{Chapter 15. Data Reduction in SAS}{}% 418 +\BOOKMARK [1][-]{section.2190}{15.1. Correction and Normalization of SANS-Raw data}{chapter.2189}% 419 +\BOOKMARK [2][-]{subsection.2194}{15.1.1. Contribution of the isolated sample}{section.2190}% 420 +\BOOKMARK [2][-]{subsection.2198}{15.1.2. Correction for sample holder and background noise}{section.2190}% 421 +\BOOKMARK [1][-]{section.2203}{15.2. Correction and normalization of SAXS raw data}{chapter.2189}% 422 +\BOOKMARK [0][-]{appendix*.2214}{Bibliography}{}% 423 diff --git a/doc/manual/sasfit.pdf b/doc/manual/sasfit.pdf index 18066621..71026766 100644 Binary files a/doc/manual/sasfit.pdf and b/doc/manual/sasfit.pdf differ diff --git a/doc/manual/sasfit.synctex b/doc/manual/sasfit.synctex index 55edd0c9..68a1f03d 100644 --- a/doc/manual/sasfit.synctex +++ b/doc/manual/sasfit.synctex @@ -348071,44 +348071,44 @@ h182,147:3263189,49769386:29368709,0,0 }416 !12 {417 -(182,183:4736286,49769386:31158801,45033100,0 -[182,183:4736286,49769386:31158801,45033100,0 -[182,183:4736286,4736286:0,0,0 -(182,183:4736286,2190005:0,0,0 -k182,183:4736286,2190005:-1724311 -) -] -[182,183:4736286,49769386:31158801,45033100,0 -h182,183:4736286,4736286:0,0,0 -[182,183:6526378,49769386:29368709,47513600,0 -[182,183:6526378,3238826:29368709,983040,0 -(182,183:6526378,3238826:29368709,403045,0 -(182,183:6526378,3238826:29368709,403045,0 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interparticle interferences}}{512}{subsection.2161} +\contentsline {subsection}{\tocsubsection {}{13.2.6}{Scattering laws and structural parameter}}{513}{subsection.2166} +\contentsline {subsubsection}{\tocsubsubsection {}{13.2.6.1}{Porod volume}}{514}{subsubsection.2167} +\contentsline {subsubsection}{\tocsubsubsection {}{13.2.6.2}{Radius of gyration and Guinier approximation}}{514}{subsubsection.2169} +\contentsline {subsubsection}{\tocsubsubsection {}{13.2.6.3}{Correlation length}}{514}{subsubsection.2173} +\contentsline {subsubsection}{\tocsubsubsection {}{13.2.6.4}{Porod law and specific surfaces}}{515}{subsubsection.2176} +\contentsline {chapter}{\tocchapter {Chapter}{14}{Experimental Setup of a Small Angle Scattering Instrument}}{517}{chapter.2184} +\contentsline {section}{\tocsection {}{14.1}{SANS-Camera}}{517}{section.2185} +\contentsline {section}{\tocsection {}{14.2}{SAXS-Camera}}{517}{section.2187} +\contentsline {chapter}{\tocchapter {Chapter}{15}{Data Reduction in SAS}}{519}{chapter.2189} +\contentsline {section}{\tocsection {}{15.1}{Correction and Normalization of SANS-Raw data}}{519}{section.2190} +\contentsline {subsection}{\tocsubsection {}{15.1.1}{Contribution of the isolated sample}}{519}{subsection.2194} +\contentsline {subsection}{\tocsubsection {}{15.1.2}{Correction for sample holder and background noise}}{520}{subsection.2198} +\contentsline {section}{\tocsection {}{15.2}{Correction and normalization of SAXS raw data}}{521}{section.2203} +\contentsline {chapter}{\tocappendix {Appendix}{}{Bibliography}}{531}{appendix*.2214} diff --git a/src/Doxyfile b/src/Doxyfile index d28fd4ab..72abfed7 100644 --- a/src/Doxyfile +++ b/src/Doxyfile @@ -1,1894 +1,1894 @@ -# Doxyfile 1.8.3.1 - -# This file describes the settings to be used by the documentation system -# doxygen (www.doxygen.org) for a project -# -# All text after a hash (#) is considered a comment and will be ignored -# The format is: -# TAG = value [value, ...] -# For lists items can 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This can be useful if your file system -# doesn't support long names like on DOS, Mac, or CD-ROM. - -SHORT_NAMES = NO - -# If the JAVADOC_AUTOBRIEF tag is set to YES then Doxygen -# will interpret the first line (until the first dot) of a JavaDoc-style -# comment as the brief description. If set to NO, the JavaDoc -# comments will behave just like regular Qt-style comments -# (thus requiring an explicit @brief command for a brief description.) - -JAVADOC_AUTOBRIEF = YES - -# If the QT_AUTOBRIEF tag is set to YES then Doxygen will -# interpret the first line (until the first dot) of a Qt-style -# comment as the brief description. If set to NO, the comments -# will behave just like regular Qt-style comments (thus requiring -# an explicit \brief command for a brief description.) - -QT_AUTOBRIEF = NO - -# The MULTILINE_CPP_IS_BRIEF tag can be set to YES to make Doxygen -# treat a multi-line C++ special comment block (i.e. a block of //! or /// -# comments) as a brief description. This used to be the default behaviour. -# The new default is to treat a multi-line C++ comment block as a detailed -# description. Set this tag to YES if you prefer the old behaviour instead. - -MULTILINE_CPP_IS_BRIEF = NO - -# If the INHERIT_DOCS tag is set to YES (the default) then an undocumented -# member inherits the documentation from any documented member that it -# re-implements. - -INHERIT_DOCS = YES - -# If the SEPARATE_MEMBER_PAGES tag is set to YES, then doxygen will produce -# a new page for each member. If set to NO, the documentation of a member will -# be part of the file/class/namespace that contains it. - -SEPARATE_MEMBER_PAGES = NO - -# The TAB_SIZE tag can be used to set the number of spaces in a tab. -# Doxygen uses this value to replace tabs by spaces in code fragments. - -TAB_SIZE = 8 - -# This tag can be used to specify a number of aliases that acts -# as commands in the documentation. An alias has the form "name=value". -# For example adding "sideeffect=\par Side Effects:\n" will allow you to -# put the command \sideeffect (or @sideeffect) in the documentation, which -# will result in a user-defined paragraph with heading "Side Effects:". -# You can put \n's in the value part of an alias to insert newlines. - -ALIASES = "modname{1}=\note The module group name is '\1' (used for plugin group membership)." \ - "toplvldescr{3}=
All \1 functions are of type \ref sasfit_func_one_t : \param q The current data point of the scattering vector. \param p Pointer to a \ref sasfit_param structure containing an array of parameter values.
The order is defined by each \1 function itself.
See its documentation (plugins) or implementation (old style) to get clarity about that. \returns The value of the \1 for the scattering vector value q. \see \ref howto_use_old \modname{\3}" \ - "vs=Microsoft Visual Studio 2005" \ - "vs_select_rel=Select 'Release' mode for this project in the symbol bar at the top." \ - "vs_build=Right-Click on the project in the solution explorer and select \e Build or \e Rebuild." \ - "vs_new_proj=Create a new project (console application) using the existing source code in \\examples. ('File' -> 'New' -> 'Project From Existing Code').\n Choose a project name and a project file location. On the next form, select 'Use Visual Studio' and 'Console application project'. When done, press 'finish' to quit this dialog." \ - "vs_select_file{1}=\vs_select_rel\n In the solution explorer, make sure that just \1 is part of it: Remove all additional files (Right-click on them and select 'Exclude From Project'). Then, right-click on the project itself and select 'Properties'." \ - "vs_add_inc{2}=In the left subwindow select 'Configuration Properties'->'C/C++'->'General'.\n Edit the entry 'Additional Include Directories' within the right subwindow: It's supposed to be empty. Add the following directories:
    \1
\2\n" \ - "vs_add_lib{2}=In the next step, select 'Configuration Properties'->'Linker'->'General' from the left subwindow and modify the entry 'Additional Library Directories' by adding
    \1
\2\n (\vs needs \e *.lib files for building, not runtime \e *.dll files)" \ - "vs_add_deps{1}=Additionally, you have to modify the entry 'Additional Dependencies' by selecting 'Configuration Properties'->'Linker'->'Input' on the left side. Enter the following library file names:
    \1
\n" \ - "vs_do_build{1}=Next, close the properties window and \vs_build When there were no errors, directory \1 (or the previously selected project file location) should contain an executable with the name of the project as listed in the solution explorer." \ - "vs_redistrib_note=On Windows systems where no \vs is installed, you also need to have the redistributable files in PATH. For sasfit they are: 'Microsoft.VC80.CRT.manifest' and 'msvcr80.dll' (if build with \vs). They are located in \vs-install-dir\\VC\\redist\\x86\\Microsoft.VC80.CRT ." \ - "win_lib_path{1}=To run this program, \1 is required. The easiest method for testing is to copy it into the same directory where the executable resides. \n Alternatively, you could add its path \sf_src\\src\\lib\\ to your systems 'PATH' environment variable or copy the library file to one of the directories in PATH. Execute echo \%PATH\% on the command prompt to see what those directories are. \n" \ - "memberof{1}=" \ - "sf_src=" \ - "sf_grp_def=groups.*.def in \sf_src/src/plugins" \ - "sf=SASfit" \ - "pb{1}=\" \ - "pn=\pb{next}" \ - "qt{1}="\1"" \ - "path{1}=\1" \ - "lnk{2}=\1" \ - "build_results{3}=If everything went fine, there is a shared (*.\1) and eventually a static (*.\2) library file in \n\n \sf_src\3src\3lib. \n\n The shared library file is copied to \n\n \sf_src\3sasfit.vfs\3lib\3Sasfit \n\n automatically (for starpack creation). In addition, each library file of a plugin as well as its public header file is automatically copied to \n\n \sf_src\3plugins. \n\n" - -# This tag can be used to specify a number of word-keyword mappings (TCL only). -# A mapping has the form "name=value". For example adding -# "class=itcl::class" will allow you to use the command class in the -# itcl::class meaning. - -TCL_SUBST = - -# Set the OPTIMIZE_OUTPUT_FOR_C tag to YES if your project consists of C -# sources only. Doxygen will then generate output that is more tailored for C. -# For instance, some of the names that are used will be different. The list -# of all members will be omitted, etc. - -OPTIMIZE_OUTPUT_FOR_C = YES - -# Set the OPTIMIZE_OUTPUT_JAVA tag to YES if your project consists of Java -# sources only. Doxygen will then generate output that is more tailored for -# Java. For instance, namespaces will be presented as packages, qualified -# scopes will look different, etc. - -OPTIMIZE_OUTPUT_JAVA = NO - -# Set the OPTIMIZE_FOR_FORTRAN tag to YES if your project consists of Fortran -# sources only. Doxygen will then generate output that is more tailored for -# Fortran. - -OPTIMIZE_FOR_FORTRAN = NO - -# Set the OPTIMIZE_OUTPUT_VHDL tag to YES if your project consists of VHDL -# sources. Doxygen will then generate output that is tailored for -# VHDL. - -OPTIMIZE_OUTPUT_VHDL = NO - -# Doxygen selects the parser to use depending on the extension of the files it -# parses. With this tag you can assign which parser to use for a given -# extension. Doxygen has a built-in mapping, but you can override or extend it -# using this tag. The format is ext=language, where ext is a file extension, -# and language is one of the parsers supported by doxygen: IDL, Java, -# Javascript, CSharp, C, C++, D, PHP, Objective-C, Python, Fortran, VHDL, C, -# C++. For instance to make doxygen treat .inc files as Fortran files (default -# is PHP), and .f files as C (default is Fortran), use: inc=Fortran f=C. Note -# that for custom extensions you also need to set FILE_PATTERNS otherwise the -# files are not read by doxygen. - -EXTENSION_MAPPING = - -# If MARKDOWN_SUPPORT is enabled (the default) then doxygen pre-processes all -# comments according to the Markdown format, which allows for more readable -# documentation. See http://daringfireball.net/projects/markdown/ for details. -# The output of markdown processing is further processed by doxygen, so you -# can mix doxygen, HTML, and XML commands with Markdown formatting. -# Disable only in case of backward compatibilities issues. - -MARKDOWN_SUPPORT = YES - -# When enabled doxygen tries to link words that correspond to documented classes, -# or namespaces to their corresponding documentation. Such a link can be -# prevented in individual cases by by putting a % sign in front of the word or -# globally by setting AUTOLINK_SUPPORT to NO. - -AUTOLINK_SUPPORT = YES - -# If you use STL classes (i.e. std::string, std::vector, etc.) but do not want -# to include (a tag file for) the STL sources as input, then you should -# set this tag to YES in order to let doxygen match functions declarations and -# definitions whose arguments contain STL classes (e.g. func(std::string) v.s. -# func(std::string) {}). This also makes the inheritance and collaboration -# diagrams that involve STL classes more complete and accurate. - -BUILTIN_STL_SUPPORT = NO - -# If you use Microsoft's C++/CLI language, you should set this option to YES to -# enable parsing support. - -CPP_CLI_SUPPORT = NO - -# Set the SIP_SUPPORT tag to YES if your project consists of sip sources only. -# Doxygen will parse them like normal C++ but will assume all classes use public -# instead of private inheritance when no explicit protection keyword is present. - -SIP_SUPPORT = NO - -# For Microsoft's IDL there are propget and propput attributes to indicate -# getter and setter methods for a property. Setting this option to YES (the -# default) will make doxygen replace the get and set methods by a property in -# the documentation. This will only work if the methods are indeed getting or -# setting a simple type. If this is not the case, or you want to show the -# methods anyway, you should set this option to NO. - -IDL_PROPERTY_SUPPORT = YES - -# If member grouping is used in the documentation and the DISTRIBUTE_GROUP_DOC -# tag is set to YES, then doxygen will reuse the documentation of the first -# member in the group (if any) for the other members of the group. By default -# all members of a group must be documented explicitly. - -DISTRIBUTE_GROUP_DOC = NO - -# Set the SUBGROUPING tag to YES (the default) to allow class member groups of -# the same type (for instance a group of public functions) to be put as a -# subgroup of that type (e.g. under the Public Functions section). Set it to -# NO to prevent subgrouping. Alternatively, this can be done per class using -# the \nosubgrouping command. - -SUBGROUPING = YES - -# When the INLINE_GROUPED_CLASSES tag is set to YES, classes, structs and -# unions are shown inside the group in which they are included (e.g. using -# @ingroup) instead of on a separate page (for HTML and Man pages) or -# section (for LaTeX and RTF). - -INLINE_GROUPED_CLASSES = NO - -# When the INLINE_SIMPLE_STRUCTS tag is set to YES, structs, classes, and -# unions with only public data fields will be shown inline in the documentation -# of the scope in which they are defined (i.e. file, namespace, or group -# documentation), provided this scope is documented. If set to NO (the default), -# structs, classes, and unions are shown on a separate page (for HTML and Man -# pages) or section (for LaTeX and RTF). - -INLINE_SIMPLE_STRUCTS = NO - -# When TYPEDEF_HIDES_STRUCT is enabled, a typedef of a struct, union, or enum -# is documented as struct, union, or enum with the name of the typedef. So -# typedef struct TypeS {} TypeT, will appear in the documentation as a struct -# with name TypeT. When disabled the typedef will appear as a member of a file, -# namespace, or class. And the struct will be named TypeS. This can typically -# be useful for C code in case the coding convention dictates that all compound -# types are typedef'ed and only the typedef is referenced, never the tag name. - -TYPEDEF_HIDES_STRUCT = NO - -# The SYMBOL_CACHE_SIZE determines the size of the internal cache use to -# determine which symbols to keep in memory and which to flush to disk. -# When the cache is full, less often used symbols will be written to disk. -# For small to medium size projects (<1000 input files) the default value is -# probably good enough. For larger projects a too small cache size can cause -# doxygen to be busy swapping symbols to and from disk most of the time -# causing a significant performance penalty. -# If the system has enough physical memory increasing the cache will improve the -# performance by keeping more symbols in memory. Note that the value works on -# a logarithmic scale so increasing the size by one will roughly double the -# memory usage. The cache size is given by this formula: -# 2^(16+SYMBOL_CACHE_SIZE). The valid range is 0..9, the default is 0, -# corresponding to a cache size of 2^16 = 65536 symbols. - -SYMBOL_CACHE_SIZE = 0 - -# Similar to the SYMBOL_CACHE_SIZE the size of the symbol lookup cache can be -# set using LOOKUP_CACHE_SIZE. This cache is used to resolve symbols given -# their name and scope. Since this can be an expensive process and often the -# same symbol appear multiple times in the code, doxygen keeps a cache of -# pre-resolved symbols. If the cache is too small doxygen will become slower. -# If the cache is too large, memory is wasted. The cache size is given by this -# formula: 2^(16+LOOKUP_CACHE_SIZE). The valid range is 0..9, the default is 0, -# corresponding to a cache size of 2^16 = 65536 symbols. - -LOOKUP_CACHE_SIZE = 0 - -#--------------------------------------------------------------------------- -# Build related configuration options -#--------------------------------------------------------------------------- - -# If the EXTRACT_ALL tag is set to YES doxygen will assume all entities in -# documentation are documented, even if no documentation was available. -# Private class members and static file members will be hidden unless -# the EXTRACT_PRIVATE and EXTRACT_STATIC tags are set to YES - -EXTRACT_ALL = YES - -# If the EXTRACT_PRIVATE tag is set to YES all private members of a class -# will be included in the documentation. - -EXTRACT_PRIVATE = NO - -# If the EXTRACT_PACKAGE tag is set to YES all members with package or internal -# scope will be included in the documentation. - -EXTRACT_PACKAGE = NO - -# If the EXTRACT_STATIC tag is set to YES all static members of a file -# will be included in the documentation. - -EXTRACT_STATIC = NO - -# If the EXTRACT_LOCAL_CLASSES tag is set to YES classes (and structs) -# defined locally in source files will be included in the documentation. -# If set to NO only classes defined in header files are included. - -EXTRACT_LOCAL_CLASSES = YES - -# This flag is only useful for Objective-C code. When set to YES local -# methods, which are defined in the implementation section but not in -# the interface are included in the documentation. -# If set to NO (the default) only methods in the interface are included. - -EXTRACT_LOCAL_METHODS = NO - -# If this flag is set to YES, the members of anonymous namespaces will be -# extracted and appear in the documentation as a namespace called -# 'anonymous_namespace{file}', where file will be replaced with the base -# name of the file that contains the anonymous namespace. By default -# anonymous namespaces are hidden. - -EXTRACT_ANON_NSPACES = NO - -# If the HIDE_UNDOC_MEMBERS tag is set to YES, Doxygen will hide all -# undocumented members of documented classes, files or namespaces. -# If set to NO (the default) these members will be included in the -# various overviews, but no documentation section is generated. -# This option has no effect if EXTRACT_ALL is enabled. - -HIDE_UNDOC_MEMBERS = NO - -# If the HIDE_UNDOC_CLASSES tag is set to YES, Doxygen will hide all -# undocumented classes that are normally visible in the class hierarchy. -# If set to NO (the default) these classes will be included in the various -# overviews. This option has no effect if EXTRACT_ALL is enabled. - -HIDE_UNDOC_CLASSES = NO - -# If the HIDE_FRIEND_COMPOUNDS tag is set to YES, Doxygen will hide all -# friend (class|struct|union) declarations. -# If set to NO (the default) these declarations will be included in the -# documentation. - -HIDE_FRIEND_COMPOUNDS = NO - -# If the HIDE_IN_BODY_DOCS tag is set to YES, Doxygen will hide any -# documentation blocks found inside the body of a function. -# If set to NO (the default) these blocks will be appended to the -# function's detailed documentation block. - -HIDE_IN_BODY_DOCS = NO - -# The INTERNAL_DOCS tag determines if documentation -# that is typed after a \internal command is included. If the tag is set -# to NO (the default) then the documentation will be excluded. -# Set it to YES to include the internal documentation. - -INTERNAL_DOCS = NO - -# If the CASE_SENSE_NAMES tag is set to NO then Doxygen will only generate -# file names in lower-case letters. If set to YES upper-case letters are also -# allowed. This is useful if you have classes or files whose names only differ -# in case and if your file system supports case sensitive file names. Windows -# and Mac users are advised to set this option to NO. - -CASE_SENSE_NAMES = NO - -# If the HIDE_SCOPE_NAMES tag is set to NO (the default) then Doxygen -# will show members with their full class and namespace scopes in the -# documentation. If set to YES the scope will be hidden. - -HIDE_SCOPE_NAMES = NO - -# If the SHOW_INCLUDE_FILES tag is set to YES (the default) then Doxygen -# will put a list of the files that are included by a file in the documentation -# of that file. - -SHOW_INCLUDE_FILES = YES - -# If the FORCE_LOCAL_INCLUDES tag is set to YES then Doxygen -# will list include files with double quotes in the documentation -# rather than with sharp brackets. - -FORCE_LOCAL_INCLUDES = NO - -# If the INLINE_INFO tag is set to YES (the default) then a tag [inline] -# is inserted in the documentation for inline members. - -INLINE_INFO = YES - -# If the SORT_MEMBER_DOCS tag is set to YES (the default) then doxygen -# will sort the (detailed) documentation of file and class members -# alphabetically by member name. If set to NO the members will appear in -# declaration order. - -SORT_MEMBER_DOCS = YES - -# If the SORT_BRIEF_DOCS tag is set to YES then doxygen will sort the -# brief documentation of file, namespace and class members alphabetically -# by member name. If set to NO (the default) the members will appear in -# declaration order. - -SORT_BRIEF_DOCS = NO - -# If the SORT_MEMBERS_CTORS_1ST tag is set to YES then doxygen -# will sort the (brief and detailed) documentation of class members so that -# constructors and destructors are listed first. If set to NO (the default) -# the constructors will appear in the respective orders defined by -# SORT_MEMBER_DOCS and SORT_BRIEF_DOCS. -# This tag will be