forked from sPHENIX-Collaboration/coresoftware
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pyhistfu.f
executable file
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pyhistfu.f
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C*********************************************************************
SUBROUTINE PYHISTFU(KF,X,Q2,XPQ,JBT)
C *******JBT specifies beam or target of the particle
C...Gives proton and pi+ parton structure functions according to a few
C...different parametrizations. Note that what is coded is x times the
C...probability distribution, i.e. xq(x,Q2) etc.
COMMON/HIPARNT/HIPR1(100),IHPR2(50),HINT1(100),IHNT2(50)
SAVE /HIPARNT/
COMMON/HIJCRDN/YP(3,300),YT(3,300)
SAVE /HIJCRDN/
C ********COMMON BLOCK FROM HIJING
COMMON/LUDAT1/MSTU(200),PARU(200),MSTJ(200),PARJ(200)
SAVE /LUDAT1/
COMMON/LUDAT2/KCHG(500,3),PMAS(500,4),PARF(2000),VCKM(4,4)
SAVE /LUDAT2/
COMMON/PYHIPARS/MSTP(200),PARP(200),MSTI(200),PARI(200)
SAVE /PYHIPARS/
COMMON/PYHIINT1/MINT(400),VINT(400)
SAVE /PYHIINT1/
DIMENSION XPQ(-6:6),XQ(6),TX(6),TT(6),TS(6),NEHLQ(8,2),
&CEHLQ(6,6,2,8,2),CDO(3,6,5,2),COW(3,5,4,2)
SAVE XQ, TX, TT, TS, NEHLQ, CEHLQ, CDO, COW ! Uzhi
C...The following data lines are coefficients needed in the
C...Eichten, Hinchliffe, Lane, Quigg proton structure function
C...parametrizations, see below.
C...Powers of 1-x in different cases.
DATA NEHLQ/3,4,7,5,7,7,7,7,3,4,7,6,7,7,7,7/
C...Expansion coefficients for up valence quark distribution.
DATA (((CEHLQ(IX,IT,NX,1,1),IX=1,6),IT=1,6),NX=1,2)/
1 7.677E-01,-2.087E-01,-3.303E-01,-2.517E-02,-1.570E-02,-1.000E-04,
2-5.326E-01,-2.661E-01, 3.201E-01, 1.192E-01, 2.434E-02, 7.620E-03,
3 2.162E-01, 1.881E-01,-8.375E-02,-6.515E-02,-1.743E-02,-5.040E-03,
4-9.211E-02,-9.952E-02, 1.373E-02, 2.506E-02, 8.770E-03, 2.550E-03,
5 3.670E-02, 4.409E-02, 9.600E-04,-7.960E-03,-3.420E-03,-1.050E-03,
6-1.549E-02,-2.026E-02,-3.060E-03, 2.220E-03, 1.240E-03, 4.100E-04,
1 2.395E-01, 2.905E-01, 9.778E-02, 2.149E-02, 3.440E-03, 5.000E-04,
2 1.751E-02,-6.090E-03,-2.687E-02,-1.916E-02,-7.970E-03,-2.750E-03,
3-5.760E-03,-5.040E-03, 1.080E-03, 2.490E-03, 1.530E-03, 7.500E-04,
4 1.740E-03, 1.960E-03, 3.000E-04,-3.400E-04,-2.900E-04,-1.800E-04,
5-5.300E-04,-6.400E-04,-1.700E-04, 4.000E-05, 6.000E-05, 4.000E-05,
6 1.700E-04, 2.200E-04, 8.000E-05, 1.000E-05,-1.000E-05,-1.000E-05/
DATA (((CEHLQ(IX,IT,NX,1,2),IX=1,6),IT=1,6),NX=1,2)/
1 7.237E-01,-2.189E-01,-2.995E-01,-1.909E-02,-1.477E-02, 2.500E-04,
2-5.314E-01,-2.425E-01, 3.283E-01, 1.119E-01, 2.223E-02, 7.070E-03,
3 2.289E-01, 1.890E-01,-9.859E-02,-6.900E-02,-1.747E-02,-5.080E-03,
4-1.041E-01,-1.084E-01, 2.108E-02, 2.975E-02, 9.830E-03, 2.830E-03,
5 4.394E-02, 5.116E-02,-1.410E-03,-1.055E-02,-4.230E-03,-1.270E-03,
6-1.991E-02,-2.539E-02,-2.780E-03, 3.430E-03, 1.720E-03, 5.500E-04,
1 2.410E-01, 2.884E-01, 9.369E-02, 1.900E-02, 2.530E-03, 2.400E-04,
2 1.765E-02,-9.220E-03,-3.037E-02,-2.085E-02,-8.440E-03,-2.810E-03,
3-6.450E-03,-5.260E-03, 1.720E-03, 3.110E-03, 1.830E-03, 8.700E-04,
4 2.120E-03, 2.320E-03, 2.600E-04,-4.900E-04,-3.900E-04,-2.300E-04,
5-6.900E-04,-8.200E-04,-2.000E-04, 7.000E-05, 9.000E-05, 6.000E-05,
6 2.400E-04, 3.100E-04, 1.100E-04, 0.000E+00,-2.000E-05,-2.000E-05/
C...Expansion coefficients for down valence quark distribution.
DATA (((CEHLQ(IX,IT,NX,2,1),IX=1,6),IT=1,6),NX=1,2)/
1 3.813E-01,-8.090E-02,-1.634E-01,-2.185E-02,-8.430E-03,-6.200E-04,
2-2.948E-01,-1.435E-01, 1.665E-01, 6.638E-02, 1.473E-02, 4.080E-03,
3 1.252E-01, 1.042E-01,-4.722E-02,-3.683E-02,-1.038E-02,-2.860E-03,
4-5.478E-02,-5.678E-02, 8.900E-03, 1.484E-02, 5.340E-03, 1.520E-03,
5 2.220E-02, 2.567E-02,-3.000E-05,-4.970E-03,-2.160E-03,-6.500E-04,
6-9.530E-03,-1.204E-02,-1.510E-03, 1.510E-03, 8.300E-04, 2.700E-04,
1 1.261E-01, 1.354E-01, 3.958E-02, 8.240E-03, 1.660E-03, 4.500E-04,
2 3.890E-03,-1.159E-02,-1.625E-02,-9.610E-03,-3.710E-03,-1.260E-03,
3-1.910E-03,-5.600E-04, 1.590E-03, 1.590E-03, 8.400E-04, 3.900E-04,
4 6.400E-04, 4.900E-04,-1.500E-04,-2.900E-04,-1.800E-04,-1.000E-04,
5-2.000E-04,-1.900E-04, 0.000E+00, 6.000E-05, 4.000E-05, 3.000E-05,
6 7.000E-05, 8.000E-05, 2.000E-05,-1.000E-05,-1.000E-05,-1.000E-05/
DATA (((CEHLQ(IX,IT,NX,2,2),IX=1,6),IT=1,6),NX=1,2)/
1 3.578E-01,-8.622E-02,-1.480E-01,-1.840E-02,-7.820E-03,-4.500E-04,
2-2.925E-01,-1.304E-01, 1.696E-01, 6.243E-02, 1.353E-02, 3.750E-03,
3 1.318E-01, 1.041E-01,-5.486E-02,-3.872E-02,-1.038E-02,-2.850E-03,
4-6.162E-02,-6.143E-02, 1.303E-02, 1.740E-02, 5.940E-03, 1.670E-03,
5 2.643E-02, 2.957E-02,-1.490E-03,-6.450E-03,-2.630E-03,-7.700E-04,
6-1.218E-02,-1.497E-02,-1.260E-03, 2.240E-03, 1.120E-03, 3.500E-04,
1 1.263E-01, 1.334E-01, 3.732E-02, 7.070E-03, 1.260E-03, 3.400E-04,
2 3.660E-03,-1.357E-02,-1.795E-02,-1.031E-02,-3.880E-03,-1.280E-03,
3-2.100E-03,-3.600E-04, 2.050E-03, 1.920E-03, 9.800E-04, 4.400E-04,
4 7.700E-04, 5.400E-04,-2.400E-04,-3.900E-04,-2.400E-04,-1.300E-04,
5-2.600E-04,-2.300E-04, 2.000E-05, 9.000E-05, 6.000E-05, 4.000E-05,
6 9.000E-05, 1.000E-04, 2.000E-05,-2.000E-05,-2.000E-05,-1.000E-05/
C...Expansion coefficients for up and down sea quark distributions.