ignored for brief docs if SORT_BRIEF_DOCS is set to NO -# and ignored for detailed docs if SORT_MEMBER_DOCS is set to NO. - -SORT_MEMBERS_CTORS_1ST = NO - -# If the SORT_GROUP_NAMES tag is set to YES then doxygen will sort the -# hierarchy of group names into alphabetical order. If set to NO (the default) -# the group names will appear in their defined order. - -SORT_GROUP_NAMES = NO - -# If the SORT_BY_SCOPE_NAME tag is set to YES, the class list will be -# sorted by fully-qualified names, including namespaces. If set to -# NO (the default), the class list will be sorted only by class name, -# not including the namespace part. -# Note: This option is not very useful if HIDE_SCOPE_NAMES is set to YES. -# Note: This option applies only to the class list, not to the -# alphabetical list. - -SORT_BY_SCOPE_NAME = NO - -# If the STRICT_PROTO_MATCHING option is enabled and doxygen fails to -# do proper type resolution of all parameters of a function it will reject a -# match between the prototype and the implementation of a member function even -# if there is only one candidate or it is obvious which candidate to choose -# by doing a simple string match. By disabling STRICT_PROTO_MATCHING doxygen -# will still accept a match between prototype and implementation in such cases. - -STRICT_PROTO_MATCHING = NO - -# The GENERATE_TODOLIST tag can be used to enable (YES) or -# disable (NO) the todo list. This list is created by putting \todo -# commands in the documentation. - -GENERATE_TODOLIST = YES - -# The GENERATE_TESTLIST tag can be used to enable (YES) or -# disable (NO) the test list. This list is created by putting \test -# commands in the documentation. - -GENERATE_TESTLIST = YES - -# The GENERATE_BUGLIST tag can be used to enable (YES) or -# disable (NO) the bug list. This list is created by putting \bug -# commands in the documentation. - -GENERATE_BUGLIST = YES - -# The GENERATE_DEPRECATEDLIST tag can be used to enable (YES) or -# disable (NO) the deprecated list. This list is created by putting -# \deprecated commands in the documentation. - -GENERATE_DEPRECATEDLIST= YES - -# The ENABLED_SECTIONS tag can be used to enable conditional -# documentation sections, marked by \if section-label ... \endif -# and \cond section-label ... \endcond blocks. - -ENABLED_SECTIONS = - -# The MAX_INITIALIZER_LINES tag determines the maximum number of lines -# the initial value of a variable or macro consists of for it to appear in -# the documentation. If the initializer consists of more lines than specified -# here it will be hidden. Use a value of 0 to hide initializers completely. -# The appearance of the initializer of individual variables and macros in the -# documentation can be controlled using \showinitializer or \hideinitializer -# command in the documentation regardless of this setting. - -MAX_INITIALIZER_LINES = 30 - -# Set the SHOW_USED_FILES tag to NO to disable the list of files generated -# at the bottom of the documentation of classes and structs. If set to YES the -# list will mention the files that were used to generate the documentation. - -SHOW_USED_FILES = YES - -# Set the SHOW_FILES tag to NO to disable the generation of the Files page. -# This will remove the Files entry from the Quick Index and from the -# Folder Tree View (if specified). The default is YES. - -SHOW_FILES = YES - -# Set the SHOW_NAMESPACES tag to NO to disable the generation of the -# Namespaces page. This will remove the Namespaces entry from the Quick Index -# and from the Folder Tree View (if specified). The default is YES. - -SHOW_NAMESPACES = YES - -# The FILE_VERSION_FILTER tag can be used to specify a program or script that -# doxygen should invoke to get the current version for each file (typically from -# the version control system). Doxygen will invoke the program by executing (via -# popen()) the command , where is the value of -# the FILE_VERSION_FILTER tag, and is the name of an input file -# provided by doxygen. Whatever the program writes to standard output -# is used as the file version. See the manual for examples. - -FILE_VERSION_FILTER = - -# The LAYOUT_FILE tag can be used to specify a layout file which will be parsed -# by doxygen. The layout file controls the global structure of the generated -# output files in an output format independent way. To create the layout file -# that represents doxygen's defaults, run doxygen with the -l option. -# You can optionally specify a file name after the option, if omitted -# DoxygenLayout.xml will be used as the name of the layout file. - -LAYOUT_FILE = - -# The CITE_BIB_FILES tag can be used to specify one or more bib files -# containing the references data. This must be a list of .bib files. The -# .bib extension is automatically appended if omitted. Using this command -# requires the bibtex tool to be installed. See also -# http://en.wikipedia.org/wiki/BibTeX for more info. For LaTeX the style -# of the bibliography can be controlled using LATEX_BIB_STYLE. To use this -# feature you need bibtex and perl available in the search path. Do not use -# file names with spaces, bibtex cannot handle them. - -CITE_BIB_FILES = - -#--------------------------------------------------------------------------- -# configuration options related to warning and progress messages -#--------------------------------------------------------------------------- - -# The QUIET tag can be used to turn on/off the messages that are generated -# by doxygen. Possible values are YES and NO. If left blank NO is used. - -QUIET = NO - -# The WARNINGS tag can be used to turn on/off the warning messages that are -# generated by doxygen. Possible values are YES and NO. If left blank -# NO is used. - -WARNINGS = YES - -# If WARN_IF_UNDOCUMENTED is set to YES, then doxygen will generate warnings -# for undocumented members. If EXTRACT_ALL is set to YES then this flag will -# automatically be disabled. - -WARN_IF_UNDOCUMENTED = YES - -# If WARN_IF_DOC_ERROR is set to YES, doxygen will generate warnings for -# potential errors in the documentation, such as not documenting some -# parameters in a documented function, or documenting parameters that -# don't exist or using markup commands wrongly. - -WARN_IF_DOC_ERROR = YES - -# The WARN_NO_PARAMDOC option can be enabled to get warnings for -# functions that are documented, but have no documentation for their parameters -# or return value. If set to NO (the default) doxygen will only warn about -# wrong or incomplete parameter documentation, but not about the absence of -# documentation. - -WARN_NO_PARAMDOC = NO - -# The WARN_FORMAT tag determines the format of the warning messages that -# doxygen can produce. The string should contain the $file, $line, and $text -# tags, which will be replaced by the file and line number from which the -# warning originated and the warning text. Optionally the format may contain -# $version, which will be replaced by the version of the file (if it could -# be obtained via FILE_VERSION_FILTER) - -WARN_FORMAT = "$file:$line: $text" - -# The WARN_LOGFILE tag can be used to specify a file to which warning -# and error messages should be written. If left blank the output is written -# to stderr. - -WARN_LOGFILE = - -#--------------------------------------------------------------------------- -# configuration options related to the input files -#--------------------------------------------------------------------------- - -# The INPUT tag can be used to specify the files and/or directories that contain -# documented source files. You may enter file names like "myfile.cpp" or -# directories like "/usr/src/myproject". Separate the files or directories -# with spaces. - -INPUT = doc \ - sasfit_common \ - sasfit_sd \ - sasfit_sq \ - sasfit_peaks \ - sasfit_ff \ - sasfit_core \ - sasfit_old \ - plugins - -# This tag can be used to specify the character encoding of the source files -# that doxygen parses. Internally doxygen uses the UTF-8 encoding, which is -# also the default input encoding. Doxygen uses libiconv (or the iconv built -# into libc) for the transcoding. See http://www.gnu.org/software/libiconv for -# the list of possible encodings. - -INPUT_ENCODING = UTF-8 - -# If the value of the INPUT tag contains directories, you can use the -# FILE_PATTERNS tag to specify one or more wildcard pattern (like *.cpp -# and *.h) to filter out the source-files in the directories. If left -# blank the following patterns are tested: -# *.c *.cc *.cxx *.cpp *.c++ *.d *.java *.ii *.ixx *.ipp *.i++ *.inl *.h *.hh -# *.hxx *.hpp *.h++ *.idl *.odl *.cs *.php *.php3 *.inc *.m *.mm *.dox *.py -# *.f90 *.f *.for *.vhd *.vhdl - -FILE_PATTERNS = *.c \ - *.h \ - *.def - -# The RECURSIVE tag can be used to turn specify whether or not subdirectories -# should be searched for input files as well. Possible values are YES and NO. -# If left blank NO is used. - -RECURSIVE = YES - -# The EXCLUDE tag can be used to specify files and/or directories that should be -# excluded from the INPUT source files. This way you can easily exclude a -# subdirectory from a directory tree whose root is specified with the INPUT tag. -# Note that relative paths are relative to the directory from which doxygen is -# run. - -EXCLUDE = - -# The EXCLUDE_SYMLINKS tag can be used to select whether or not files or -# directories that are symbolic links (a Unix file system feature) are excluded -# from the input. - -EXCLUDE_SYMLINKS = YES - -# If the value of the INPUT tag contains directories, you can use the -# EXCLUDE_PATTERNS tag to specify one or more wildcard patterns to exclude -# certain files from those directories. Note that the wildcards are matched -# against the file with absolute path, so to exclude all test directories -# for example use the pattern */test/* - -EXCLUDE_PATTERNS = *.dir \ - .svn \ - */CMakeFiles \ - */lib - -# The EXCLUDE_SYMBOLS tag can be used to specify one or more symbol names -# (namespaces, classes, functions, etc.) that should be excluded from the -# output. The symbol name can be a fully qualified name, a word, or if the -# wildcard * is used, a substring. Examples: ANamespace, AClass, -# AClass::ANamespace, ANamespace::*Test - -EXCLUDE_SYMBOLS = - -# The EXAMPLE_PATH tag can be used to specify one or more files or -# directories that contain example code fragments that are included (see -# the \include command). - -EXAMPLE_PATH = ../examples/ - -# If the value of the EXAMPLE_PATH tag contains directories, you can use the -# EXAMPLE_PATTERNS tag to specify one or more wildcard pattern (like *.cpp -# and *.h) to filter out the source-files in the directories. If left -# blank all files are included. - -EXAMPLE_PATTERNS = *.c - -# If the EXAMPLE_RECURSIVE tag is set to YES then subdirectories will be -# searched for input files to be used with the \include or \dontinclude -# commands irrespective of the value of the RECURSIVE tag. -# Possible values are YES and NO. If left blank NO is used. - -EXAMPLE_RECURSIVE = NO - -# The IMAGE_PATH tag can be used to specify one or more files or -# directories that contain image that are included in the documentation (see -# the \image command). - -IMAGE_PATH = ../doc/images/ - -# The INPUT_FILTER tag can be used to specify a program that doxygen should -# invoke to filter for each input file. Doxygen will invoke the filter program -# by executing (via popen()) the command , where -# is the value of the INPUT_FILTER tag, and is the name of an -# input file. Doxygen will then use the output that the filter program writes -# to standard output. If FILTER_PATTERNS is specified, this tag will be -# ignored. - -INPUT_FILTER = - -# The FILTER_PATTERNS tag can be used to specify filters on a per file pattern -# basis. Doxygen will compare the file name with each pattern and apply the -# filter if there is a match. The filters are a list of the form: -# pattern=filter (like *.cpp=my_cpp_filter). See INPUT_FILTER for further -# info on how filters are used. If FILTER_PATTERNS is empty or if -# non of the patterns match the file name, INPUT_FILTER is applied. - -FILTER_PATTERNS = - -# If the FILTER_SOURCE_FILES tag is set to YES, the input filter (if set using -# INPUT_FILTER) will be used to filter the input files when producing source -# files to browse (i.e. when SOURCE_BROWSER is set to YES). - -FILTER_SOURCE_FILES = NO - -# The FILTER_SOURCE_PATTERNS tag can be used to specify source filters per file -# pattern. A pattern will override the setting for FILTER_PATTERN (if any) -# and it is also possible to disable source filtering for a specific pattern -# using *.ext= (so without naming a filter). This option only has effect when -# FILTER_SOURCE_FILES is enabled. - -FILTER_SOURCE_PATTERNS = - -# If the USE_MD_FILE_AS_MAINPAGE tag refers to the name of a markdown file that -# is part of the input, its contents will be placed on the main page (index.html). -# This can be useful if you have a project on for instance GitHub and want reuse -# the introduction page also for the doxygen output. - -USE_MDFILE_AS_MAINPAGE = - -#--------------------------------------------------------------------------- -# configuration options related to source browsing -#--------------------------------------------------------------------------- - -# If the SOURCE_BROWSER tag is set to YES then a list of source files will -# be generated. Documented entities will be cross-referenced with these sources. -# Note: To get rid of all source code in the generated output, make sure also -# VERBATIM_HEADERS is set to NO. - -SOURCE_BROWSER = YES - -# Setting the INLINE_SOURCES tag to YES will include the body -# of functions and classes directly in the documentation. - -INLINE_SOURCES = NO - -# Setting the STRIP_CODE_COMMENTS tag to YES (the default) will instruct -# doxygen to hide any special comment blocks from generated source code -# fragments. Normal C, C++ and Fortran comments will always remain visible. - -STRIP_CODE_COMMENTS = YES - -# If the REFERENCED_BY_RELATION tag is set to YES -# then for each documented function all documented -# functions referencing it will be listed. - -REFERENCED_BY_RELATION = YES - -# If the REFERENCES_RELATION tag is set to YES -# then for each documented function all documented entities -# called/used by that function will be listed. - -REFERENCES_RELATION = YES - -# If the REFERENCES_LINK_SOURCE tag is set to YES (the default) -# and SOURCE_BROWSER tag is set to YES, then the hyperlinks from -# functions in REFERENCES_RELATION and REFERENCED_BY_RELATION lists will -# link to the source code. Otherwise they will link to the documentation. - -REFERENCES_LINK_SOURCE = YES - -# If the USE_HTAGS tag is set to YES then the references to source code -# will point to the HTML generated by the htags(1) tool instead of doxygen -# built-in source browser. The htags tool is part of GNU's global source -# tagging system (see http://www.gnu.org/software/global/global.html). You -# will need version 4.8.6 or higher. - -USE_HTAGS = NO - -# If the VERBATIM_HEADERS tag is set to YES (the default) then Doxygen -# will generate a verbatim copy of the header file for each class for -# which an include is specified. Set to NO to disable this. - -VERBATIM_HEADERS = YES - -#--------------------------------------------------------------------------- -# configuration options related to the alphabetical class index -#--------------------------------------------------------------------------- - -# If the ALPHABETICAL_INDEX tag is set to YES, an alphabetical index -# of all compounds will be generated. Enable this if the project -# contains a lot of classes, structs, unions or interfaces. - -ALPHABETICAL_INDEX = NO - -# If the alphabetical index is enabled (see ALPHABETICAL_INDEX) then -# the COLS_IN_ALPHA_INDEX tag can be used to specify the number of columns -# in which this list will be split (can be a number in the range [1..20]) - -COLS_IN_ALPHA_INDEX = 5 - -# In case all classes in a project start with a common prefix, all -# classes will be put under the same header in the alphabetical index. -# The IGNORE_PREFIX tag can be used to specify one or more prefixes that -# should be ignored while generating the index headers. - -IGNORE_PREFIX = - -#--------------------------------------------------------------------------- -# configuration options related to the HTML output -#--------------------------------------------------------------------------- - -# If the GENERATE_HTML tag is set to YES (the default) Doxygen will -# generate HTML output. - -GENERATE_HTML = YES - -# The HTML_OUTPUT tag is used to specify where the HTML docs will be put. -# If a relative path is entered the value of OUTPUT_DIRECTORY will be -# put in front of it. If left blank `html' will be used as the default path. - -HTML_OUTPUT = html - -# The HTML_FILE_EXTENSION tag can be used to specify the file extension for -# each generated HTML page (for example: .htm,.php,.asp). If it is left blank -# doxygen will generate files with .html extension. - -HTML_FILE_EXTENSION = .html - -# The HTML_HEADER tag can be used to specify a personal HTML header for -# each generated HTML page. If it is left blank doxygen will generate a -# standard header. Note that when using a custom header you are responsible -# for the proper inclusion of any scripts and style sheets that doxygen -# needs, which is dependent on the configuration options used. -# It is advised to generate a default header using "doxygen -w html -# header.html footer.html stylesheet.css YourConfigFile" and then modify -# that header. Note that the header is subject to change so you typically -# have to redo this when upgrading to a newer version of doxygen or when -# changing the value of configuration settings such as GENERATE_TREEVIEW! - -HTML_HEADER = - -# The HTML_FOOTER tag can be used to specify a personal HTML footer for -# each generated HTML page. If it is left blank doxygen will generate a -# standard footer. - -HTML_FOOTER = doc/footer.html - -# The HTML_STYLESHEET tag can be used to specify a user-defined cascading -# style sheet that is used by each HTML page. It can be used to -# fine-tune the look of the HTML output. If left blank doxygen will -# generate a default style sheet. Note that it is recommended to use -# HTML_EXTRA_STYLESHEET instead of this one, as it is more robust and this -# tag will in the future become obsolete. - -HTML_STYLESHEET = doc/stylesheet.css - -# The HTML_EXTRA_STYLESHEET tag can be used to specify an additional -# user-defined cascading style sheet that is included after the standard -# style sheets created by doxygen. Using this option one can overrule -# certain style aspects. This is preferred over using HTML_STYLESHEET -# since it does not replace the standard style sheet and is therefor more -# robust against future updates. Doxygen will copy the style sheet file to -# the output directory. - -HTML_EXTRA_STYLESHEET = - -# The HTML_EXTRA_FILES tag can be used to specify one or more extra images or -# other source files which should be copied to the HTML output directory. Note -# that these files will be copied to the base HTML output directory. Use the -# $relpath$ marker in the HTML_HEADER and/or HTML_FOOTER files to load these -# files. In the HTML_STYLESHEET file, use the file name only. Also note that -# the files will be copied as-is there are no commands or markers available. - -HTML_EXTRA_FILES = - -# The HTML_COLORSTYLE_HUE tag controls the color of the HTML output. -# Doxygen will adjust the colors in the style sheet and background images -# according to this color. Hue is specified as an angle on a colorwheel, -# see http://en.wikipedia.org/wiki/Hue for more information. -# For instance the value 0 represents red, 60 is yellow, 120 is green, -# 180 is cyan, 240 is blue, 300 purple, and 360 is red again. -# The allowed range is 0 to 359. - -HTML_COLORSTYLE_HUE = 220 - -# The HTML_COLORSTYLE_SAT tag controls the purity (or saturation) of -# the colors in the HTML output. For a value of 0 the output will use -# grayscales only. A value of 255 will produce the most vivid colors. - -HTML_COLORSTYLE_SAT = 100 - -# The HTML_COLORSTYLE_GAMMA tag controls the gamma correction applied to -# the luminance component of the colors in the HTML output. Values below -# 100 gradually make the output lighter, whereas values above 100 make -# the output darker. The value divided by 100 is the actual gamma applied, -# so 80 represents a gamma of 0.8, The value 220 represents a gamma of 2.2, -# and 100 does not change the gamma. - -HTML_COLORSTYLE_GAMMA = 80 - -# If the HTML_TIMESTAMP tag is set to YES then the footer of each generated HTML -# page will contain the date and time when the page was generated. Setting -# this to NO can help when comparing the output of multiple runs. - -HTML_TIMESTAMP = YES - -# If the HTML_DYNAMIC_SECTIONS tag is set to YES then the generated HTML -# documentation will contain sections that can be hidden and shown after the -# page has loaded. - -HTML_DYNAMIC_SECTIONS = NO - -# With HTML_INDEX_NUM_ENTRIES one can control the preferred number of -# entries shown in the various tree structured indices initially the user -# can expand and collapse entries dynamically later on. Doxygen will expand -# the tree to such a level that at most the specified number of entries are -# visible (unless a fully collapsed tree already exceeds this amount). -# So setting the number of entries 1 will produce a full collapsed tree by -# default. 