DATA (((CEHLQ(IX,IT,NX,3,1),IX=1,6),IT=1,6),NX=1,2)/
1 6.870E-02,-6.861E-02, 2.973E-02,-5.400E-03, 3.780E-03,-9.700E-04,
2-1.802E-02, 1.400E-04, 6.490E-03,-8.540E-03, 1.220E-03,-1.750E-03,
3-4.650E-03, 1.480E-03,-5.930E-03, 6.000E-04,-1.030E-03,-8.000E-05,
4 6.440E-03, 2.570E-03, 2.830E-03, 1.150E-03, 7.100E-04, 3.300E-04,
5-3.930E-03,-2.540E-03,-1.160E-03,-7.700E-04,-3.600E-04,-1.900E-04,
6 2.340E-03, 1.930E-03, 5.300E-04, 3.700E-04, 1.600E-04, 9.000E-05,
1 1.014E+00,-1.106E+00, 3.374E-01,-7.444E-02, 8.850E-03,-8.700E-04,
2 9.233E-01,-1.285E+00, 4.475E-01,-9.786E-02, 1.419E-02,-1.120E-03,
3 4.888E-02,-1.271E-01, 8.606E-02,-2.608E-02, 4.780E-03,-6.000E-04,
4-2.691E-02, 4.887E-02,-1.771E-02, 1.620E-03, 2.500E-04,-6.000E-05,
5 7.040E-03,-1.113E-02, 1.590E-03, 7.000E-04,-2.000E-04, 0.000E+00,
6-1.710E-03, 2.290E-03, 3.800E-04,-3.500E-04, 4.000E-05, 1.000E-05/
DATA (((CEHLQ(IX,IT,NX,3,2),IX=1,6),IT=1,6),NX=1,2)/
1 1.008E-01,-7.100E-02, 1.973E-02,-5.710E-03, 2.930E-03,-9.900E-04,
2-5.271E-02,-1.823E-02, 1.792E-02,-6.580E-03, 1.750E-03,-1.550E-03,
3 1.220E-02, 1.763E-02,-8.690E-03,-8.800E-04,-1.160E-03,-2.100E-04,
4-1.190E-03,-7.180E-03, 2.360E-03, 1.890E-03, 7.700E-04, 4.100E-04,
5-9.100E-04, 2.040E-03,-3.100E-04,-1.050E-03,-4.000E-04,-2.400E-04,
6 1.190E-03,-1.700E-04,-2.000E-04, 4.200E-04, 1.700E-04, 1.000E-04,
1 1.081E+00,-1.189E+00, 3.868E-01,-8.617E-02, 1.115E-02,-1.180E-03,
2 9.917E-01,-1.396E+00, 4.998E-01,-1.159E-01, 1.674E-02,-1.720E-03,
3 5.099E-02,-1.338E-01, 9.173E-02,-2.885E-02, 5.890E-03,-6.500E-04,
4-3.178E-02, 5.703E-02,-2.070E-02, 2.440E-03, 1.100E-04,-9.000E-05,
5 8.970E-03,-1.392E-02, 2.050E-03, 6.500E-04,-2.300E-04, 2.000E-05,
6-2.340E-03, 3.010E-03, 5.000E-04,-3.900E-04, 6.000E-05, 1.000E-05/
C...Expansion coefficients for gluon distribution.