0 is a special value representing an infinite number of entries -# and will result in a full expanded tree by default. - -HTML_INDEX_NUM_ENTRIES = 100 - -# If the GENERATE_DOCSET tag is set to YES, additional index files -# will be generated that can be used as input for Apple's Xcode 3 -# integrated development environment, introduced with OSX 10.5 (Leopard). -# To create a documentation set, doxygen will generate a Makefile in the -# HTML output directory. Running make will produce the docset in that -# directory and running "make install" will install the docset in -# ~/Library/Developer/Shared/Documentation/DocSets so that Xcode will find -# it at startup. -# See http://developer.apple.com/tools/creatingdocsetswithdoxygen.html -# for more information. - -GENERATE_DOCSET = NO - -# When GENERATE_DOCSET tag is set to YES, this tag determines the name of the -# feed. A documentation feed provides an umbrella under which multiple -# documentation sets from a single provider (such as a company or product suite) -# can be grouped. - -DOCSET_FEEDNAME = "Doxygen generated docs" - -# When GENERATE_DOCSET tag is set to YES, this tag specifies a string that -# should uniquely identify the documentation set bundle. This should be a -# reverse domain-name style string, e.g. com.mycompany.MyDocSet. Doxygen -# will append .docset to the name. - -DOCSET_BUNDLE_ID = org.doxygen.Project - -# When GENERATE_PUBLISHER_ID tag specifies a string that should uniquely -# identify the documentation publisher. This should be a reverse domain-name -# style string, e.g. com.mycompany.MyDocSet.documentation. - -DOCSET_PUBLISHER_ID = org.doxygen.Publisher - -# The GENERATE_PUBLISHER_NAME tag identifies the documentation publisher. - -DOCSET_PUBLISHER_NAME = Publisher - -# If the GENERATE_HTMLHELP tag is set to YES, additional index files -# will be generated that can be used as input for tools like the -# Microsoft HTML help workshop to generate a compiled HTML help file (.chm) -# of the generated HTML documentation. - -GENERATE_HTMLHELP = YES - -# If the GENERATE_HTMLHELP tag is set to YES, the CHM_FILE tag can -# be used to specify the file name of the resulting .chm file. You -# can add a path in front of the file if the result should not be -# written to the html output directory. - -CHM_FILE = - -# If the GENERATE_HTMLHELP tag is set to YES, the HHC_LOCATION tag can -# be used to specify the location (absolute path including file name) of -# the HTML help compiler (hhc.exe). If non-empty doxygen will try to run -# the HTML help compiler on the generated index.hhp. - -HHC_LOCATION = - -# If the GENERATE_HTMLHELP tag is set to YES, the GENERATE_CHI flag -# controls if a separate .chi index file is generated (YES) or that -# it should be included in the master .chm file (NO). - -GENERATE_CHI = NO - -# If the GENERATE_HTMLHELP tag is set to YES, the CHM_INDEX_ENCODING -# is used to encode HtmlHelp index (hhk), content (hhc) and project file -# content. - -CHM_INDEX_ENCODING = - -# If the GENERATE_HTMLHELP tag is set to YES, the BINARY_TOC flag -# controls whether a binary table of contents is generated (YES) or a -# normal table of contents (NO) in the .chm file. - -BINARY_TOC = NO - -# The TOC_EXPAND flag can be set to YES to add extra items for group members -# to the contents of the HTML help documentation and to the tree view. - -TOC_EXPAND = NO - -# If the GENERATE_QHP tag is set to YES and both QHP_NAMESPACE and -# QHP_VIRTUAL_FOLDER are set, an additional index file will be generated -# that can be used as input for Qt's qhelpgenerator to generate a -# Qt Compressed Help (.qch) of the generated HTML documentation. - -GENERATE_QHP = NO - -# If the QHG_LOCATION tag is specified, the QCH_FILE tag can -# be used to specify the file name of the resulting .qch file. -# The path specified is relative to the HTML output folder. - -QCH_FILE = - -# The QHP_NAMESPACE tag specifies the namespace to use when generating -# Qt Help Project output. For more information please see -# http://doc.trolltech.com/qthelpproject.html#namespace - -QHP_NAMESPACE = org.doxygen.Project - -# The QHP_VIRTUAL_FOLDER tag specifies the namespace to use when generating -# Qt Help Project output. For more information please see -# http://doc.trolltech.com/qthelpproject.html#virtual-folders - -QHP_VIRTUAL_FOLDER = doc - -# If QHP_CUST_FILTER_NAME is set, it specifies the name of a custom filter to -# add. For more information please see -# http://doc.trolltech.com/qthelpproject.html#custom-filters - -QHP_CUST_FILTER_NAME = - -# The QHP_CUST_FILT_ATTRS tag specifies the list of the attributes of the -# custom filter to add. For more information please see -# -# Qt Help Project / Custom Filters. - -QHP_CUST_FILTER_ATTRS = - -# The QHP_SECT_FILTER_ATTRS tag specifies the list of the attributes this -# project's -# filter section matches. -# -# Qt Help Project / Filter Attributes. - -QHP_SECT_FILTER_ATTRS = - -# If the GENERATE_QHP tag is set to YES, the QHG_LOCATION tag can -# be used to specify the location of Qt's qhelpgenerator. -# If non-empty doxygen will try to run qhelpgenerator on the generated -# .qhp file. - -QHG_LOCATION = - -# If the GENERATE_ECLIPSEHELP tag is set to YES, additional index files -# will be generated, which together with the HTML files, form an Eclipse help -# plugin. To install this plugin and make it available under the help contents -# menu in Eclipse, the contents of the directory containing the HTML and XML -# files needs to be copied into the plugins directory of eclipse. The name of -# the directory within the plugins directory should be the same as -# the ECLIPSE_DOC_ID value. After copying Eclipse needs to be restarted before -# the help appears. - -GENERATE_ECLIPSEHELP = NO - -# A unique identifier for the eclipse help plugin. When installing the plugin -# the directory name containing the HTML and XML files should also have -# this name. - -ECLIPSE_DOC_ID = org.doxygen.Project - -# The DISABLE_INDEX tag can be used to turn on/off the condensed index (tabs) -# at top of each HTML page. The value NO (the default) enables the index and -# the value YES disables it. Since the tabs have the same information as the -# navigation tree you can set this option to NO if you already set -# GENERATE_TREEVIEW to YES. - -DISABLE_INDEX = NO - -# The GENERATE_TREEVIEW tag is used to specify whether a tree-like index -# structure should be generated to display hierarchical information. -# If the tag value is set to YES, a side panel will be generated -# containing a tree-like index structure (just like the one that -# is generated for HTML Help). For this to work a browser that supports -# JavaScript, DHTML, CSS and frames is required (i.e. any modern browser). -# Windows users are probably better off using the HTML help feature. -# Since the tree basically has the same information as the tab index you -# could consider to set DISABLE_INDEX to NO when enabling this option. - -GENERATE_TREEVIEW = NO - -# The ENUM_VALUES_PER_LINE tag can be used to set the number of enum values -# (range [0,1..20]) that doxygen will group on one line in the generated HTML -# documentation. Note that a value of 0 will completely suppress the enum -# values from appearing in the overview section. - -ENUM_VALUES_PER_LINE = 4 - -# If the treeview is enabled (see GENERATE_TREEVIEW) then this tag can be -# used to set the initial width (in pixels) of the frame in which the tree -# is shown. - -TREEVIEW_WIDTH = 250 - -# When the EXT_LINKS_IN_WINDOW option is set to YES doxygen will open -# links to external symbols imported via tag files in a separate window. - -EXT_LINKS_IN_WINDOW = NO - -# Use this tag to change the font size of Latex formulas included -# as images in the HTML documentation. The default is 10. Note that -# when you change the font size after a successful doxygen run you need -# to manually remove any form_*.png images from the HTML output directory -# to force them to be regenerated. - -FORMULA_FONTSIZE = 10 - -# Use the FORMULA_TRANPARENT tag to determine whether or not the images -# generated for formulas are transparent PNGs. Transparent PNGs are -# not supported properly for IE 6.0, but are supported on all modern browsers. -# Note that when changing this option you need to delete any form_*.png files -# in the HTML output before the changes have effect. - -FORMULA_TRANSPARENT = YES - -# Enable the USE_MATHJAX option to render LaTeX formulas using MathJax -# (see http://www.mathjax.org) which uses client side Javascript for the -# rendering instead of using prerendered bitmaps. Use this if you do not -# have LaTeX installed or if you want to formulas look prettier in the HTML -# output. When enabled you may also need to install MathJax separately and -# configure the path to it using the MATHJAX_RELPATH option. - -USE_MATHJAX = YES - -# When MathJax is enabled you can set the default output format to be used for -# thA MathJax output. Supported types are HTML-CSS, NativeMML (i.e. MathML) and -# SVG. The default value is HTML-CSS, which is slower, but has the best -# compatibility. - -MATHJAX_FORMAT = HTML-CSS - -# When MathJax is enabled you need to specify the location relative to the -# HTML output directory using the MATHJAX_RELPATH option. The destination -# directory should contain the MathJax.js script. For instance, if the mathjax -# directory is located at the same level as the HTML output directory, then -# MATHJAX_RELPATH should be ../mathjax. The default value points to -# the MathJax Content Delivery Network so you can quickly see the result without -# installing MathJax. However, it is strongly recommended to install a local -# copy of MathJax from http://www.mathjax.org before deployment. - -MATHJAX_RELPATH = http://cdn.mathjax.org/mathjax/latest - -# The MATHJAX_EXTENSIONS tag can be used to specify one or MathJax extension -# names that should be enabled during MathJax rendering. - -MATHJAX_EXTENSIONS = - -# When the SEARCHENGINE tag is enabled doxygen will generate a search box -# for the HTML output. The underlying search engine uses javascript -# and DHTML and should work on any modern browser. Note that when using -# HTML help (GENERATE_HTMLHELP), Qt help (GENERATE_QHP), or docsets -# (GENERATE_DOCSET) there is already a search function so this one should -# typically be disabled. For large projects the javascript based search engine -# can be slow, then enabling SERVER_BASED_SEARCH may provide a better solution. - -SEARCHENGINE = YES - -# When the SERVER_BASED_SEARCH tag is enabled the search engine will be -# implemented using a web server instead of a web client using Javascript. -# There are two flavours of web server based search depending on the -# EXTERNAL_SEARCH setting. When disabled, doxygen will generate a PHP script for -# searching and an index file used by the script. When EXTERNAL_SEARCH is -# enabled the indexing and searching needs to be provided by external tools. -# See the manual for details. - -SERVER_BASED_SEARCH = NO - -# When EXTERNAL_SEARCH is enabled doxygen will no longer generate the PHP -# script for searching. Instead the search results are written to an XML file -# which needs to be processed by an external indexer. Doxygen will invoke an -# external search engine pointed to by the SEARCHENGINE_URL option to obtain -# the search results. Doxygen ships with an example indexer (doxyindexer) and -# search engine (doxysearch.cgi) which are based on the open source search engine -# library Xapian. See the manual for configuration details. - -EXTERNAL_SEARCH = NO - -# The SEARCHENGINE_URL should point to a search engine hosted by a web server -# which will returned the search results when EXTERNAL_SEARCH is enabled. -# Doxygen ships with an example search engine (doxysearch) which is based on -# the open source search engine library Xapian. See the manual for configuration -# details. - -SEARCHENGINE_URL = - -# When SERVER_BASED_SEARCH and EXTERNAL_SEARCH are both enabled the unindexed -# search data is written to a file for indexing by an external tool. With the -# SEARCHDATA_FILE tag the name of this file can be specified. - -SEARCHDATA_FILE = searchdata.xml - -# When SERVER_BASED_SEARCH AND EXTERNAL_SEARCH are both enabled the -# EXTERNAL_SEARCH_ID tag can be used as an identifier for the project. This is -# useful in combination with EXTRA_SEARCH_MAPPINGS to search through multiple -# projects and redirect the results back to the right project. - -EXTERNAL_SEARCH_ID = - -# The EXTRA_SEARCH_MAPPINGS tag can be used to enable searching through doxygen -# projects other than the one defined by this configuration file, but that are -# all added to the same external search index. Each project needs to have a -# unique id set via EXTERNAL_SEARCH_ID. The search mapping then maps the id -# of to a relative location where the documentation can be found. -# The format is: EXTRA_SEARCH_MAPPINGS = id1=loc1 id2=loc2 ... - -EXTRA_SEARCH_MAPPINGS = - -#--------------------------------------------------------------------------- -# configuration options related to the LaTeX output -#--------------------------------------------------------------------------- - -# If the GENERATE_LATEX tag is set to YES (the default) Doxygen will -# generate Latex output. - -GENERATE_LATEX = NO - -# The LATEX_OUTPUT tag is used to specify where the LaTeX docs will be put. -# If a relative path is entered the value of OUTPUT_DIRECTORY will be -# put in front of it. If left blank `latex' will be used as the default path. - -LATEX_OUTPUT = latex - -# The LATEX_CMD_NAME tag can be used to specify the LaTeX command name to be -# invoked. If left blank `latex' will be used as the default command name. -# Note that when enabling USE_PDFLATEX this option is only used for -# generating bitmaps for formulas in the HTML output, but not in the -# Makefile that is written to the output directory. - -LATEX_CMD_NAME = latex - -# The MAKEINDEX_CMD_NAME tag can be used to specify the command name to -# generate index for LaTeX. If left blank `makeindex' will be used as the -# default command name. - -MAKEINDEX_CMD_NAME = makeindex - -# If the COMPACT_LATEX tag is set to YES Doxygen generates more compact -# LaTeX documents. This may be useful for small projects and may help to -# save some trees in general. - -COMPACT_LATEX = YES - -# The PAPER_TYPE tag can be used to set the paper type that is used -# by the printer. Possible values are: a4, letter, legal and -# executive. If left blank a4wide will be used. - -PAPER_TYPE = a4wide - -# The EXTRA_PACKAGES tag can be to specify one or more names of LaTeX -# packages that should be included in the LaTeX output. - -EXTRA_PACKAGES = - -# The LATEX_HEADER tag can be used to specify a personal LaTeX header for -# the generated latex document. The header should contain everything until -# the first chapter. If it is left blank doxygen will generate a -# standard header. Notice: only use this tag if you know what you are doing! - -LATEX_HEADER = - -# The LATEX_FOOTER tag can be used to specify a personal LaTeX footer for -# the generated latex document. The footer should contain everything after -# the last chapter. If it is left blank doxygen will generate a -# standard footer. Notice: only use this tag if you know what you are doing! - -LATEX_FOOTER = - -# If the PDF_HYPERLINKS tag is set to YES, the LaTeX that is generated -# is prepared for conversion to pdf (using ps2pdf). The pdf file will -# contain links (just like the HTML output) instead of page references -# This makes the output suitable for online browsing using a pdf viewer. - -PDF_HYPERLINKS = YES - -# If the USE_PDFLATEX tag is set to YES, pdflatex will be used instead of -# plain latex in the generated Makefile. Set this option to YES to get a -# higher quality PDF documentation. - -USE_PDFLATEX = YES - -# If the LATEX_BATCHMODE tag is set to YES, doxygen will add the \\batchmode. -# command to the generated LaTeX files. This will instruct LaTeX to keep -# running if errors occur, instead of asking the user for help. -# This option is also used when generating formulas in HTML. - -LATEX_BATCHMODE = YES - -# If LATEX_HIDE_INDICES is set to YES then doxygen will not -# include the index chapters (such as File Index, Compound Index, etc.) -# in the output. - -LATEX_HIDE_INDICES = NO - -# If LATEX_SOURCE_CODE is set to YES then doxygen will include -# source code with syntax highlighting in the LaTeX output. -# Note that which sources are shown also depends on other settings -# such as SOURCE_BROWSER. - -LATEX_SOURCE_CODE = NO - -# The LATEX_BIB_STYLE tag can be used to specify the style to use for the -# bibliography, e.g. plainnat, or ieeetr. The default style is "plain". See -# http://en.wikipedia.org/wiki/BibTeX for more info. - -LATEX_BIB_STYLE = plain - -#--------------------------------------------------------------------------- -# configuration options related to the RTF output -#--------------------------------------------------------------------------- - -# If the GENERATE_RTF tag is set to YES Doxygen will generate RTF output -# The RTF output is optimized for Word 97 and may not look very pretty with -# other RTF readers or editors. - -GENERATE_RTF = NO - -# The RTF_OUTPUT tag is used to specify where the RTF docs will be put. -# If a relative path is entered the value of OUTPUT_DIRECTORY will be -# put in front of it. If left blank `rtf' will be used as the default path. - -RTF_OUTPUT = rtf - -# If the COMPACT_RTF tag is set to YES Doxygen generates more compact -# RTF documents. This may be useful for small projects and may help to -# save some trees in general. - -COMPACT_RTF = NO - -# If the RTF_HYPERLINKS tag is set to YES, the RTF that is generated -# will contain hyperlink fields. The RTF file will -# contain links (just like the HTML output) instead of page references. -# This makes the output suitable for online browsing using WORD or other -# programs which support those fields. -# Note: wordpad (write) and others do not support links. - -RTF_HYPERLINKS = NO - -# Load style sheet definitions from file. Syntax is similar to doxygen's -# config file, i.e. a series of assignments. You only have to provide -# replacements, missing definitions are set to their default value. - -RTF_STYLESHEET_FILE = - -# Set optional variables used in the generation of an rtf document. -# Syntax is similar to doxygen's config file. - -RTF_EXTENSIONS_FILE = - -#--------------------------------------------------------------------------- -# configuration options related to the man page output -#--------------------------------------------------------------------------- - -# If the GENERATE_MAN tag is set to YES (the default) Doxygen will -# generate man pages - -GENERATE_MAN = NO - -# The MAN_OUTPUT tag is used to specify where the man pages will be put. -# If a relative path is entered the value of OUTPUT_DIRECTORY will be -# put in front of it. If left blank `man' will be used as the default path. - -MAN_OUTPUT = man - -# The MAN_EXTENSION tag determines the extension that is added to -# the generated man pages (default is the subroutine's section .3) - -MAN_EXTENSION = .3 - -# If the MAN_LINKS tag is set to YES and Doxygen generates man output, -# then it will generate one additional man file for each entity -# documented in the real man page(s). These additional files -# only source the real man page, but without them the man command -# would be unable to find the correct page. The default is NO. - -MAN_LINKS = NO - -#--------------------------------------------------------------------------- -# configuration options related to the XML output -#--------------------------------------------------------------------------- - -# If the GENERATE_XML tag is set to YES Doxygen will -# generate an XML file that captures the structure of -# the code including all documentation. - -GENERATE_XML = NO - -# The XML_OUTPUT tag is used to specify where the XML pages will be put. -# If a relative path is entered the value of OUTPUT_DIRECTORY will be -# put in front of it. If left blank `xml' will be used as the default path. - -XML_OUTPUT = xml - -# The XML_SCHEMA tag can be used to specify an XML schema, -# which can be used by a validating XML parser to check the -# syntax of the XML files. - -XML_SCHEMA = - -# The XML_DTD tag can be used to specify an XML DTD, -# which can be used by a validating XML parser to check the -# syntax of the XML files. - -XML_DTD = - -# If the XML_PROGRAMLISTING tag is set to YES Doxygen will -# dump the program listings (including syntax highlighting -# and cross-referencing information) to the XML output. Note that -# enabling this will significantly increase the size of the XML output. - -XML_PROGRAMLISTING = NO - -#--------------------------------------------------------------------------- -# configuration options for the AutoGen Definitions output -#--------------------------------------------------------------------------- - -# If the GENERATE_AUTOGEN_DEF tag is set to YES Doxygen will -# generate an AutoGen Definitions (see autogen.sf.net) file -# that captures the structure of the code including all -# documentation. Note that this feature is still experimental -# and incomplete at the moment. - -GENERATE_AUTOGEN_DEF = NO - -#--------------------------------------------------------------------------- -# configuration options related to the Perl module output -#--------------------------------------------------------------------------- - -# If the GENERATE_PERLMOD tag is set to YES Doxygen will -# generate a Perl module file that captures the structure of -# the code including all documentation. Note that this -# feature is still experimental and incomplete at the -# moment. - -GENERATE_PERLMOD = NO - -# If the PERLMOD_LATEX tag is set to YES Doxygen will generate -# the necessary Makefile rules, Perl scripts and LaTeX code to be able -# to generate PDF and DVI output from the Perl module output. - -PERLMOD_LATEX = NO - -# If the PERLMOD_PRETTY tag is set to YES the Perl module output will be -# nicely formatted so it can be parsed by a human reader. This is useful -# if you want to understand what is going on. On the other hand, if this -# tag is set to NO the size of the Perl module output will be much smaller -# and Perl will parse it just the same. - -PERLMOD_PRETTY = YES - -# The names of the make variables in the generated doxyrules.make file -# are prefixed with the string contained in PERLMOD_MAKEVAR_PREFIX. -# This is useful so different doxyrules.make files included by the same -# Makefile don't overwrite each other's variables. - -PERLMOD_MAKEVAR_PREFIX = - -#--------------------------------------------------------------------------- -# Configuration options related to the preprocessor -#--------------------------------------------------------------------------- - -# If the ENABLE_PREPROCESSING tag is set to YES (the default) Doxygen will -# evaluate all C-preprocessor directives found in the sources and include -# files. - -ENABLE_PREPROCESSING = YES - -# If the MACRO_EXPANSION tag is set to YES Doxygen will expand all macro -# names in the source code. If set to NO (the default) only conditional -# compilation will be performed. Macro expansion can be done in a controlled -# way by setting EXPAND_ONLY_PREDEF to YES. - -MACRO_EXPANSION = NO - -# If the EXPAND_ONLY_PREDEF and MACRO_EXPANSION tags are both set to YES -# then the macro expansion is limited to the macros specified with the -# PREDEFINED and EXPAND_AS_DEFINED tags. - -EXPAND_ONLY_PREDEF = NO - -# If the SEARCH_INCLUDES tag is set to YES (the default) the includes files -# pointed to by INCLUDE_PATH will be searched when a #include is found. - -SEARCH_INCLUDES = YES - -# The INCLUDE_PATH tag can be used to specify one or more directories that -# contain include files that are not input files but should be processed by -# the preprocessor. - -INCLUDE_PATH = - -# You can use the INCLUDE_FILE_PATTERNS tag to specify one or more wildcard -# patterns (like *.h and *.hpp) to filter out the header-files in the -# directories. If left blank, the patterns specified with FILE_PATTERNS will -# be used. - -INCLUDE_FILE_PATTERNS = - -# The PREDEFINED tag can be used to specify one or more macro names that -# are defined before the preprocessor is started (similar to the -D option of -# gcc). The argument of the tag is a list of macros of the form: name -# or name=definition (no spaces). If the definition and the = are -# omitted =1 is assumed. To prevent a macro definition from being -# undefined via #undef or recursively expanded use the := operator -# instead of the = operator. - -PREDEFINED = - -# If the MACRO_EXPANSION and EXPAND_ONLY_PREDEF tags are set to YES then -# this tag can be used to specify a list of macro names that should be expanded. -# The macro definition that is found in the sources will be used. -# Use the PREDEFINED tag if you want to use a different macro definition that -# overrules the definition found in the source code. - -EXPAND_AS_DEFINED = - -# If the SKIP_FUNCTION_MACROS tag is set to YES (the default) then -# doxygen's preprocessor will remove all references to function-like macros -# that are alone on a line, have an all uppercase name, and do not end with a -# semicolon, because these will confuse the parser if not removed. - -SKIP_FUNCTION_MACROS = YES - -#--------------------------------------------------------------------------- -# Configuration::additions related to external references -#--------------------------------------------------------------------------- - -# The TAGFILES option can be used to specify one or more tagfiles. For each -# tag file the location of the external documentation should be added. The -# format of a tag file without this location is as follows: -# TAGFILES = file1 file2 ... -# Adding location for the tag files is done as follows: -# TAGFILES = file1=loc1 "file2 = loc2" ... -# where "loc1" and "loc2" can be relative or absolute paths -# or URLs. Note that each tag file must have a unique name (where the name does -# NOT include the path). If a tag file is not located in the directory in which -# doxygen is run, you must also specify the path to the tagfile here. - -TAGFILES = - -# When a file name is specified after GENERATE_TAGFILE, doxygen will create -# a tag file that is based on the input files it reads. - -GENERATE_TAGFILE = - -# If the ALLEXTERNALS tag is set to YES all external classes will be listed -# in the class index. If set to NO only the inherited external classes -# will be listed. - -ALLEXTERNALS = NO - -# If the EXTERNAL_GROUPS tag is set to YES all external groups will be listed -# in the modules index. If set to NO, only the current project's groups will -# be listed. - -EXTERNAL_GROUPS = YES - -# The PERL_PATH should be the absolute path and name of the perl script -# interpreter (i.e. the result of `which perl'). - -PERL_PATH = /usr/bin/perl - -#--------------------------------------------------------------------------- -# Configuration options related to the dot tool -#--------------------------------------------------------------------------- - -# If the CLASS_DIAGRAMS tag is set to YES (the default) Doxygen will -# generate a inheritance diagram (in HTML, RTF and LaTeX) for classes with base -# or super classes. Setting the tag to NO turns the diagrams off. Note that -# this option also works with HAVE_DOT disabled, but it is recommended to -# install and use dot, since it yields more powerful graphs. - -CLASS_DIAGRAMS = NO - -# You can define message sequence charts within doxygen comments using the \msc -# command. Doxygen will then run the mscgen tool (see -# http://www.mcternan.me.uk/mscgen/) to produce the chart and insert it in the -# documentation. The MSCGEN_PATH tag allows you to specify the directory where -# the mscgen tool resides. If left empty the tool is assumed to be found in the -# default search path. - -MSCGEN_PATH = - -# If set to YES, the inheritance and collaboration graphs will hide -# inheritance and usage relations if the target is undocumented -# or is not a class. - -HIDE_UNDOC_RELATIONS = YES - -# If you set the HAVE_DOT tag to YES then doxygen will assume the dot tool is -# available from the path. This tool is part of Graphviz, a graph visualization -# toolkit from AT&T and Lucent Bell Labs. The other options in this section -# have no effect if this option is set to NO (the default) - -HAVE_DOT = YES - -# The DOT_NUM_THREADS specifies the number of dot invocations doxygen is -# allowed to run in parallel. When set to 0 (the default) doxygen will -# base this on the number of processors available in the system. You can set it -# explicitly to a value larger than 0 to get control over the balance -# between CPU load and processing speed. - -DOT_NUM_THREADS = 0 - -# By default doxygen will use the Helvetica font for all dot files that -# doxygen generates. When you want a differently looking font you can specify -# the font name using DOT_FONTNAME. You need to make sure dot is able to find -# the font, which can be done by putting it in a standard location or by setting -# the DOTFONTPATH environment variable or by setting DOT_FONTPATH to the -# directory containing the font. - -DOT_FONTNAME = FreeSans.ttf - -# The DOT_FONTSIZE tag can be used to set the size of the font of dot graphs. -# The default size is 10pt. - -DOT_FONTSIZE = 10 - -# By default doxygen will tell dot to use the Helvetica font. -# If you specify a different font using DOT_FONTNAME you can use DOT_FONTPATH to -# set the path where dot can find it. - -DOT_FONTPATH = - -# If the CLASS_GRAPH and HAVE_DOT tags are set to YES then doxygen -# will generate a graph for each documented class showing the direct and -# indirect inheritance relations. Setting this tag to YES will force the -# CLASS_DIAGRAMS tag to NO. - -CLASS_GRAPH = YES - -# If the COLLABORATION_GRAPH and HAVE_DOT tags are set to YES then doxygen -# will generate a graph for each documented class showing the direct and -# indirect implementation dependencies (inheritance, containment, and -# class references variables) of the class with other documented classes. - -COLLABORATION_GRAPH = YES - -# If the GROUP_GRAPHS and HAVE_DOT tags are set to YES then doxygen -# will generate a graph for groups, showing the direct groups dependencies - -GROUP_GRAPHS = YES - -# If the UML_LOOK tag is set to YES doxygen will generate inheritance and -# collaboration diagrams in a style similar to the OMG's Unified Modeling -# Language. - -UML_LOOK = NO - -# If the UML_LOOK tag is enabled, the fields and methods are shown inside -# the class node. If there are many fields or methods and many nodes the -# graph may become too big to be useful. The UML_LIMIT_NUM_FIELDS -# threshold limits the number of items for each type to make the size more -# managable. Set this to 0 for no limit. Note that the threshold may be -# exceeded by 50% before the limit is enforced. - -UML_LIMIT_NUM_FIELDS = 10 - -# If set to YES, the inheritance and collaboration graphs will show the -# relations between templates and their instances. - -TEMPLATE_RELATIONS = NO - -# If the ENABLE_PREPROCESSING, SEARCH_INCLUDES, INCLUDE_GRAPH, and HAVE_DOT -# tags are set to YES then doxygen will generate a graph for each documented -# file showing the direct and indirect include dependencies of the file with -# other documented files. - -INCLUDE_GRAPH = YES - -# If the ENABLE_PREPROCESSING, SEARCH_INCLUDES, INCLUDED_BY_GRAPH, and -# HAVE_DOT tags are set to YES then doxygen will generate a graph for each -# documented header file showing the documented files that directly or -# indirectly include this file. - -INCLUDED_BY_GRAPH = NO - -# If the CALL_GRAPH and HAVE_DOT options are set to YES then -# doxygen will generate a call dependency graph for every global function -# or class method. Note that enabling this option will significantly increase -# the time of a run. So in most cases it will be better to enable call graphs -# for selected functions only using the \callgraph command. - -CALL_GRAPH = NO - -# If the CALLER_GRAPH and HAVE_DOT tags are set to YES then -# doxygen will generate a caller dependency graph for every global function -# or class method. Note that enabling this option will significantly increase -# the time of a run. So in most cases it will be better to enable caller -# graphs for selected functions only using the \callergraph command. - -CALLER_GRAPH = NO - -# If the GRAPHICAL_HIERARCHY and HAVE_DOT tags are set to YES then doxygen -# will generate a graphical hierarchy of all classes instead of a textual one. - -GRAPHICAL_HIERARCHY = YES - -# If the DIRECTORY_GRAPH and HAVE_DOT tags are set to YES -# then doxygen will show the dependencies a directory has on other directories -# in a graphical way. The dependency relations are determined by the #include -# relations between the files in the directories. - -DIRECTORY_GRAPH = YES - -# The DOT_IMAGE_FORMAT tag can be used to set the image format of the images -# generated by dot. Possible values are svg, png, jpg, or gif. -# If left blank png will be used. If you choose svg you need to set -# HTML_FILE_EXTENSION to xhtml in order to make the SVG files -# visible in IE 9+ (other browsers do not have this requirement). - -DOT_IMAGE_FORMAT = png - -# If DOT_IMAGE_FORMAT is set to svg, then this option can be set to YES to -# enable generation of interactive SVG images that allow zooming and panning. -# Note that this requires a modern browser other than Internet Explorer. -# Tested and working are Firefox, Chrome, Safari, and Opera. For IE 9+ you -# need to set HTML_FILE_EXTENSION to xhtml in order to make the SVG files -# visible. Older versions of IE do not have SVG support. - -INTERACTIVE_SVG = NO - -# The tag DOT_PATH can be used to specify the path where the dot tool can be -# found. If left blank, it is assumed the dot tool can be found in the path. - -DOT_PATH = - -# The DOTFILE_DIRS tag can be used to specify one or more directories that -# contain dot files that are included in the documentation (see the -# \dotfile command). - -DOTFILE_DIRS = - -# The MSCFILE_DIRS tag can be used to specify one or more directories that -# contain msc files that are included in the documentation (see the -# \mscfile command). - -MSCFILE_DIRS = - -# The DOT_GRAPH_MAX_NODES tag can be used to set the maximum number of -# nodes that will be shown in the graph. If the number of nodes in a graph -# becomes larger than this value, doxygen will truncate the graph, which is -# visualized by representing a node as a red box. Note that doxygen if the -# number of direct children of the root node in a graph is already larger than -# DOT_GRAPH_MAX_NODES then the graph will not be shown at all. Also note -# that the size of a graph can be further restricted by MAX_DOT_GRAPH_DEPTH. - -DOT_GRAPH_MAX_NODES = 50 - -# The MAX_DOT_GRAPH_DEPTH tag can be used to set the maximum depth of the -# graphs generated by dot. A depth value of 3 means that only nodes reachable -# from the root by following a path via at most 3 edges will be shown. Nodes -# that lay further from the root node will be omitted. Note that setting this -# option to 1 or 2 may greatly reduce the computation time needed for large -# code bases. Also note that the size of a graph can be further restricted by -# DOT_GRAPH_MAX_NODES. Using a depth of 0 means no depth restriction. - -MAX_DOT_GRAPH_DEPTH = 0 - -# Set the DOT_TRANSPARENT tag to YES to generate images with a transparent -# background. This is disabled by default, because dot on Windows does not -# seem to support this out of the box. Warning: Depending on the platform used, -# enabling this option may lead to badly anti-aliased labels on the edges of -# a graph (i.e. they become hard to read). - -DOT_TRANSPARENT = YES - -# Set the DOT_MULTI_TARGETS tag to YES allow dot to generate multiple output -# files in one run (i.e. multiple -o and -T options on the command line). This -# makes dot run faster, but since only newer versions of dot (>1.8.10) -# support this, this feature is disabled by default. - -DOT_MULTI_TARGETS = NO - -# If the GENERATE_LEGEND tag is set to YES (the default) Doxygen will -# generate a legend page explaining the meaning of the various boxes and -# arrows in the dot generated graphs. - -GENERATE_LEGEND = YES - -# If the DOT_CLEANUP tag is set to YES (the default) Doxygen will -# remove the intermediate dot files that are used to generate -# the various graphs. - -DOT_CLEANUP = YES +# Doxyfile 1.8.3.1 + +# This file describes the settings to be used by the documentation system +# doxygen (www.doxygen.org) for a project +# +# All text after a hash (#) is considered a comment and will be ignored +# The format is: +# TAG = value [value, ...] +# For lists items can also be appended using: +# TAG += value [value, ...] +# Values that contain spaces should be placed between quotes (" ") + +#--------------------------------------------------------------------------- +# Project related configuration options +#--------------------------------------------------------------------------- + +# This tag specifies the encoding used for all characters in the config file +# that follow. The default is UTF-8 which is also the encoding used for all +# text before the first occurrence of this tag. Doxygen uses libiconv (or the +# iconv built into libc) for the transcoding. See +# http://www.gnu.org/software/libiconv for the list of possible encodings. + +DOXYFILE_ENCODING = UTF-8 + +# The PROJECT_NAME tag is a single word (or sequence of words) that should +# identify the project. Note that if you do not use Doxywizard you need +# to put quotes around the project name if it contains spaces. + +PROJECT_NAME = SASfit + +# The PROJECT_NUMBER tag can be used to enter a project or revision number. +# This could be handy for archiving the generated documentation or +# if some version control system is used. + +PROJECT_NUMBER = 0.94.10 + +# Using the PROJECT_BRIEF tag one can provide an optional one line description +# for a project that appears at the top of each page and should give viewer +# a quick idea about the purpose of the project. Keep the description short. + +PROJECT_BRIEF = + +# With the PROJECT_LOGO tag one can specify an logo or icon that is +# included in the documentation. The maximum height of the logo should not +# exceed 55 pixels and the maximum width should not exceed 200 pixels. +# Doxygen will copy the logo to the output directory. + +PROJECT_LOGO = ../doc/images/sasfit_icon_base_75x75.png + +# The OUTPUT_DIRECTORY tag is used to specify the (relative or absolute) +# base path where the generated documentation will be put. +# If a relative path is entered, it will be relative to the location +# where doxygen was started. If left blank the current directory will be used. + +OUTPUT_DIRECTORY = ../doc + +# If the CREATE_SUBDIRS tag is set to YES, then doxygen will create +# 4096 sub-directories (in 2 levels) under the output directory of each output +# format and will distribute the generated files over these directories. +# Enabling this option can be useful when feeding doxygen a huge amount of +# source files, where putting all generated files in the same directory would +# otherwise cause performance problems for the file system. + +CREATE_SUBDIRS = NO + +# The OUTPUT_LANGUAGE tag is used to specify the language in which all +# documentation generated by doxygen is written. Doxygen will use this +# information to generate all constant output in the proper language. +# The default language is English, other supported languages are: +# Afrikaans, Arabic, Brazilian, Catalan, Chinese, Chinese-Traditional, +# Croatian, Czech, Danish, Dutch, Esperanto, Farsi, Finnish, French, German, +# Greek, Hungarian, Italian, Japanese, Japanese-en (Japanese with English +# messages), Korean, Korean-en, Lithuanian, Norwegian, Macedonian, Persian, +# Polish, Portuguese, Romanian, Russian, Serbian, Serbian-Cyrillic, Slovak, +# Slovene, Spanish, Swedish, Ukrainian, and Vietnamese. + +OUTPUT_LANGUAGE = English + +# If the BRIEF_MEMBER_DESC tag is set to YES (the default) Doxygen will +# include brief member descriptions after the members that are listed in +# the file and class documentation (similar to JavaDoc). +# Set to NO to disable this. + +BRIEF_MEMBER_DESC = YES + +# If the REPEAT_BRIEF tag is set to YES (the default) Doxygen will prepend +# the brief description of a member or function before the detailed description. +# Note: if both HIDE_UNDOC_MEMBERS and BRIEF_MEMBER_DESC are set to NO, the +# brief descriptions will be completely suppressed. + +REPEAT_BRIEF = YES + +# This tag implements a quasi-intelligent brief description abbreviator +# that is used to form the text in various listings. Each string +# in this list, if found as the leading text of the brief description, will be +# stripped from the text and the result after processing the whole list, is +# used as the annotated text. Otherwise, the brief description is used as-is. +# If left blank, the following values are used ("$name" is automatically +# replaced with the name of the entity): "The $name class" "The $name widget" +# "The $name file" "is" "provides" "specifies" "contains" +# "represents" "a" "an" "the" + +ABBREVIATE_BRIEF = + +# If the ALWAYS_DETAILED_SEC and REPEAT_BRIEF tags are both set to YES then +# Doxygen will generate a detailed section even if there is only a brief +# description. + +ALWAYS_DETAILED_SEC = NO + +# If the INLINE_INHERITED_MEMB tag is set to YES, doxygen will show all +# inherited members of a class in the documentation of that class as if those +# members were ordinary class members. Constructors, destructors and assignment +# operators of the base classes will not be shown. + +INLINE_INHERITED_MEMB = NO + +# If the FULL_PATH_NAMES tag is set to YES then Doxygen will prepend the full +# path before files name in the file list and in the header files. If set +# to NO the shortest path that makes the file name unique will be used. + +FULL_PATH_NAMES = YES + +# If the FULL_PATH_NAMES tag is set to YES then the STRIP_FROM_PATH tag +# can be used to strip a user-defined part of the path. Stripping is +# only done if one of the specified strings matches the left-hand part of +# the path. The tag can be used to show relative paths in the file list. +# If left blank the directory from which doxygen is run is used as the +# path to strip. Note that you specify absolute paths here, but also +# relative paths, which will be relative from the directory where doxygen is +# started. + +STRIP_FROM_PATH = + +# The STRIP_FROM_INC_PATH tag can be used to strip a user-defined part of +# the path mentioned in the documentation of a class, which tells +# the reader which header file to include in order to use a class. +# If left blank only the name of the header file containing the class +# definition is used. Otherwise one should specify the include paths that +# are normally passed to the compiler using the -I flag. + +STRIP_FROM_INC_PATH = + +# If the SHORT_NAMES tag is set to YES, doxygen will generate much shorter +# (but less readable) file names. This can be useful if your file system +# doesn't support long names like on DOS, Mac, or CD-ROM. + +SHORT_NAMES = NO + +# If the JAVADOC_AUTOBRIEF tag is set to YES then Doxygen +# will interpret the first line (until the first dot) of a JavaDoc-style +# comment as the brief description. If set to NO, the JavaDoc +# comments will behave just like regular Qt-style comments +# (thus requiring an explicit @brief command for a brief description.) + +JAVADOC_AUTOBRIEF = YES + +# If the QT_AUTOBRIEF tag is set to YES then Doxygen will +# interpret the first line (until the first dot) of a Qt-style +# comment as the brief description. If set to NO, the comments +# will behave just like regular Qt-style comments (thus requiring +# an explicit \brief command for a brief description.) + +QT_AUTOBRIEF = NO + +# The MULTILINE_CPP_IS_BRIEF tag can be set to YES to make Doxygen +# treat a multi-line C++ special comment block (i.e. a block of //! or /// +# comments) as a brief description. This used to be the default behaviour. +# The new default is to treat a multi-line C++ comment block as a detailed +# description. Set this tag to YES if you prefer the old behaviour instead. + +MULTILINE_CPP_IS_BRIEF = NO + +# If the INHERIT_DOCS tag is set to YES (the default) then an undocumented +# member inherits the documentation from any documented member that it +# re-implements. + +INHERIT_DOCS = YES + +# If the SEPARATE_MEMBER_PAGES tag is set to YES, then doxygen will produce +# a new page for each member. If set to NO, the documentation of a member will +# be part of the file/class/namespace that contains it. + +SEPARATE_MEMBER_PAGES = NO + +# The TAB_SIZE tag can be used to set the number of spaces in a tab. +# Doxygen uses this value to replace tabs by spaces in code fragments. + +TAB_SIZE = 8 + +# This tag can be used to specify a number of aliases that acts +# as commands in the documentation. An alias has the form "name=value". +# For example adding "sideeffect=\par Side Effects:\n" will allow you to +# put the command \sideeffect (or @sideeffect) in the documentation, which +# will result in a user-defined paragraph with heading "Side Effects:". +# You can put \n's in the value part of an alias to insert newlines. + +ALIASES = "modname{1}=\note The module group name is '\1' (used for plugin group membership)." \ + "toplvldescr{3}=
All \1 functions are of type \ref sasfit_func_one_t : \param q The current data point of the scattering vector. \param p Pointer to a \ref sasfit_param structure containing an array of parameter values.