DATA (((CEHLQ(IX,IT,NX,4,1),IX=1,6),IT=1,6),NX=1,2)/
1 9.482E-01,-9.578E-01, 1.009E-01,-1.051E-01, 3.456E-02,-3.054E-02,
2-9.627E-01, 5.379E-01, 3.368E-01,-9.525E-02, 1.488E-02,-2.051E-02,
3 4.300E-01,-8.306E-02,-3.372E-01, 4.902E-02,-9.160E-03, 1.041E-02,
4-1.925E-01,-1.790E-02, 2.183E-01, 7.490E-03, 4.140E-03,-1.860E-03,
5 8.183E-02, 1.926E-02,-1.072E-01,-1.944E-02,-2.770E-03,-5.200E-04,
6-3.884E-02,-1.234E-02, 5.410E-02, 1.879E-02, 3.350E-03, 1.040E-03,
1 2.948E+01,-3.902E+01, 1.464E+01,-3.335E+00, 5.054E-01,-5.915E-02,
2 2.559E+01,-3.955E+01, 1.661E+01,-4.299E+00, 6.904E-01,-8.243E-02,
3-1.663E+00, 1.176E+00, 1.118E+00,-7.099E-01, 1.948E-01,-2.404E-02,
4-2.168E-01, 8.170E-01,-7.169E-01, 1.851E-01,-1.924E-02,-3.250E-03,
5 2.088E-01,-4.355E-01, 2.239E-01,-2.446E-02,-3.620E-03, 1.910E-03,
6-9.097E-02, 1.601E-01,-5.681E-02,-2.500E-03, 2.580E-03,-4.700E-04/
DATA (((CEHLQ(IX,IT,NX,4,2),IX=1,6),IT=1,6),NX=1,2)/
1 2.367E+00, 4.453E-01, 3.660E-01, 9.467E-02, 1.341E-01, 1.661E-02,
2-3.170E+00,-1.795E+00, 3.313E-02,-2.874E-01,-9.827E-02,-7.119E-02,
3 1.823E+00, 1.457E+00,-2.465E-01, 3.739E-02, 6.090E-03, 1.814E-02,
4-1.033E+00,-9.827E-01, 2.136E-01, 1.169E-01, 5.001E-02, 1.684E-02,
5 5.133E-01, 5.259E-01,-1.173E-01,-1.139E-01,-4.988E-02,-2.021E-02,
6-2.881E-01,-3.145E-01, 5.667E-02, 9.161E-02, 4.568E-02, 1.951E-02,
1 3.036E+01,-4.062E+01, 1.578E+01,-3.699E+00, 6.020E-01,-7.031E-02,
2 2.700E+01,-4.167E+01, 1.770E+01,-4.804E+00, 7.862E-01,-1.060E-01,
3-1.909E+00, 1.357E+00, 1.127E+00,-7.181E-01, 2.232E-01,-2.481E-02,
4-2.488E-01, 9.781E-01,-8.127E-01, 2.094E-01,-2.997E-02,-4.710E-03,
5 2.506E-01,-5.427E-01, 2.672E-01,-3.103E-02,-1.800E-03, 2.870E-03,
6-1.128E-01, 2.087E-01,-6.972E-02,-2.480E-03, 2.630E-03,-8.400E-04/
C...Expansion coefficients for strange sea quark distribution.
DATA (((CEHLQ(IX,IT,NX,5,1),IX=1,6),IT=1,6),NX=1,2)/
1 4.968E-02,-4.173E-02, 2.102E-02,-3.270E-03, 3.240E-03,-6.700E-04,
2-6.150E-03,-1.294E-02, 6.740E-03,-6.890E-03, 9.000E-04,-1.510E-03,
3-8.580E-03, 5.050E-03,-4.900E-03,-1.600E-04,-9.400E-04,-1.500E-04,
4 7.840E-03, 1.510E-03, 2.220E-03, 1.400E-03, 7.000E-04, 3.500E-04,
5-4.410E-03,-2.220E-03,-8.900E-04,-8.500E-04,-3.600E-04,-2.000E-04,
6 2.520E-03, 1.840E-03, 4.100E-04, 3.900E-04, 1.600E-04, 9.000E-05,
1 9.235E-01,-1.085E+00, 3.464E-01,-7.210E-02, 9.140E-03,-9.100E-04,
2 9.315E-01,-1.274E+00, 4.512E-01,-9.775E-02, 1.380E-02,-1.310E-03,
3 4.739E-02,-1.296E-01, 8.482E-02,-2.642E-02, 4.760E-03,-5.700E-04,
4-2.653E-02, 4.953E-02,-1.735E-02, 1.750E-03, 2.800E-04,-6.000E-05,
5 6.940E-03,-1.132E-02, 1.480E-03, 6.500E-04,-2.100E-04, 0.000E+00,
6-1.680E-03, 2.340E-03, 4.200E-04,-3.400E-04, 5.000E-05, 1.000E-05/
DATA (((CEHLQ(IX,IT,NX,5,2),IX=1,6),IT=1,6),NX=1,2)/
1 6.478E-02,-4.537E-02, 1.643E-02,-3.490E-03, 2.710E-03,-6.700E-04,
2-2.223E-02,-2.126E-02, 1.247E-02,-6.290E-03, 1.120E-03,-1.440E-03,
3-1.340E-03, 1.362E-02,-6.130E-03,-7.900E-04,-9.000E-04,-2.000E-04,
4 5.080E-03,-3.610E-03, 1.700E-03, 1.830E-03, 6.800E-04, 4.000E-04,
5-3.580E-03, 6.000E-05,-2.600E-04,-1.050E-03,-3.800E-04,-2.300E-04,
6 2.420E-03, 9.300E-04,-1.000E-04, 4.500E-04, 1.700E-04, 1.100E-04,
1 9.868E-01,-1.171E+00, 3.940E-01,-8.459E-02, 1.124E-02,-1.250E-03,
2 1.001E+00,-1.383E+00, 5.044E-01,-1.152E-01, 1.658E-02,-1.830E-03,
3 4.928E-02,-1.368E-01, 9.021E-02,-2.935E-02, 5.800E-03,-6.600E-04,
4-3.133E-02, 5.785E-02,-2.023E-02, 2.630E-03, 1.600E-04,-8.000E-05,
5 8.840E-03,-1.416E-02, 1.900E-03, 5.800E-04,-2.500E-04, 1.000E-05,
6-2.300E-03, 3.080E-03, 5.500E-04,-3.700E-04, 7.000E-05, 1.000E-05/
C...Expansion coefficients for charm sea quark distribution.
DATA (((CEHLQ(IX,IT,NX,6,1),IX=1,6),IT=1,6),NX=1,2)/
1 9.270E-03,-1.817E-02, 9.590E-03,-6.390E-03, 1.690E-03,-1.540E-03,
2 5.710E-03,-1.188E-02, 6.090E-03,-4.650E-03, 1.240E-03,-1.310E-03,
3-3.960E-03, 7.100E-03,-3.590E-03, 1.840E-03,-3.900E-04, 3.400E-04,
4 1.120E-03,-1.960E-03, 1.120E-03,-4.800E-04, 1.000E-04,-4.000E-05,
5 4.000E-05,-3.000E-05,-1.800E-04, 9.000E-05,-5.000E-05,-2.000E-05,
6-4.200E-04, 7.300E-04,-1.600E-04, 5.000E-05, 5.000E-05, 5.000E-05,
1 8.098E-01,-1.042E+00, 3.398E-01,-6.824E-02, 8.760E-03,-9.000E-04,
2 8.961E-01,-1.217E+00, 4.339E-01,-9.287E-02, 1.304E-02,-1.290E-03,
3 3.058E-02,-1.040E-01, 7.604E-02,-2.415E-02, 4.600E-03,-5.000E-04,
4-2.451E-02, 4.432E-02,-1.651E-02, 1.430E-03, 1.200E-04,-1.000E-04,
5 1.122E-02,-1.457E-02, 2.680E-03, 5.800E-04,-1.200E-04, 3.000E-05,
6-7.730E-03, 7.330E-03,-7.600E-04,-2.400E-04, 1.000E-05, 0.000E+00/
DATA (((CEHLQ(IX,IT,NX,6,2),IX=1,6),IT=1,6),NX=1,2)/
1 9.980E-03,-1.945E-02, 1.055E-02,-6.870E-03, 1.860E-03,-1.560E-03,
2 5.700E-03,-1.203E-02, 6.250E-03,-4.860E-03, 1.310E-03,-1.370E-03,
3-4.490E-03, 7.990E-03,-4.170E-03, 2.050E-03,-4.400E-04, 3.300E-04,
4 1.470E-03,-2.480E-03, 1.460E-03,-5.700E-04, 1.200E-04,-1.000E-05,