The order is defined by each \1 function itself.
See its documentation (plugins) or implementation (old style) to get clarity about that. \returns The value of the \1 for the scattering vector value q. \see \ref howto_use_old \modname{\3}" \ + "vs=Microsoft Visual Studio 2005" \ + "vs_select_rel=Select 'Release' mode for this project in the symbol bar at the top." \ + "vs_build=Right-Click on the project in the solution explorer and select \e Build or \e Rebuild." \ + "vs_new_proj=Create a new project (console application) using the existing source code in \\examples. ('File' -> 'New' -> 'Project From Existing Code').\n Choose a project name and a project file location. On the next form, select 'Use Visual Studio' and 'Console application project'. When done, press 'finish' to quit this dialog." \ + "vs_select_file{1}=\vs_select_rel\n In the solution explorer, make sure that just \1 is part of it: Remove all additional files (Right-click on them and select 'Exclude From Project'). Then, right-click on the project itself and select 'Properties'." \ + "vs_add_inc{2}=In the left subwindow select 'Configuration Properties'->'C/C++'->'General'.\n Edit the entry 'Additional Include Directories' within the right subwindow: It's supposed to be empty. Add the following directories:
    \1
\2\n" \ + "vs_add_lib{2}=In the next step, select 'Configuration Properties'->'Linker'->'General' from the left subwindow and modify the entry 'Additional Library Directories' by adding
    \1
\2\n (\vs needs \e *.lib files for building, not runtime \e *.dll files)" \ + "vs_add_deps{1}=Additionally, you have to modify the entry 'Additional Dependencies' by selecting 'Configuration Properties'->'Linker'->'Input' on the left side. Enter the following library file names:
    \1
\n" \ + "vs_do_build{1}=Next, close the properties window and \vs_build When there were no errors, directory \1 (or the previously selected project file location) should contain an executable with the name of the project as listed in the solution explorer." \ + "vs_redistrib_note=On Windows systems where no \vs is installed, you also need to have the redistributable files in PATH. For sasfit they are: 'Microsoft.VC80.CRT.manifest' and 'msvcr80.dll' (if build with \vs). They are located in \vs-install-dir\\VC\\redist\\x86\\Microsoft.VC80.CRT ." \ + "win_lib_path{1}=To run this program, \1 is required. The easiest method for testing is to copy it into the same directory where the executable resides. \n Alternatively, you could add its path \sf_src\\src\\lib\\ to your systems 'PATH' environment variable or copy the library file to one of the directories in PATH. Execute echo \%PATH\% on the command prompt to see what those directories are. \n" \ + "memberof{1}=" \ + "sf_src=" \ + "sf_grp_def=groups.*.def in \sf_src/src/plugins" \ + "sf=SASfit" \ + "pb{1}=\" \ + "pn=\pb{next}" \ + "qt{1}="\1"" \ + "path{1}=\1" \ + "lnk{2}=\1" \ + "build_results{3}=If everything went fine, there is a shared (*.\1) and eventually a static (*.\2) library file in \n\n \sf_src\3src\3lib. \n\n The shared library file is copied to \n\n \sf_src\3sasfit.vfs\3lib\3Sasfit \n\n automatically (for starpack creation). In addition, each library file of a plugin as well as its public header file is automatically copied to \n\n \sf_src\3plugins. \n\n" + +# This tag can be used to specify a number of word-keyword mappings (TCL only). +# A mapping has the form "name=value". For example adding +# "class=itcl::class" will allow you to use the command class in the +# itcl::class meaning. + +TCL_SUBST = + +# Set the OPTIMIZE_OUTPUT_FOR_C tag to YES if your project consists of C +# sources only. Doxygen will then generate output that is more tailored for C. +# For instance, some of the names that are used will be different. The list +# of all members will be omitted, etc. + +OPTIMIZE_OUTPUT_FOR_C = YES + +# Set the OPTIMIZE_OUTPUT_JAVA tag to YES if your project consists of Java +# sources only. Doxygen will then generate output that is more tailored for +# Java. For instance, namespaces will be presented as packages, qualified +# scopes will look different, etc. + +OPTIMIZE_OUTPUT_JAVA = NO + +# Set the OPTIMIZE_FOR_FORTRAN tag to YES if your project consists of Fortran +# sources only. Doxygen will then generate output that is more tailored for +# Fortran. + +OPTIMIZE_FOR_FORTRAN = NO + +# Set the OPTIMIZE_OUTPUT_VHDL tag to YES if your project consists of VHDL +# sources. Doxygen will then generate output that is tailored for +# VHDL. + +OPTIMIZE_OUTPUT_VHDL = NO + +# Doxygen selects the parser to use depending on the extension of the files it +# parses. With this tag you can assign which parser to use for a given +# extension. Doxygen has a built-in mapping, but you can override or extend it +# using this tag. The format is ext=language, where ext is a file extension, +# and language is one of the parsers supported by doxygen: IDL, Java, +# Javascript, CSharp, C, C++, D, PHP, Objective-C, Python, Fortran, VHDL, C, +# C++. For instance to make doxygen treat .inc files as Fortran files (default +# is PHP), and .f files as C (default is Fortran), use: inc=Fortran f=C. Note +# that for custom extensions you also need to set FILE_PATTERNS otherwise the +# files are not read by doxygen. + +EXTENSION_MAPPING = + +# If MARKDOWN_SUPPORT is enabled (the default) then doxygen pre-processes all +# comments according to the Markdown format, which allows for more readable +# documentation. See http://daringfireball.net/projects/markdown/ for details. +# The output of markdown processing is further processed by doxygen, so you +# can mix doxygen, HTML, and XML commands with Markdown formatting. +# Disable only in case of backward compatibilities issues. + +MARKDOWN_SUPPORT = YES + +# When enabled doxygen tries to link words that correspond to documented classes, +# or namespaces to their corresponding documentation. Such a link can be +# prevented in individual cases by by putting a % sign in front of the word or +# globally by setting AUTOLINK_SUPPORT to NO. + +AUTOLINK_SUPPORT = YES + +# If you use STL classes (i.e. std::string, std::vector, etc.) but do not want +# to include (a tag file for) the STL sources as input, then you should +# set this tag to YES in order to let doxygen match functions declarations and +# definitions whose arguments contain STL classes (e.g. func(std::string) v.s. +# func(std::string) {}). This also makes the inheritance and collaboration +# diagrams that involve STL classes more complete and accurate. + +BUILTIN_STL_SUPPORT = NO + +# If you use Microsoft's C++/CLI language, you should set this option to YES to +# enable parsing support. + +CPP_CLI_SUPPORT = NO + +# Set the SIP_SUPPORT tag to YES if your project consists of sip sources only. +# Doxygen will parse them like normal C++ but will assume all classes use public +# instead of private inheritance when no explicit protection keyword is present. + +SIP_SUPPORT = NO + +# For Microsoft's IDL there are propget and propput attributes to indicate +# getter and setter methods for a property. Setting this option to YES (the +# default) will make doxygen replace the get and set methods by a property in +# the documentation. This will only work if the methods are indeed getting or +# setting a simple type. If this is not the case, or you want to show the +# methods anyway, you should set this option to NO. + +IDL_PROPERTY_SUPPORT = YES + +# If member grouping is used in the documentation and the DISTRIBUTE_GROUP_DOC +# tag is set to YES, then doxygen will reuse the documentation of the first +# member in the group (if any) for the other members of the group. By default +# all members of a group must be documented explicitly. + +DISTRIBUTE_GROUP_DOC = NO + +# Set the SUBGROUPING tag to YES (the default) to allow class member groups of +# the same type (for instance a group of public functions) to be put as a +# subgroup of that type (e.g. under the Public Functions section). Set it to +# NO to prevent subgrouping. Alternatively, this can be done per class using +# the \nosubgrouping command. + +SUBGROUPING = YES + +# When the INLINE_GROUPED_CLASSES tag is set to YES, classes, structs and +# unions are shown inside the group in which they are included (e.g. using +# @ingroup) instead of on a separate page (for HTML and Man pages) or +# section (for LaTeX and RTF). + +INLINE_GROUPED_CLASSES = NO + +# When the INLINE_SIMPLE_STRUCTS tag is set to YES, structs, classes, and +# unions with only public data fields will be shown inline in the documentation +# of the scope in which they are defined (i.e. file, namespace, or group +# documentation), provided this scope is documented. If set to NO (the default), +# structs, classes, and unions are shown on a separate page (for HTML and Man +# pages) or section (for LaTeX and RTF). + +INLINE_SIMPLE_STRUCTS = NO + +# When TYPEDEF_HIDES_STRUCT is enabled, a typedef of a struct, union, or enum +# is documented as struct, union, or enum with the name of the typedef. So +# typedef struct TypeS {} TypeT, will appear in the documentation as a struct +# with name TypeT. When disabled the typedef will appear as a member of a file, +# namespace, or class. And the struct will be named TypeS. This can typically +# be useful for C code in case the coding convention dictates that all compound +# types are typedef'ed and only the typedef is referenced, never the tag name. + +TYPEDEF_HIDES_STRUCT = NO + +# The SYMBOL_CACHE_SIZE determines the size of the internal cache use to +# determine which symbols to keep in memory and which to flush to disk. +# When the cache is full, less often used symbols will be written to disk. +# For small to medium size projects (<1000 input files) the default value is +# probably good enough. For larger projects a too small cache size can cause +# doxygen to be busy swapping symbols to and from disk most of the time +# causing a significant performance penalty. +# If the system has enough physical memory increasing the cache will improve the +# performance by keeping more symbols in memory. Note that the value works on +# a logarithmic scale so increasing the size by one will roughly double the +# memory usage. The cache size is given by this formula: +# 2^(16+SYMBOL_CACHE_SIZE). The valid range is 0..9, the default is 0, +# corresponding to a cache size of 2^16 = 65536 symbols. + +SYMBOL_CACHE_SIZE = 0 + +# Similar to the SYMBOL_CACHE_SIZE the size of the symbol lookup cache can be +# set using LOOKUP_CACHE_SIZE. This cache is used to resolve symbols given +# their name and scope. Since this can be an expensive process and often the +# same symbol appear multiple times in the code, doxygen keeps a cache of +# pre-resolved symbols. If the cache is too small doxygen will become slower. +# If the cache is too large, memory is wasted. The cache size is given by this +# formula: 2^(16+LOOKUP_CACHE_SIZE). The valid range is 0..9, the default is 0, +# corresponding to a cache size of 2^16 = 65536 symbols. + +LOOKUP_CACHE_SIZE = 0 + +#--------------------------------------------------------------------------- +# Build related configuration options +#--------------------------------------------------------------------------- + +# If the EXTRACT_ALL tag is set to YES doxygen will assume all entities in +# documentation are documented, even if no documentation was available. +# Private class members and static file members will be hidden unless +# the EXTRACT_PRIVATE and EXTRACT_STATIC tags are set to YES + +EXTRACT_ALL = YES + +# If the EXTRACT_PRIVATE tag is set to YES all private members of a class +# will be included in the documentation. + +EXTRACT_PRIVATE = NO + +# If the EXTRACT_PACKAGE tag is set to YES all members with package or internal +# scope will be included in the documentation. + +EXTRACT_PACKAGE = NO + +# If the EXTRACT_STATIC tag is set to YES all static members of a file +# will be included in the documentation. + +EXTRACT_STATIC = NO + +# If the EXTRACT_LOCAL_CLASSES tag is set to YES classes (and structs) +# defined locally in source files will be included in the documentation. +# If set to NO only classes defined in header files are included. + +EXTRACT_LOCAL_CLASSES = YES + +# This flag is only useful for Objective-C code. When set to YES local +# methods, which are defined in the implementation section but not in +# the interface are included in the documentation. +# If set to NO (the default) only methods in the interface are included. + +EXTRACT_LOCAL_METHODS = NO + +# If this flag is set to YES, the members of anonymous namespaces will be +# extracted and appear in the documentation as a namespace called +# 'anonymous_namespace{file}', where file will be replaced with the base +# name of the file that contains the anonymous namespace. By default +# anonymous namespaces are hidden. + +EXTRACT_ANON_NSPACES = NO + +# If the HIDE_UNDOC_MEMBERS tag is set to YES, Doxygen will hide all +# undocumented members of documented classes, files or namespaces. +# If set to NO (the default) these members will be included in the +# various overviews, but no documentation section is generated. +# This option has no effect if EXTRACT_ALL is enabled. + +HIDE_UNDOC_MEMBERS = NO + +# If the HIDE_UNDOC_CLASSES tag is set to YES, Doxygen will hide all +# undocumented classes that are normally visible in the class hierarchy. +# If set to NO (the default) these classes will be included in the various +# overviews. This option has no effect if EXTRACT_ALL is enabled. + +HIDE_UNDOC_CLASSES = NO + +# If the HIDE_FRIEND_COMPOUNDS tag is set to YES, Doxygen will hide all +# friend (class|struct|union) declarations. +# If set to NO (the default) these declarations will be included in the +# documentation. + +HIDE_FRIEND_COMPOUNDS = NO + +# If the HIDE_IN_BODY_DOCS tag is set to YES, Doxygen will hide any +# documentation blocks found inside the body of a function. +# If set to NO (the default) these blocks will be appended to the +# function's detailed documentation block. + +HIDE_IN_BODY_DOCS = NO + +# The INTERNAL_DOCS tag determines if documentation +# that is typed after a \internal command is included. If the tag is set +# to NO (the default) then the documentation will be excluded. +# Set it to YES to include the internal documentation. + +INTERNAL_DOCS = NO + +# If the CASE_SENSE_NAMES tag is set to NO then Doxygen will only generate +# file names in lower-case letters. If set to YES upper-case letters are also +# allowed. This is useful if you have classes or files whose names only differ +# in case and if your file system supports case sensitive file names. Windows +# and Mac users are advised to set this option to NO. + +CASE_SENSE_NAMES = NO + +# If the HIDE_SCOPE_NAMES tag is set to NO (the default) then Doxygen +# will show members with their full class and namespace scopes in the +# documentation. If set to YES the scope will be hidden. + +HIDE_SCOPE_NAMES = NO + +# If the SHOW_INCLUDE_FILES tag is set to YES (the default) then Doxygen +# will put a list of the files that are included by a file in the documentation +# of that file. + +SHOW_INCLUDE_FILES = YES + +# If the FORCE_LOCAL_INCLUDES tag is set to YES then Doxygen +# will list include files with double quotes in the documentation +# rather than with sharp brackets. + +FORCE_LOCAL_INCLUDES = NO + +# If the INLINE_INFO tag is set to YES (the default) then a tag [inline] +# is inserted in the documentation for inline members. + +INLINE_INFO = YES + +# If the SORT_MEMBER_DOCS tag is set to YES (the default) then doxygen +# will sort the (detailed) documentation of file and class members +# alphabetically by member name. If set to NO the members will appear in +# declaration order. + +SORT_MEMBER_DOCS = YES + +# If the SORT_BRIEF_DOCS tag is set to YES then doxygen will sort the +# brief documentation of file, namespace and class members alphabetically +# by member name. If set to NO (the default) the members will appear in +# declaration order. + +SORT_BRIEF_DOCS = NO + +# If the SORT_MEMBERS_CTORS_1ST tag is set to YES then doxygen +# will sort the (brief and detailed) documentation of class members so that +# constructors and destructors are listed first. If set to NO (the default) +# the constructors will appear in the respective orders defined by +# SORT_MEMBER_DOCS and SORT_BRIEF_DOCS. +# This tag will be ignored for brief docs if SORT_BRIEF_DOCS is set to NO +# and ignored for detailed docs if SORT_MEMBER_DOCS is set to NO. + +SORT_MEMBERS_CTORS_1ST = NO + +# If the SORT_GROUP_NAMES tag is set to YES then doxygen will sort the +# hierarchy of group names into alphabetical order. If set to NO (the default) +# the group names will appear in their defined order. + +SORT_GROUP_NAMES = NO + +# If the SORT_BY_SCOPE_NAME tag is set to YES, the class list will be +# sorted by fully-qualified names, including namespaces. If set to +# NO (the default), the class list will be sorted only by class name, +# not including the namespace part. +# Note: This option is not very useful if HIDE_SCOPE_NAMES is set to YES. +# Note: This option applies only to the class list, not to the +# alphabetical list. + +SORT_BY_SCOPE_NAME = NO + +# If the STRICT_PROTO_MATCHING option is enabled and doxygen fails to +# do proper type resolution of all parameters of a function it will reject a +# match between the prototype and the implementation of a member function even +# if there is only one candidate or it is obvious which candidate to choose +# by doing a simple string match. By disabling STRICT_PROTO_MATCHING doxygen +# will still accept a match between prototype and implementation in such cases. + +STRICT_PROTO_MATCHING = NO + +# The GENERATE_TODOLIST tag can be used to enable (YES) or +# disable (NO) the todo list. This list is created by putting \todo +# commands in the documentation. + +GENERATE_TODOLIST = YES + +# The GENERATE_TESTLIST tag can be used to enable (YES) or +# disable (NO) the test list. This list is created by putting \test +# commands in the documentation. + +GENERATE_TESTLIST = YES + +# The GENERATE_BUGLIST tag can be used to enable (YES) or +# disable (NO) the bug list. This list is created by putting \bug +# commands in the documentation. + +GENERATE_BUGLIST = YES + +# The GENERATE_DEPRECATEDLIST tag can be used to enable (YES) or +# disable (NO) the deprecated list. This list is created by putting +# \deprecated commands in the documentation. + +GENERATE_DEPRECATEDLIST= YES + +# The ENABLED_SECTIONS tag can be used to enable conditional +# documentation sections, marked by \if section-label ... \endif +# and \cond section-label ... \endcond blocks. + +ENABLED_SECTIONS = + +# The MAX_INITIALIZER_LINES tag determines the maximum number of lines +# the initial value of a variable or macro consists of for it to appear in +# the documentation. If the initializer consists of more lines than specified +# here it will be hidden. Use a value of 0 to hide initializers completely. +# The appearance of the initializer of individual variables and macros in the +# documentation