5-9.000E-05, 1.500E-04,-3.200E-04, 1.200E-04,-6.000E-05,-4.000E-05,
6-4.200E-04, 7.600E-04,-1.400E-04, 4.000E-05, 7.000E-05, 5.000E-05,
1 8.698E-01,-1.131E+00, 3.836E-01,-8.111E-02, 1.048E-02,-1.300E-03,
2 9.626E-01,-1.321E+00, 4.854E-01,-1.091E-01, 1.583E-02,-1.700E-03,
3 3.057E-02,-1.088E-01, 8.022E-02,-2.676E-02, 5.590E-03,-5.600E-04,
4-2.845E-02, 5.164E-02,-1.918E-02, 2.210E-03,-4.000E-05,-1.500E-04,
5 1.311E-02,-1.751E-02, 3.310E-03, 5.100E-04,-1.200E-04, 5.000E-05,
6-8.590E-03, 8.380E-03,-9.200E-04,-2.600E-04, 1.000E-05,-1.000E-05/
C...Expansion coefficients for bottom sea quark distribution.
DATA (((CEHLQ(IX,IT,NX,7,1),IX=1,6),IT=1,6),NX=1,2)/
1 9.010E-03,-1.401E-02, 7.150E-03,-4.130E-03, 1.260E-03,-1.040E-03,
2 6.280E-03,-9.320E-03, 4.780E-03,-2.890E-03, 9.100E-04,-8.200E-04,
3-2.930E-03, 4.090E-03,-1.890E-03, 7.600E-04,-2.300E-04, 1.400E-04,
4 3.900E-04,-1.200E-03, 4.400E-04,-2.500E-04, 2.000E-05,-2.000E-05,
5 2.600E-04, 1.400E-04,-8.000E-05, 1.000E-04, 1.000E-05, 1.000E-05,
6-2.600E-04, 3.200E-04, 1.000E-05,-1.000E-05, 1.000E-05,-1.000E-05,
1 8.029E-01,-1.075E+00, 3.792E-01,-7.843E-02, 1.007E-02,-1.090E-03,
2 7.903E-01,-1.099E+00, 4.153E-01,-9.301E-02, 1.317E-02,-1.410E-03,
3-1.704E-02,-1.130E-02, 2.882E-02,-1.341E-02, 3.040E-03,-3.600E-04,
4-7.200E-04, 7.230E-03,-5.160E-03, 1.080E-03,-5.000E-05,-4.000E-05,
5 3.050E-03,-4.610E-03, 1.660E-03,-1.300E-04,-1.000E-05, 1.000E-05,
6-4.360E-03, 5.230E-03,-1.610E-03, 2.000E-04,-2.000E-05, 0.000E+00/
DATA (((CEHLQ(IX,IT,NX,7,2),IX=1,6),IT=1,6),NX=1,2)/
1 8.980E-03,-1.459E-02, 7.510E-03,-4.410E-03, 1.310E-03,-1.070E-03,
2 5.970E-03,-9.440E-03, 4.800E-03,-3.020E-03, 9.100E-04,-8.500E-04,
3-3.050E-03, 4.440E-03,-2.100E-03, 8.500E-04,-2.400E-04, 1.400E-04,
4 5.300E-04,-1.300E-03, 5.600E-04,-2.700E-04, 3.000E-05,-2.000E-05,
5 2.000E-04, 1.400E-04,-1.100E-04, 1.000E-04, 0.000E+00, 0.000E+00,
6-2.600E-04, 3.200E-04, 0.000E+00,-3.000E-05, 1.000E-05,-1.000E-05,
1 8.672E-01,-1.174E+00, 4.265E-01,-9.252E-02, 1.244E-02,-1.460E-03,
2 8.500E-01,-1.194E+00, 4.630E-01,-1.083E-01, 1.614E-02,-1.830E-03,
3-2.241E-02,-5.630E-03, 2.815E-02,-1.425E-02, 3.520E-03,-4.300E-04,
4-7.300E-04, 8.030E-03,-5.780E-03, 1.380E-03,-1.300E-04,-4.000E-05,
5 3.460E-03,-5.380E-03, 1.960E-03,-2.100E-04, 1.000E-05, 1.000E-05,
6-4.850E-03, 5.950E-03,-1.890E-03, 2.600E-04,-3.000E-05, 0.000E+00/
C...Expansion coefficients for top sea quark distribution.