can be controlled using \showinitializer or \hideinitializer +# command in the documentation regardless of this setting. + +MAX_INITIALIZER_LINES = 30 + +# Set the SHOW_USED_FILES tag to NO to disable the list of files generated +# at the bottom of the documentation of classes and structs. If set to YES the +# list will mention the files that were used to generate the documentation. + +SHOW_USED_FILES = YES + +# Set the SHOW_FILES tag to NO to disable the generation of the Files page. +# This will remove the Files entry from the Quick Index and from the +# Folder Tree View (if specified). The default is YES. + +SHOW_FILES = YES + +# Set the SHOW_NAMESPACES tag to NO to disable the generation of the +# Namespaces page. This will remove the Namespaces entry from the Quick Index +# and from the Folder Tree View (if specified). The default is YES. + +SHOW_NAMESPACES = YES + +# The FILE_VERSION_FILTER tag can be used to specify a program or script that +# doxygen should invoke to get the current version for each file (typically from +# the version control system). Doxygen will invoke the program by executing (via +# popen()) the command , where is the value of +# the FILE_VERSION_FILTER tag, and is the name of an input file +# provided by doxygen. Whatever the program writes to standard output +# is used as the file version. See the manual for examples. + +FILE_VERSION_FILTER = + +# The LAYOUT_FILE tag can be used to specify a layout file which will be parsed +# by doxygen. The layout file controls the global structure of the generated +# output files in an output format independent way. To create the layout file +# that represents doxygen's defaults, run doxygen with the -l option. +# You can optionally specify a file name after the option, if omitted +# DoxygenLayout.xml will be used as the name of the layout file. + +LAYOUT_FILE = + +# The CITE_BIB_FILES tag can be used to specify one or more bib files +# containing the references data. This must be a list of .bib files. The +# .bib extension is automatically appended if omitted. Using this command +# requires the bibtex tool to be installed. See also +# http://en.wikipedia.org/wiki/BibTeX for more info. For LaTeX the style +# of the bibliography can be controlled using LATEX_BIB_STYLE. To use this +# feature you need bibtex and perl available in the search path. Do not use +# file names with spaces, bibtex cannot handle them. + +CITE_BIB_FILES = + +#--------------------------------------------------------------------------- +# configuration options related to warning and progress messages +#--------------------------------------------------------------------------- + +# The QUIET tag can be used to turn on/off the messages that are generated +# by doxygen. Possible values are YES and NO. If left blank NO is used. + +QUIET = NO + +# The WARNINGS tag can be used to turn on/off the warning messages that are +# generated by doxygen. Possible values are YES and NO. If left blank +# NO is used. + +WARNINGS = YES + +# If WARN_IF_UNDOCUMENTED is set to YES, then doxygen will generate warnings +# for undocumented members. If EXTRACT_ALL is set to YES then this flag will +# automatically be disabled. + +WARN_IF_UNDOCUMENTED = YES + +# If WARN_IF_DOC_ERROR is set to YES, doxygen will generate warnings for +# potential errors in the documentation, such as not documenting some +# parameters in a documented function, or documenting parameters that +# don't exist or using markup commands wrongly. + +WARN_IF_DOC_ERROR = YES + +# The WARN_NO_PARAMDOC option can be enabled to get warnings for +# functions that are documented, but have no documentation for their parameters +# or return value. If set to NO (the default) doxygen will only warn about +# wrong or incomplete parameter documentation, but not about the absence of +# documentation. + +WARN_NO_PARAMDOC = NO + +# The WARN_FORMAT tag determines the format of the warning messages that +# doxygen can produce. The string should contain the $file, $line, and $text +# tags, which will be replaced by the file and line number from which the +# warning originated and the warning text. Optionally the format may contain +# $version, which will be replaced by the version of the file (if it could +# be obtained via FILE_VERSION_FILTER) + +WARN_FORMAT = "$file:$line: $text" + +# The WARN_LOGFILE tag can be used to specify a file to which warning +# and error messages should be written. If left blank the output is written +# to stderr. + +WARN_LOGFILE = + +#--------------------------------------------------------------------------- +# configuration options related to the input files +#--------------------------------------------------------------------------- + +# The INPUT tag can be used to specify the files and/or directories that contain +# documented source files. You may enter file names like "myfile.cpp" or +# directories like "/usr/src/myproject". Separate the files or directories +# with spaces. + +INPUT = doc \ + sasfit_common \ + sasfit_sd \ + sasfit_sq \ + sasfit_peaks \ + sasfit_ff \ + sasfit_core \ + sasfit_old \ + plugins + +# This tag can be used to specify the character encoding of the source files +# that doxygen parses. Internally doxygen uses the UTF-8 encoding, which is +# also the default input encoding. Doxygen uses libiconv (or the iconv built +# into libc) for the transcoding. See http://www.gnu.org/software/libiconv for +# the list of possible encodings. + +INPUT_ENCODING = UTF-8 + +# If the value of the INPUT tag contains directories, you can use the +# FILE_PATTERNS tag to specify one or more wildcard pattern (like *.cpp +# and *.h) to filter out the source-files in the directories. If left +# blank the following patterns are tested: +# *.c *.cc *.cxx *.cpp *.c++ *.d *.java *.ii *.ixx *.ipp *.i++ *.inl *.h *.hh +# *.hxx *.hpp *.h++ *.idl *.odl *.cs *.php *.php3 *.inc *.m *.mm *.dox *.py +# *.f90 *.f *.for *.vhd *.vhdl + +FILE_PATTERNS = *.c \ + *.h \ + *.def + +# The RECURSIVE tag can be used to turn specify whether or not subdirectories +# should be searched for input files as well. Possible values are YES and NO. +# If left blank NO is used. + +RECURSIVE = YES + +# The EXCLUDE tag can be used to specify files and/or directories that should be +# excluded from the INPUT source files. This way you can easily exclude a +# subdirectory from a directory tree whose root is specified with the INPUT tag. +# Note that relative paths are relative to the directory from which doxygen is +# run. + +EXCLUDE = + +# The EXCLUDE_SYMLINKS tag can be used to select whether or not files or +# directories that are symbolic links (a Unix file system feature) are excluded +# from the input. + +EXCLUDE_SYMLINKS = YES + +# If the value of the INPUT tag contains directories, you can use the +# EXCLUDE_PATTERNS tag to specify one or more wildcard patterns to exclude +# certain files from those directories. Note that the wildcards are matched +# against the file with absolute path, so to exclude all test directories +# for example use the pattern */test/* + +EXCLUDE_PATTERNS = *.dir \ + .svn \ + */CMakeFiles \ + */lib + +# The EXCLUDE_SYMBOLS tag can be used to specify one or more symbol names +# (namespaces, classes, functions, etc.) that should be excluded from the +# output. The symbol name can be a fully qualified name, a word, or if the +# wildcard * is used, a substring. Examples: ANamespace, AClass, +# AClass::ANamespace, ANamespace::*Test + +EXCLUDE_SYMBOLS = + +# The EXAMPLE_PATH tag can be used to specify one or more files or +# directories that contain example code fragments that are included (see +# the \include command). + +EXAMPLE_PATH = ../examples/ + +# If the value of the EXAMPLE_PATH tag contains directories, you can use the +# EXAMPLE_PATTERNS tag to specify one or more wildcard pattern (like *.cpp +# and *.h) to filter out the source-files in the directories. If left +# blank all files are included. + +EXAMPLE_PATTERNS = *.c + +# If the EXAMPLE_RECURSIVE tag is set to YES then subdirectories will be +# searched for input files to be used with the \include or \dontinclude +# commands irrespective of the value of the RECURSIVE tag. +# Possible values are YES and NO. If left blank NO is used. + +EXAMPLE_RECURSIVE = NO + +# The IMAGE_PATH tag can be used to specify one or more files or +# directories that contain image that are included in the documentation (see +# the \image command). + +IMAGE_PATH = ../doc/images/ + +# The INPUT_FILTER tag can be used to specify a program that doxygen should +# invoke to filter for each input file. Doxygen will invoke the filter program +# by executing (via popen()) the command , where +# is the value of the INPUT_FILTER tag, and is the name of an +# input file. Doxygen will then use the output that the filter program writes +# to standard output. If FILTER_PATTERNS is specified, this tag will be +# ignored. + +INPUT_FILTER = + +# The FILTER_PATTERNS tag can be used to specify filters on a per file pattern +# basis. Doxygen will compare the file name with each pattern and apply the +# filter if there is a match. The filters are a list of the form: +# pattern=filter (like *.cpp=my_cpp_filter). See INPUT_FILTER for further +# info on how filters are used. If FILTER_PATTERNS is empty or if +# non of the patterns match the file name, INPUT_FILTER is applied. + +FILTER_PATTERNS = + +# If the FILTER_SOURCE_FILES tag is set to YES, the input filter (if set using +# INPUT_FILTER) will be used to filter the input files when producing source +# files to browse (i.e. when SOURCE_BROWSER is set to YES). + +FILTER_SOURCE_FILES = NO + +# The FILTER_SOURCE_PATTERNS tag can be used to specify source filters per file +# pattern. A pattern will override the setting for FILTER_PATTERN (if any) +# and it is also possible to disable source filtering for a specific pattern +# using *.ext= (so without naming a filter). This option only has effect when +# FILTER_SOURCE_FILES is enabled. + +FILTER_SOURCE_PATTERNS = + +# If the USE_MD_FILE_AS_MAINPAGE tag refers to the name of a markdown file that +# is part of the input, its contents will be placed on the main page (index.html). +# This can be useful if you have a project on for instance GitHub and want reuse +# the introduction page also for the doxygen output. + +USE_MDFILE_AS_MAINPAGE = + +#--------------------------------------------------------------------------- +# configuration options related to source browsing +#--------------------------------------------------------------------------- + +# If the SOURCE_BROWSER tag is set to YES then a list of source files will +# be generated. Documented entities will be cross-referenced with these sources. +# Note: To get rid of all source code in the generated output, make sure also +# VERBATIM_HEADERS is set to NO. + +SOURCE_BROWSER = YES + +# Setting the INLINE_SOURCES tag to YES will include the body +# of functions and classes directly in the documentation. + +INLINE_SOURCES = NO + +# Setting the STRIP_CODE_COMMENTS tag to YES (the default) will instruct +# doxygen to hide any special comment blocks from generated source code +# fragments. Normal C, C++ and Fortran comments will always remain visible. + +STRIP_CODE_COMMENTS = YES + +# If the REFERENCED_BY_RELATION tag is set to YES +# then for each documented function all documented +# functions referencing it will be listed. + +REFERENCED_BY_RELATION = YES + +# If the REFERENCES_RELATION tag is set to YES +# then for each documented function all documented entities +# called/used by that function will be listed. + +REFERENCES_RELATION = YES + +# If the REFERENCES_LINK_SOURCE tag is set to YES (the default) +# and SOURCE_BROWSER tag is set to YES, then the hyperlinks from +# functions in REFERENCES_RELATION and REFERENCED_BY_RELATION lists will +# link to the source code. Otherwise they will link to the documentation. + +REFERENCES_LINK_SOURCE = YES + +# If the USE_HTAGS tag is set to YES then the references to source code +# will point to the HTML generated by the htags(1) tool instead of doxygen +# built-in source browser. The htags tool is part of GNU's global source +# tagging system (see http://www.gnu.org/software/global/global.html). You +# will need version 4.8.6 or higher. + +USE_HTAGS = NO + +# If the VERBATIM_HEADERS tag is set to YES (the default) then Doxygen +# will generate a verbatim copy of the header file for each class for +# which an include is specified. Set to NO to disable this. + +VERBATIM_HEADERS = YES + +#--------------------------------------------------------------------------- +# configuration options related to the alphabetical class index +#--------------------------------------------------------------------------- + +# If the ALPHABETICAL_INDEX tag is set to YES, an alphabetical index +# of all compounds will be generated. Enable this if the project +# contains a lot of classes, structs, unions or interfaces. + +ALPHABETICAL_INDEX = NO + +# If the alphabetical index is enabled (see ALPHABETICAL_INDEX) then +# the COLS_IN_ALPHA_INDEX tag can be used to specify the number of columns +# in which this list will be split (can be a number in the range [1..20]) + +COLS_IN_ALPHA_INDEX = 5 + +# In case all classes in a project start with a common prefix, all +# classes will be put under the same header in the alphabetical index. +# The IGNORE_PREFIX tag can be used to specify one or more prefixes that +# should be ignored while generating the index headers. + +IGNORE_PREFIX = + +#--------------------------------------------------------------------------- +# configuration options related to the HTML output +#--------------------------------------------------------------------------- + +# If the GENERATE_HTML tag is set to YES (the default) Doxygen will +# generate HTML output. + +GENERATE_HTML = YES + +# The HTML_OUTPUT tag is used to specify where the HTML docs will be put. +# If a relative path is entered the value of OUTPUT_DIRECTORY will be +# put in front of it. If left blank `html' will be used as the default path. + +HTML_OUTPUT = html + +# The HTML_FILE_EXTENSION tag can be used to specify the file extension for +# each generated HTML page (for example: .htm,.php,.asp). If it is left blank +# doxygen will generate files with .html extension. + +HTML_FILE_EXTENSION = .html + +# The HTML_HEADER tag can be used to specify a personal HTML header for +# each generated HTML page. If it is left blank doxygen will generate a +# standard header. Note that when using a custom header you are responsible +# for the proper inclusion of any scripts and style sheets that doxygen +# needs, which is dependent on the configuration options used. +# It is advised to generate a default header using "doxygen -w html +# header.html footer.html stylesheet.css YourConfigFile" and then modify +# that header. Note that the header is subject to change so you typically +# have to redo this when upgrading to a newer version of doxygen or when +# changing the value of configuration settings such as GENERATE_TREEVIEW! + +HTML_HEADER = + +# The HTML_FOOTER tag can be used to specify a personal HTML footer for +# each generated HTML page. If it is left blank doxygen will generate a +# standard footer. + +HTML_FOOTER = doc/footer.html + +# The HTML_STYLESHEET tag can be used to specify a user-defined cascading +# style sheet that is used by each HTML page. It can be used to +# fine-tune the look of the HTML output. If left blank doxygen will +# generate a default style sheet. Note that it is recommended to use +# HTML_EXTRA_STYLESHEET instead of this one, as it is more robust and this +# tag will in the future become obsolete. + +HTML_STYLESHEET = doc/stylesheet.css + +# The HTML_EXTRA_STYLESHEET tag can be used to specify an additional +# user-defined cascading style sheet that is included after the standard +# style sheets created by doxygen. Using this option one can overrule +# certain style aspects. This is preferred over using HTML_STYLESHEET +# since it does not replace the standard style sheet and is therefor more +# robust against future updates. Doxygen will copy the style sheet file to +# the output directory. + +HTML_EXTRA_STYLESHEET = + +# The HTML_EXTRA_FILES tag can be used to specify one or more extra images or +# other source files which should be copied to the HTML output directory. Note +# that these files will be copied to the base HTML output directory. Use the +# $relpath$ marker in the HTML_HEADER and/or HTML_FOOTER files to load these +# files. In the HTML_STYLESHEET file, use the file name only. Also note that +# the files will be copied as-is there are no commands or markers available. + +HTML_EXTRA_FILES = + +# The HTML_COLORSTYLE_HUE tag controls the color of the HTML output. +# Doxygen will adjust the colors in the style sheet and background images +# according to this color. Hue is specified as an angle on a colorwheel, +# see http://en.wikipedia.org/wiki/Hue for more information. +# For instance the value 0 represents red, 60 is yellow, 120 is green, +# 180 is cyan, 240 is blue, 300 purple, and 360 is red again. +# The allowed range is 0 to 359. + +HTML_COLORSTYLE_HUE = 220 + +# The HTML_COLORSTYLE_SAT tag controls the purity (or saturation) of +# the colors in the HTML output. For a value of 0 the output will use +# grayscales only. A value of 255 will produce the most vivid colors. + +HTML_COLORSTYLE_SAT = 100 + +# The HTML_COLORSTYLE_GAMMA tag controls the gamma correction applied to +# the luminance component of the colors in the HTML output. Values below +# 100 gradually make the output lighter, whereas values above 100 make +# the output darker. The value divided by 100 is the actual gamma applied, +# so 80 represents a gamma of 0.8, The value 220 represents a gamma of 2.2, +# and 100 does not change the gamma. + +HTML_COLORSTYLE_GAMMA = 80 + +# If the HTML_TIMESTAMP tag is set to YES then the footer of each generated HTML +# page will contain the date and time when the page was generated. Setting +# this to NO can help when comparing the output of multiple runs. + +HTML_TIMESTAMP = YES + +# If the HTML_DYNAMIC_SECTIONS tag is set to YES then the generated HTML +# documentation will contain sections that can be hidden and shown after the +# page has loaded. + +HTML_DYNAMIC_SECTIONS = NO + +# With HTML_INDEX_NUM_ENTRIES one can control the preferred number of +# entries shown in the various tree structured indices initially the user +# can expand and collapse entries dynamically later on. Doxygen will expand +# the tree to such a level that at most the specified number of entries are +# visible (unless a fully collapsed tree already exceeds this amount). +# So setting the number of entries 1 will produce a full collapsed tree by +# default. 0 is a special value representing an infinite number of entries +# and will result in a full expanded tree by default. + +HTML_INDEX_NUM_ENTRIES = 100 + +# If the GENERATE_DOCSET tag is set to YES, additional index files +# will be generated that can be used as input for Apple's Xcode 3 +# integrated development environment, introduced with OSX 10.5 (Leopard). +# To create a documentation set, doxygen will generate a Makefile in the +# HTML output directory. Running make will produce the docset in that +# directory and running "make install" will install the docset in +# ~/Library/Developer/Shared/Documentation/DocSets so that Xcode will find +# it at startup. +# See http://developer.apple.com/tools/creatingdocsetswithdoxygen.html +# for more information. + +GENERATE_DOCSET = NO + +# When GENERATE_DOCSET tag is set to YES, this tag determines the name of the +# feed. A documentation feed provides an umbrella under which multiple +# documentation sets from a single provider (such as a company or product suite) +# can be grouped. + +DOCSET_FEEDNAME = "Doxygen generated docs" + +# When GENERATE_DOCSET tag is set to YES, this tag specifies a string that +# should uniquely identify the documentation set bundle. This should be a +# reverse domain-name style string, e.g. com.mycompany.MyDocSet. Doxygen +# will append .docset to the name. + +DOCSET_BUNDLE_ID = org.doxygen.Project + +# When GENERATE_PUBLISHER_ID tag specifies a string that should uniquely +# identify the documentation publisher. This should be a reverse domain-name +# style string, e.g. com.mycompany.MyDocSet.documentation. + +DOCSET_PUBLISHER_ID = org.doxygen.Publisher + +# The GENERATE_PUBLISHER_NAME tag identifies the documentation publisher. + +DOCSET_PUBLISHER_NAME = Publisher + +# If the GENERATE_HTMLHELP tag is set to YES, additional index files +# will be generated that can be used as input for tools like the +# Microsoft HTML help workshop to generate a compiled HTML help file (.chm) +# of the generated HTML documentation. + +GENERATE_HTMLHELP = YES + +# If the GENERATE_HTMLHELP tag is set to YES, the CHM_FILE tag can +# be used to specify the file name of the resulting .chm file. You +# can add a path in front of the file if the result should not be +# written to the html output directory. + +CHM_FILE = + +# If the GENERATE_HTMLHELP tag is set to YES, the HHC_LOCATION tag can +# be used to specify the location (absolute path including file name) of +# the HTML help compiler (hhc.exe). If non-empty doxygen will try to run +# the HTML help compiler on the generated index.hhp. + +HHC_LOCATION = + +# If the GENERATE_HTMLHELP tag is set to YES, the GENERATE_CHI flag +# controls if a separate .chi index file is generated (YES) or that +# it should be included in the master .chm file (NO). + +GENERATE_CHI = NO + +# If the GENERATE_HTMLHELP tag is set to YES, the CHM_INDEX_ENCODING +# is used to encode HtmlHelp index (hhk), content (hhc) and project file +# content. + +CHM_INDEX_ENCODING = + +# If the GENERATE_HTMLHELP tag is set to YES, the BINARY_TOC flag +# controls whether a binary table of contents is generated (YES) or a +# normal table of contents (NO) in the .chm file. + +BINARY_TOC = NO + +# The TOC_EXPAND flag can be set to YES to add extra items for group members +# to the contents of the HTML help documentation and to the tree view. + +TOC_EXPAND = NO + +# If the GENERATE_QHP tag is set to YES and both QHP_NAMESPACE and +# QHP_VIRTUAL_FOLDER are set, an additional index file will be generated +# that can be used as input for Qt's qhelpgenerator to generate a +# Qt Compressed Help (.qch) of the generated HTML documentation. + +GENERATE_QHP = NO + +# If the QHG_LOCATION tag is specified, the QCH_FILE tag can +# be used to specify the file name of the resulting .qch file. +# The path specified is relative to the HTML output folder. + +QCH_FILE = + +# The QHP_NAMESPACE tag specifies the namespace to use when generating +# Qt Help Project output. For more information please see +# http://doc.trolltech.com/qthelpproject.html#namespace + +QHP_NAMESPACE = org.doxygen.Project + +# The QHP_VIRTUAL_FOLDER tag specifies the namespace to use when generating +# Qt Help Project output. For more information please see +# http://doc.trolltech.com/qthelpproject.html#virtual-folders + +QHP_VIRTUAL_FOLDER = doc + +# If QHP_CUST_FILTER_NAME is set, it specifies the name of a custom filter to +# add. For more information please see +# http://doc.trolltech.com/qthelpproject.html#custom-filters + +QHP_CUST_FILTER_NAME = + +# The QHP_CUST_FILT_ATTRS tag specifies the list of the attributes of the +# custom filter to add. For more information please see +# +# Qt Help Project / Custom Filters. + +QHP_CUST_FILTER_ATTRS = + +# The QHP_SECT_FILTER_ATTRS tag specifies the list of the attributes this +# project's +# filter section matches. +# +# Qt Help Project / Filter Attributes. + +QHP_SECT_FILTER_ATTRS = + +# If the GENERATE_QHP tag is set to YES, the QHG_LOCATION tag can +# be used to specify the location of Qt's qhelpgenerator. +# If non-empty doxygen will try to run qhelpgenerator on the generated +# .qhp file. + +QHG_LOCATION = + +# If the GENERATE_ECLIPSEHELP tag is set to YES, additional index files +# will be generated, which together with the HTML files, form an Eclipse help +# plugin. To install this plugin and make it available under the help contents +# menu in Eclipse, the contents of the directory containing the HTML and XML +# files needs to be copied into the plugins directory of eclipse. The name of +# the directory within the plugins directory should be the same as +# the ECLIPSE_DOC_ID value. After copying Eclipse needs to be restarted before +# the help appears. + +GENERATE_ECLIPSEHELP = NO + +# A unique identifier for the eclipse help plugin. When installing the plugin +# the directory name containing the HTML and XML files should also have +# this name. + +ECLIPSE_DOC_ID = org.doxygen.Project + +# The DISABLE_INDEX tag can be used to turn on/off the condensed index (tabs) +# at top of each HTML page. The value NO (the default) enables the index and +# the value YES disables it. Since the tabs have the same information as the +# navigation tree you can set this option to NO if you already set +# GENERATE_TREEVIEW to YES. + +DISABLE_INDEX = NO + +# The GENERATE_TREEVIEW tag is used to specify whether a tree-like index +# structure should be generated to display hierarchical information. +# If the tag value is set to YES, a side panel will be generated +# containing a tree-like index structure (just like the one that +# is generated for HTML Help). For this to work a browser that supports +# JavaScript, DHTML, CSS and frames is required (i.e. any modern browser). +# Windows users are probably better off using the HTML help feature. +# Since the tree basically has the same information as the tab index you +# could consider to set DISABLE_INDEX to NO when enabling this option. + +GENERATE_TREEVIEW = NO + +# The ENUM_VALUES_PER_LINE tag can be used to set the number of enum values +# (range [0,1..20]) that doxygen will group on one line in the generated HTML +# documentation. Note that a value of 0 will completely suppress the enum +# values from appearing in the overview section. + +ENUM_VALUES_PER_LINE = 4 + +# If the treeview is enabled (see GENERATE_TREEVIEW) then this tag can be +# used to set the initial width (in pixels) of the frame in which the tree +# is shown. + +TREEVIEW_WIDTH = 250 + +# When the EXT_LINKS_IN_WINDOW option is set to YES doxygen will open +# links to external symbols imported via tag files in a separate window. + +EXT_LINKS_IN_WINDOW = NO + +# Use this tag to change the font size of Latex formulas included +# as images in the HTML documentation. The default is 10. Note that +# when you change the font size after a successful doxygen run you need +# to manually remove any form_*.png images from the HTML output directory +# to force them to be regenerated. + +FORMULA_FONTSIZE = 10 + +# Use the FORMULA_TRANPARENT tag to determine whether or not the images +# generated for formulas are transparent PNGs. Transparent PNGs are +# not supported properly for IE 6.0, but are supported on all modern browsers. +# Note that when changing this option you need to delete any form_*.png files +# in the HTML output before the changes have effect. + +FORMULA_TRANSPARENT = YES + +# Enable the USE_MATHJAX option to render LaTeX formulas using MathJax +# (see http://www.mathjax.org) which uses client side Javascript for the +# rendering instead of using prerendered bitmaps. Use this if you do not +# have LaTeX installed or if you want to formulas look prettier in the HTML +# output. When enabled you may also need to install MathJax separately and +# configure the path to it using the MATHJAX_RELPATH option. + +USE_MATHJAX = YES + +# When MathJax is enabled you can set the default output format to be used for +# thA MathJax output. Supported types are HTML-CSS, NativeMML (i.e. MathML) and +# SVG. The default value is HTML-CSS, which is slower, but has the best +# compatibility. + +MATHJAX_FORMAT = HTML-CSS + +# When MathJax is enabled you need to specify the location relative to the +# HTML output directory using the MATHJAX_RELPATH option. The destination +# directory should contain the MathJax.js script. For instance, if the mathjax +# directory is located at the same level as the HTML output directory, then +# MATHJAX_RELPATH should be ../mathjax. The default value points to +# the MathJax Content Delivery Network so you can quickly see the result without +# installing MathJax. However, it is strongly recommended to install a local +# copy of MathJax from http://www.mathjax.org before deployment. + +MATHJAX_RELPATH = http://cdn.mathjax.org/mathjax/latest + +# The MATHJAX_EXTENSIONS tag can be used to specify one or MathJax extension +# names that should be enabled during MathJax rendering. + +MATHJAX_EXTENSIONS = + +# When the SEARCHENGINE tag is enabled doxygen will generate a search box +# for the HTML output. The underlying search engine uses javascript +# and DHTML and should work on any modern browser. Note that when using +# HTML help (GENERATE_HTMLHELP), Qt help (GENERATE_QHP), or docsets +# (GENERATE_DOCSET) there is already a search function so this one should +# typically be disabled. For large projects the javascript based search engine +# can be slow, then enabling SERVER_BASED_SEARCH may provide a better solution. + +SEARCHENGINE = YES + +# When the SERVER_BASED_SEARCH tag is enabled the search engine will be +# implemented using a web server instead of a web client using Javascript. +# There are two flavours of web server based search depending on the +# EXTERNAL_SEARCH setting. When disabled, doxygen will generate a PHP script for +# searching and an index file used by the script. When EXTERNAL_SEARCH is +# enabled the indexing and searching needs to be provided by external tools. +# See the manual for details. + +SERVER_BASED_SEARCH = NO + +# When EXTERNAL_SEARCH is enabled doxygen will no longer generate the PHP +# script for searching. Instead the search results are written to an XML file +# which needs to be processed by an external indexer. Doxygen will invoke an +# external search engine pointed to by the SEARCHENGINE_URL option to obtain +# the search results. Doxygen ships with an example indexer (doxyindexer) and +# search engine (doxysearch.cgi) which are based on the open source search engine +# library Xapian. See the manual for configuration details. + +EXTERNAL_SEARCH = NO + +# The SEARCHENGINE_URL should point to a search engine hosted by a web server +# which will returned the search results when EXTERNAL_SEARCH is enabled. +# Doxygen ships with an example search engine (doxysearch) which is based on +# the open source search engine library Xapian. See the manual for configuration +# details. + +SEARCHENGINE_URL = + +# When SERVER_BASED_SEARCH and EXTERNAL_SEARCH are both enabled the unindexed +# search data is written to a file for indexing by an external tool. With the +# SEARCHDATA_FILE tag the name of this file can be specified. + +SEARCHDATA_FILE = searchdata.xml + +# When SERVER_BASED_SEARCH AND EXTERNAL_SEARCH are both enabled the +# EXTERNAL_SEARCH_ID tag can be used as an identifier for the project. This is +# useful in combination with EXTRA_SEARCH_MAPPINGS to search through multiple +# projects and redirect the results back to the right project. + +EXTERNAL_SEARCH_ID = + +# The EXTRA_SEARCH_MAPPINGS tag can be used to enable searching through doxygen +# projects other than the one defined by this configuration file, but that are +# all added to the same external search index. Each project needs to have a +# unique id set via EXTERNAL_SEARCH_ID. The search mapping then maps the id +# of to a relative location where the documentation can be found. +# The format is: EXTRA_SEARCH_MAPPINGS = id1=loc1 id2=loc2 ... + +EXTRA_SEARCH_MAPPINGS = + +#--------------------------------------------------------------------------- +# configuration options related to the LaTeX output +#--------------------------------------------------------------------------- + +# If the GENERATE_LATEX tag is set to YES (the default) Doxygen will +# generate Latex output. + +GENERATE_LATEX = NO + +# The LATEX_OUTPUT tag is used to specify where the LaTeX docs will be put. +# If a relative path is entered the value of OUTPUT_DIRECTORY will be +# put in front of it. If left blank `latex' will be used as the default path. + +LATEX_OUTPUT = latex + +# The LATEX_CMD_NAME tag can be used to specify the LaTeX command name to be +# invoked. If left blank `latex' will be used as the default command name. +# Note that when enabling USE_PDFLATEX this option is only used for +# generating bitmaps for formulas in the HTML output, but not in the +# Makefile that is written to the output directory. + +LATEX_CMD_NAME = latex + +# The MAKEINDEX_CMD_NAME tag can be used to specify the command name to +# generate index for LaTeX. If left blank `makeindex' will be used as the +# default command name. + +MAKEINDEX_CMD_NAME = makeindex + +# If the COMPACT_LATEX tag is set to YES Doxygen generates more compact +# LaTeX documents. This may be useful for small projects and may help to +# save some trees in general. + +COMPACT_LATEX = YES + +# The PAPER_TYPE tag can be used to set the paper type that is used +# by the printer. Possible values are: a4, letter, legal and +# executive. If left blank a4wide will be used. + +PAPER_TYPE = a4wide + +# The EXTRA_PACKAGES tag can be to specify one or more names of LaTeX +# packages that should be included in the LaTeX output. + +EXTRA_PACKAGES = + +# The LATEX_HEADER tag can be used to specify a personal LaTeX header for +# the generated latex document. The header should contain everything until +# the first chapter. If it is left blank doxygen will generate a +# standard header. Notice: only use this tag if you know what you are doing! + +LATEX_HEADER = + +# The LATEX_FOOTER tag can be used to specify a personal LaTeX footer for +# the generated latex document. The footer should contain everything after +# the last chapter. If it is left blank doxygen will generate a +# standard footer. Notice: only use this tag if you know what you are doing! + +LATEX_FOOTER = + +# If the PDF_HYPERLINKS tag is set to YES, the LaTeX that is generated +# is prepared for conversion to pdf (using ps2pdf). The pdf file will +# contain links (just like the HTML output) instead of page references +# This makes the output suitable for online browsing using a pdf viewer. + +PDF_HYPERLINKS = YES + +# If the USE_PDFLATEX tag is set to YES, pdflatex will be used instead of +# plain latex in the generated Makefile. Set this option to YES to get a +# higher quality PDF documentation. + +USE_PDFLATEX = YES + +# If the LATEX_BATCHMODE tag is set to YES, doxygen will add the \\batchmode. +# command to the generated LaTeX files. This will instruct LaTeX to keep +# running if errors occur, instead of asking the user for help. +# This option is also used when generating formulas in HTML. + +LATEX_BATCHMODE = YES + +# If LATEX_HIDE_INDICES is set to YES then doxygen will not +# include the index chapters (such as File Index, Compound Index, etc.) +# in the output. + +LATEX_HIDE_INDICES = NO + +# If LATEX_SOURCE_CODE is set to YES then doxygen will include +# source code with syntax highlighting in the LaTeX output. +# Note that which sources are shown also depends on other settings +# such as SOURCE_BROWSER. + +LATEX_SOURCE_CODE = NO + +# The LATEX_BIB_STYLE tag can be used to specify the style to use for the +# bibliography, e.g. plainnat, or ieeetr. The default style is "plain". See +# http://en.wikipedia.org/wiki/BibTeX for more info. + +LATEX_BIB_STYLE = plain + +#--------------------------------------------------------------------------- +# configuration options related to the RTF output +#--------------------------------------------------------------------------- + +# If the GENERATE_RTF tag is set to YES Doxygen will generate RTF output +# The RTF output is optimized for Word 97 and may not look very pretty with +# other RTF readers or editors. + +GENERATE_RTF = NO + +# The RTF_OUTPUT tag is used to specify where the RTF docs will be put. +# If a relative path is entered the value of OUTPUT_DIRECTORY will be +# put in front of it. If left blank `rtf' will be used as the default path. + +RTF_OUTPUT = rtf + +# If the COMPACT_RTF tag is set to YES Doxygen generates more compact +# RTF documents. This may be useful for small projects and may help to +# save some trees in general. + +COMPACT_RTF = NO + +# If the RTF_HYPERLINKS tag is set to YES, the RTF that is generated +# will contain hyperlink fields. The RTF file will +# contain links (just like the HTML output) instead of page references. +# This makes the output suitable for online browsing using WORD or other +# programs which support those fields. +# Note: wordpad (write) and others do not support links. + +RTF_HYPERLINKS = NO + +# Load style sheet definitions from file. Syntax is similar to doxygen's +# config file, i.e. a series of assignments. You only have to provide +# replacements, missing definitions are set to their default value. + +RTF_STYLESHEET_FILE = + +# Set optional variables used in the generation of an rtf document. +# Syntax is similar to doxygen's config file. + +RTF_EXTENSIONS_FILE = + +#--------------------------------------------------------------------------- +# configuration options related to the man page output +#--------------------------------------------------------------------------- + +# If the GENERATE_MAN tag is set to YES (the default) Doxygen will +# generate man pages + +GENERATE_MAN = NO + +# The MAN_OUTPUT tag is used to specify where the man pages will be put. +# If a relative path is entered the value of OUTPUT_DIRECTORY will be +# put in front of it. If left blank `man' will be used as the default path. + +MAN_OUTPUT = man + +# The MAN_EXTENSION tag determines the extension that is added to +# the generated man pages (default is the subroutine's section .3) + +MAN_EXTENSION = .3 + +# If the MAN_LINKS tag is set to YES and Doxygen generates man output, +# then it will generate one additional man file for each entity +# documented in the real man page(s). These additional files +# only source the real man page, but without them the man command +# would be unable to find the correct page. The default is NO. + +MAN_LINKS = NO + +#--------------------------------------------------------------------------- +# configuration options related to the XML output +#--------------------------------------------------------------------------- + +# If the GENERATE_XML tag is set to YES Doxygen will +# generate an XML file that captures the structure of +# the code including all documentation. + +GENERATE_XML = NO + +# The XML_OUTPUT tag is used to specify where the XML pages will be put. +# If a relative path is entered the value of OUTPUT_DIRECTORY will be +# put in front of it. If left blank `xml' will be used as the default path. + +XML_OUTPUT = xml + +# The XML_SCHEMA tag can be used to specify an XML schema, +# which can be used by a validating XML parser to check the +# syntax of the XML files. + +XML_SCHEMA = + +# The XML_DTD tag can be used to specify an XML DTD, +# which can be used by a validating XML parser to check the +# syntax of the XML files. + +XML_DTD = + +# If the XML_PROGRAMLISTING tag is set to YES Doxygen will +# dump the program listings (including syntax highlighting +# and cross-referencing information) to the XML output. Note that +# enabling this will significantly increase the size of the XML output. + +XML_PROGRAMLISTING = NO + +#--------------------------------------------------------------------------- +# configuration options for the AutoGen Definitions output +#--------------------------------------------------------------------------- + +# If the GENERATE_AUTOGEN_DEF tag is set to YES Doxygen will +# generate an AutoGen Definitions (see autogen.sf.net) file +# that captures the structure of the code including all +# documentation. Note that this feature is still experimental +# and incomplete at the moment. + +GENERATE_AUTOGEN_DEF = NO + +#--------------------------------------------------------------------------- +# configuration options related to the Perl module output +#--------------------------------------------------------------------------- + +# If the GENERATE_PERLMOD tag is set to YES Doxygen will +# generate a Perl module file that captures the structure of +# the code including all documentation. Note that this +# feature is still experimental and incomplete at the +# moment. + +GENERATE_PERLMOD = NO + +# If the PERLMOD_LATEX tag is set to YES Doxygen will generate +# the necessary Makefile rules, Perl scripts and LaTeX code to be able +# to generate PDF and DVI output from the Perl module output. + +PERLMOD_LATEX = NO + +# If the PERLMOD_PRETTY tag is set to YES the Perl module output will be +# nicely formatted so it can be parsed by a human reader. This is useful +# if you want to understand what is going on. On the other hand, if this +# tag is set to NO the size of the Perl module output will be much smaller +# and Perl will parse it just the same. + +PERLMOD_PRETTY = YES + +# The names of the make variables in the generated doxyrules.make file +# are prefixed with the string contained in PERLMOD_MAKEVAR_PREFIX. +# This is useful so different doxyrules.make files included by the same +# Makefile don't overwrite each other's variables. + +PERLMOD_MAKEVAR_PREFIX = + +#--------------------------------------------------------------------------- +# Configuration options related to the preprocessor +#--------------------------------------------------------------------------- + +# If the ENABLE_PREPROCESSING tag is set to YES (the default) Doxygen will +# evaluate all C-preprocessor directives found in the sources and include +# files. + +ENABLE_PREPROCESSING = YES + +# If the MACRO_EXPANSION tag is set to YES Doxygen will expand all macro +# names in the source code. 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Older versions of IE do not have SVG support. + +INTERACTIVE_SVG = NO + +# The tag DOT_PATH can be used to specify the path where the dot tool can be +# found. If left blank, it is assumed the dot tool can be found in the path. + +DOT_PATH = + +# The DOTFILE_DIRS tag can be used to specify one or more directories that +# contain dot files that are included in the documentation (see the +# \dotfile command). + +DOTFILE_DIRS = + +# The MSCFILE_DIRS tag can be used to specify one or more directories that +# contain msc files that are included in the documentation (see the +# \mscfile command). + +MSCFILE_DIRS = + +# The DOT_GRAPH_MAX_NODES tag can be used to set the maximum number of +# nodes that will be shown in the graph. If the number of nodes in a graph +# becomes larger than this value, doxygen will truncate the graph, which is +# visualized by representing a node as a red box. Note that doxygen if the +# number of direct children of the root node in a graph is already larger than +# DOT_GRAPH_MAX_NODES then the graph will not be shown at all. Also note +# that the size of a graph can be further restricted by MAX_DOT_GRAPH_DEPTH. + +DOT_GRAPH_MAX_NODES = 50 + +# The MAX_DOT_GRAPH_DEPTH tag can be used to set the maximum depth of the +# graphs generated by dot. A depth value of 3 means that only nodes reachable +# from the root by following a path via at most 3 edges will be shown. Nodes +# that lay further from the root node will be omitted. Note that setting this +# option to 1 or 2 may greatly reduce the computation time needed for large +# code bases. Also note that the size of a graph can be further restricted by +# DOT_GRAPH_MAX_NODES. Using a depth of 0 means no depth restriction. + +MAX_DOT_GRAPH_DEPTH = 0 + +# Set the DOT_TRANSPARENT tag to YES to generate images with a transparent +# background. This is disabled by default, because dot on Windows does not +# seem to support this out of the box. Warning: Depending on the platform used, +# enabling this option may lead to badly anti-aliased labels on the edges of +# a graph (i.e. they become hard to read). + +DOT_TRANSPARENT = YES + +# Set the DOT_MULTI_TARGETS tag to YES allow dot to generate multiple output +# files in one run (i.e. multiple -o and -T options on the command line). This +# makes dot run faster, but since only newer versions of dot (>1.8.10) +# support this, this feature is disabled by default. + +DOT_MULTI_TARGETS = NO + +# If the GENERATE_LEGEND tag is set to YES (the default) Doxygen will +# generate a legend page explaining the meaning of the various boxes and +# arrows in the dot generated graphs. + +GENERATE_LEGEND = YES + +# If the DOT_CLEANUP tag is set to YES (the default) Doxygen will +# remove the intermediate dot files that are used to generate +# the various graphs. + +DOT_CLEANUP = YES diff --git a/src/plugins/ellipsoidal_shell/sasfit_ff_ellipsoidal_shell_2.c b/src/plugins/ellipsoidal_shell/sasfit_ff_ellipsoidal_shell_2.c index 733e32b3..1566e3c1 100644 --- a/src/plugins/ellipsoidal_shell/sasfit_ff_ellipsoidal_shell_2.c +++ b/src/plugins/ellipsoidal_shell/sasfit_ff_ellipsoidal_shell_2.c @@ -9,7 +9,7 @@ // define shortcuts for local parameters/variables #define R_PRINCIPLE param->p[0]*NU #define R_EQUATORIAL param->p[1]*NU -#define T param->p[3]*NU +#define T param->p[3] #define RP param->p[0] #define RE param->p[1] #define TT param->p[3] diff --git a/src/plugins/triax_ellip_shell/CMakeLists.txt b/src/plugins/triax_ellip_shell/CMakeLists.txt index b9a5efb4..da7ae483 100644 --- a/src/plugins/triax_ellip_shell/CMakeLists.txt +++ b/src/plugins/triax_ellip_shell/CMakeLists.txt @@ -12,6 +12,7 @@ set(LIBS_EXT set(SOURCE_${PRJ_NAME} sasfit_ff_triax_ellip_shell_utils.c sasfit_ff_triax_ellip_shell.c + sasfit_ff_triax_ellip_shell_t.c sasfit_ff_triax_ellip_shell_1.c sasfit_ff_triax_ellip_shell_1t.c sasfit_ff_triax_ellip_shell_2.c diff --git a/src/plugins/triax_ellip_shell/include/sasfit_triax_ellip_shell.h b/src/plugins/triax_ellip_shell/include/sasfit_triax_ellip_shell.h index c8146f34..46a2e3d1 100644 --- a/src/plugins/triax_ellip_shell/include/sasfit_triax_ellip_shell.h +++ b/src/plugins/triax_ellip_shell/include/sasfit_triax_ellip_shell.h @@ -61,8 +61,8 @@ * \b t * shell thickness * - * \b sigma - * width of LogNorm size distribution + * \b dummy + * * * \b eta_c * core scattering length density @@ -394,6 +394,67 @@ sasfit_triax_ellip_shell_DLLEXP scalar sasfit_ff_triax_ellip_shell_1_f(scalar q, sasfit_triax_ellip_shell_DLLEXP scalar sasfit_ff_triax_ellip_shell_1_v(scalar q, sasfit_param * p, int dist); /* ################ stop ff_triax_ellip_shell_1 ################ */ +/* ################ start ff_triax_ellip_shell_t ################ */ +/** + * \defgroup ff_triax_ellip_shell_t triax ellip shell t + * \ingroup ff_plugins_triax_ellshells + * + * \brief \ + * + * + * + * \note Default (Size) Distribution: \ref delta + * + * \par Required parameters: + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + * + *
\b asemi-axis
\b bsemi-axis
\b csemi-axis
\b tshell thickness
\b sigmawidth of LogNorm size distribution
\b eta_ccore scattering length density
\b eta_shshell scattering length density
\b eta_solsolvent scattering length density
+ */ + +/** + * \ingroup ff_triax_ellip_shell_t + * + * \sa sasfit_triax_ellip_shell.h, ff_plugins_triax_ellshells + */ +sasfit_triax_ellip_shell_DLLEXP scalar sasfit_ff_triax_ellip_shell_t(scalar q, sasfit_param * p); + +/** + * \ingroup ff_triax_ellip_shell_t + * + * \sa sasfit_triax_ellip_shell.h, ff_plugins_triax_ellshells + */ +sasfit_triax_ellip_shell_DLLEXP scalar sasfit_ff_triax_ellip_shell_t_f(scalar q, sasfit_param * p); + +/** + * \ingroup ff_triax_ellip_shell_t + * + * \sa sasfit_triax_ellip_shell.h, ff_plugins_triax_ellshells + */ +sasfit_triax_ellip_shell_DLLEXP scalar sasfit_ff_triax_ellip_shell_t_v(scalar q, sasfit_param * p, int dist); +/* ################ stop ff_triax_ellip_shell_t ################ */ + /* ################ start ff_triax_ellip_shell_1t ################ */ /** * \defgroup ff_triax_ellip_shell_1t triax ellip shell 1t diff --git a/src/plugins/triax_ellip_shell/interface.c b/src/plugins/triax_ellip_shell/interface.c index 1a771984..765e6a10 100644 --- a/src/plugins/triax_ellip_shell/interface.c +++ b/src/plugins/triax_ellip_shell/interface.c @@ -7,8 +7,9 @@ #include "include/private.h" // functions to mark for export -SASFIT_PLUGIN_EXP_BEGIN(10) +SASFIT_PLUGIN_EXP_BEGIN(11) SASFIT_PLUGIN_EXP_ADD( ff_triax_ellip_shell ) +SASFIT_PLUGIN_EXP_ADD( ff_triax_ellip_shell_t ) SASFIT_PLUGIN_EXP_ADD( ff_triax_ellip_shell_1 ) SASFIT_PLUGIN_EXP_ADD( ff_triax_ellip_shell_1t ) SASFIT_PLUGIN_EXP_ADD( ff_triax_ellip_shell_2 ) diff --git a/src/plugins/triax_ellip_shell/sasfit_ff_triax_ellip_shell_t.c b/src/plugins/triax_ellip_shell/sasfit_ff_triax_ellip_shell_t.c new file mode 100644 index 00000000..d927f754 --- /dev/null +++ b/src/plugins/triax_ellip_shell/sasfit_ff_triax_ellip_shell_t.c @@ -0,0 +1,324 @@ +/* + * src/plugins/triax_ellip_shell/sasfit_ff_triax_ellip_shell.c + * + * Copyright (c) 2008-2009, Paul Scherrer Institute (PSI) + * + * This file is part of SASfit. + * + * SASfit is free software: you can redistribute it and/or modify + * it under the terms of the GNU General Public License as published by + * the Free Software Foundation, either version 3 of the License, or + * (at your option) any later version. + * + * SASfit is distributed in the hope that it will be useful, + * but WITHOUT ANY WARRANTY; without even the implied warranty of + * MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the + * GNU General Public License for more details. + * + * You should have received a copy of the GNU General Public License + * along with SASfit. If not, see . + */ + +/* + * Author(s) of this file: + * Joachim Kohlbrecher (joachim.kohlbrecher@psi.ch) + * Ingo Bressler (ingo@cs.tu-berlin.de) + */ + +#include "include/private.h" +#include + +// define shortcuts for local parameters/variables +#define A param->p[0] +#define B param->p[1] +#define C param->p[2] +#define T param->p[3]*NU +#define AA param->p[0] +#define BB param->p[1] +#define CC param->p[2] +#define TT param->p[3] + +scalar sasfit_ff_triax_ellip_shell_t_core(sasfit_param * param) +{ + scalar u_c, u_sh; + scalar f_c, f_sh; + + SASFIT_ASSERT_PTR(param); + + if (fabs(A*B*C) + fabs(T) == 0.0) return 0.0; + + u_c = Q*sqrt(( pow(A*cos(X*M_PI/2.),2.) + pow(B*sin(X*M_PI/2.),2.) )*(1.-Y*Y) + pow(C*Y,2.)); + u_sh = Q*sqrt(( pow((A+T)*cos(X*M_PI/2.),2.) + pow((B+T)*sin(X*M_PI/2.),2.) ) * (1.-Y*Y) + pow((C+T)*Y,2.)); + + f_c = 4./3.*M_PI*A*B*C*(ETA_C-ETA_SH); + if (u_c != 0.0) + { + f_c = f_c * 3*(sin(u_c) -u_c *cos(u_c) )/pow(u_c ,3); + } + + f_sh = 4./3.*M_PI*(A+T)*(B+T)*(C+T)*(ETA_SH-ETA_SOL); + if (u_sh != 0.0) + { + f_sh = f_sh * 3*(sin(u_sh)-u_sh*cos(u_sh))/pow(u_sh,3); + } + + return LNDISTR*gsl_sf_pow_int(f_sh+f_c, lround(P)); +} + + +scalar sasfit_ff_triax_ellip_shell_t_core_NU(scalar x, sasfit_param * param) +{ + sasfit_param subParam; + sasfit_init_param( &subParam ); + if (SIGMA==0) { + LNDISTR = 1; + NU = 1; + } else { + subParam.p[0] = 1.0; + subParam.p[1] = SIGMA; + subParam.p[2] = 1.0; + subParam.p[3] = 1.0; + LNDISTR = sasfit_sd_LogNorm(x, &subParam); + NU=x; + SASFIT_CHECK_SUB_ERR(param, subParam); + if ( subParam.errStatus != FALSE ) { + sasfit_out("LogNormError: SIGMA:%lf\n",SIGMA); + return 1; + } + } + return sasfit_ff_triax_ellip_shell_t_core(param); +} +scalar sasfit_ff_triax_ellip_shell_t_core_y(scalar y, sasfit_param * param) +{ + scalar res; + + SASFIT_ASSERT_PTR(param); + + Y = y; + if (SIGMA == 0) { + NU = 1; + LNDISTR = 1; + res = sasfit_ff_triax_ellip_shell_t_core(param); + } else { + res = sasfit_integrate(NUMIN, NUMAX, sasfit_ff_triax_ellip_shell_t_core_NU, param); + } + + return res; +} + +scalar sasfit_ff_triax_ellip_shell_t_core_x(scalar x, sasfit_param * param) +{ + scalar res; + + SASFIT_ASSERT_PTR(param); + + X = x; + + res = sasfit_integrate(0.0, 1.0, sasfit_ff_triax_ellip_shell_t_core_y, param); + + return res; +} + +scalar sasfit_ff_triax_ellip_shell_t(scalar q, sasfit_param * param) +{ + scalar *aw, res,err,sum; + scalar cubxmin[3], cubxmax[3], fval[1], ferr[1]; + size_t neval; + int intstrategy, ndim, lenaw=4000; + cubature_param cparam; + + SASFIT_ASSERT_PTR(param); // assert pointer param is valid + + NU = 1; + LNDISTR=1.0; + + SASFIT_CHECK_COND1((q < 0.0), param, "q(%lg) < 0",q); + SASFIT_CHECK_COND1((A < 0.0), param, "a(%lg) < 0",A); + SASFIT_CHECK_COND1((B < 0.0), param, "b(%lg) < 0",B); + SASFIT_CHECK_COND1((C < 0.0), param, "c(%lg) < 0",C); + SASFIT_CHECK_COND1((T < 0.0), param, "t(%lg) < 0",T); + SASFIT_CHECK_COND1((SIGMA < 0.0), param, "SIGMA(%lg) < 0",SIGMA); + + Q = q; // Q + P = 2.0; // pow + if (SIGMA==0) { + ndim=2; + NUMIN = 1; + NUMAX = 1; + } else { + ndim =3; + find_LogNorm_int_range(6,1,SIGMA,&NUMIN, &NUMAX, param); + } + cubxmin[0]=0; + cubxmax[0]=1; + cubxmin[1]=0; + cubxmax[1]=1; + cubxmin[2]=NUMIN; + cubxmax[2]=NUMAX; + cparam.param = param; + cparam.cubxmin=cubxmin; + cparam.cubxmax=cubxmax; + cparam.ndim=ndim; + cparam.func = &sasfit_ff_triax_ellip_shell_t_core; + + intstrategy = sasfit_get_int_strategy(); + intstrategy=P_CUBATURE; + switch(intstrategy) { + case OOURA_DOUBLE_EXP_QUADRATURE: { + aw = (scalar *)malloc((lenaw)*sizeof(scalar)); + sasfit_intdeini(lenaw, GSL_DBL_MIN, sasfit_eps_get_nriq(), aw); + sasfit_intde(&Kernel_P_OOURA1, 0,1, aw, &res, &err, param); + sum=res; + free(aw); + break; + } + case OOURA_CLENSHAW_CURTIS_QUADRATURE: { + aw = (scalar *)malloc((lenaw+1)*sizeof(scalar)); + sasfit_intccini(lenaw, aw); + sasfit_intcc(&Kernel_P_OOURA1, 0,1, sasfit_eps_get_nriq(), lenaw, aw, &res, &err,param); + sum=res; + free(aw); + break; + } + case H_CUBATURE: { + hcubature(1, &triax_ellip_shell_cubature,&cparam,ndim, cubxmin, cubxmax, + 100000, 0.0, sasfit_eps_get_nriq(), ERROR_PAIRED, + fval, ferr); + sum = fval[0]; + break; + } + case P_CUBATURE: { + pcubature(1, &triax_ellip_shell_cubature,&cparam,ndim, cubxmin, cubxmax, + 100000, 0.0, sasfit_eps_get_nriq(), ERROR_PAIRED, + fval, ferr); + sum = fval[0]; + break; + } + default: { +// sasfit_out("ise default sasfit_integrate routine\n"); + sum=sasfit_integrate(0.0, 1.0, sasfit_ff_triax_ellip_shell_t_core_x, param); + break; + } + } + return sum; +} + +scalar sasfit_ff_triax_ellip_shell_t_f(scalar q, sasfit_param * param) +{ + scalar *aw, res,err,sum; + scalar cubxmin[3], cubxmax[3], fval[1], ferr[1]; + size_t neval; + int intstrategy, ndim, lenaw=4000; + cubature_param cparam; + + SASFIT_ASSERT_PTR(param); // assert pointer param is valid + + NU = 1; + LNDISTR=1.0; + + SASFIT_CHECK_COND1((q < 0.0), param, "q(%lg) < 0",q); + SASFIT_CHECK_COND1((A < 0.0), param, "a(%lg) < 0",A); + SASFIT_CHECK_COND1((B < 0.0), param, "b(%lg) < 0",B); + SASFIT_CHECK_COND1((C < 0.0), param, "c(%lg) < 0",C); + SASFIT_CHECK_COND1((T < 0.0), param, "t(%lg) < 0",T); + SASFIT_CHECK_COND1((SIGMA < 0.0), param, "SIGMA(%lg) < 0",SIGMA); + + Q = q; // Q + P = 1.0; // pow + if (SIGMA==0) { + ndim=2; + NUMIN = 1; + NUMAX = 1; + } else { + ndim =3; + find_LogNorm_int_range(6,1,SIGMA,&NUMIN, &NUMAX, param); + } + cubxmin[0]=0; + cubxmax[0]=1; + cubxmin[1]=0; + cubxmax[1]=1; + cubxmin[2]=NUMIN; + cubxmax[2]=NUMAX; + cparam.param = param; + cparam.cubxmin=cubxmin; + cparam.cubxmax=cubxmax; + cparam.ndim=ndim; + cparam.func = &sasfit_ff_triax_ellip_shell_t_core; + + intstrategy = sasfit_get_int_strategy(); + intstrategy=P_CUBATURE; + switch(intstrategy) { + case OOURA_DOUBLE_EXP_QUADRATURE: { + aw = (scalar *)malloc((lenaw)*sizeof(scalar)); + sasfit_intdeini(lenaw, GSL_DBL_MIN, sasfit_eps_get_nriq(), aw); + sasfit_intde(&Kernel_P_OOURA1, 0,1, aw, &res, &err, param); + sum=res; + free(aw); + break; + } + case OOURA_CLENSHAW_CURTIS_QUADRATURE: { + aw = (scalar *)malloc((lenaw+1)*sizeof(scalar)); + sasfit_intccini(lenaw, aw); + sasfit_intcc(&Kernel_P_OOURA1, 0,1, sasfit_eps_get_nriq(), lenaw, aw, &res, &err,param); + sum=res; + free(aw); + break; + } + case H_CUBATURE: { + hcubature(1, &triax_ellip_shell_cubature,&cparam,ndim, cubxmin, cubxmax, + 100000, 0.0, sasfit_eps_get_nriq(), ERROR_PAIRED, + fval, ferr); + sum = fval[0]; + break; + } + case P_CUBATURE: { + pcubature(1, &triax_ellip_shell_cubature,&cparam,ndim, cubxmin, cubxmax, + 100000, 0.0, sasfit_eps_get_nriq(), ERROR_PAIRED, + fval, ferr); + sum = fval[0]; + break; + } + default: { +// sasfit_out("ise default sasfit_integrate routine\n"); + sum=sasfit_integrate(0.0, 1.0, sasfit_ff_triax_ellip_shell_t_core_x, param); + break; + } + } + return sum; +} + +scalar sasfit_ff_triax_ellip_shell_t_v(scalar x, sasfit_param * param, int dist) +{ + scalar V,nu1,nu2,nu3,TT3,TT2; + SASFIT_ASSERT_PTR(param); + nu1=exp(0.5*SIGMA*SIGMA*1*1); + nu2=exp(0.5*SIGMA*SIGMA*2*2); + nu3=exp(0.5*SIGMA*SIGMA*3*3); + TT3= gsl_pow_3(TT); + TT2=gsl_pow_2(TT); + + V = (A*TT2+A*C*T+A*B*T+A*B*C)*nu1+TT3+C*TT2+B*TT2+B*C*T; + V=V*4./3.*M_PI; + return V; + + switch ( dist ) + { + case 0: + V = (x + T) * (B + T) * (C + T); + break; + case 1: + V = (A + T) * (x + T) * (C + T); + break; + case 2: + V = (A + T) * (B + T) * (x + T); + break; + case 3: + V = (A + x) * (B + x) * (C + x); + break; + default: + V = (A + T) * (B + T) * (C + T); + break; + } + return 4.0/3.0 * M_PI * x; +} +