DATA (((CEHLQ(IX,IT,NX,8,1),IX=1,6),IT=1,6),NX=1,2)/
1 4.410E-03,-7.480E-03, 3.770E-03,-2.580E-03, 7.300E-04,-7.100E-04,
2 3.840E-03,-6.050E-03, 3.030E-03,-2.030E-03, 5.800E-04,-5.900E-04,
3-8.800E-04, 1.660E-03,-7.500E-04, 4.700E-04,-1.000E-04, 1.000E-04,
4-8.000E-05,-1.500E-04, 1.200E-04,-9.000E-05, 3.000E-05, 0.000E+00,
5 1.300E-04,-2.200E-04,-2.000E-05,-2.000E-05,-2.000E-05,-2.000E-05,
6-7.000E-05, 1.900E-04,-4.000E-05, 2.000E-05, 0.000E+00, 0.000E+00,
1 6.623E-01,-9.248E-01, 3.519E-01,-7.930E-02, 1.110E-02,-1.180E-03,
2 6.380E-01,-9.062E-01, 3.582E-01,-8.479E-02, 1.265E-02,-1.390E-03,
3-2.581E-02, 2.125E-02, 4.190E-03,-4.980E-03, 1.490E-03,-2.100E-04,
4 7.100E-04, 5.300E-04,-1.270E-03, 3.900E-04,-5.000E-05,-1.000E-05,
5 3.850E-03,-5.060E-03, 1.860E-03,-3.500E-04, 4.000E-05, 0.000E+00,
6-3.530E-03, 4.460E-03,-1.500E-03, 2.700E-04,-3.000E-05, 0.000E+00/
DATA (((CEHLQ(IX,IT,NX,8,2),IX=1,6),IT=1,6),NX=1,2)/
1 4.260E-03,-7.530E-03, 3.830E-03,-2.680E-03, 7.600E-04,-7.300E-04,
2 3.640E-03,-6.050E-03, 3.030E-03,-2.090E-03, 5.900E-04,-6.000E-04,
3-9.200E-04, 1.710E-03,-8.200E-04, 5.000E-04,-1.200E-04, 1.000E-04,
4-5.000E-05,-1.600E-04, 1.300E-04,-9.000E-05, 3.000E-05, 0.000E+00,
5 1.300E-04,-2.100E-04,-1.000E-05,-2.000E-05,-2.000E-05,-1.000E-05,
6-8.000E-05, 1.800E-04,-5.000E-05, 2.000E-05, 0.000E+00, 0.000E+00,
1 7.146E-01,-1.007E+00, 3.932E-01,-9.246E-02, 1.366E-02,-1.540E-03,
2 6.856E-01,-9.828E-01, 3.977E-01,-9.795E-02, 1.540E-02,-1.790E-03,
3-3.053E-02, 2.758E-02, 2.150E-03,-4.880E-03, 1.640E-03,-2.500E-04,
4 9.200E-04, 4.200E-04,-1.340E-03, 4.600E-04,-8.000E-05,-1.000E-05,
5 4.230E-03,-5.660E-03, 2.140E-03,-4.300E-04, 6.000E-05, 0.000E+00,
6-3.890E-03, 5.000E-03,-1.740E-03, 3.300E-04,-4.000E-05, 0.000E+00/
C...The following data lines are coefficients needed in the
C...Duke, Owens proton structure function parametrizations, see below.
C...Expansion coefficients for (up+down) valence quark distribution.
DATA ((CDO(IP,IS,1,1),IS=1,6),IP=1,3)/
1 4.190E-01, 3.460E+00, 4.400E+00, 0.000E+00, 0.000E+00, 0.000E+00,
2 4.000E-03, 7.240E-01,-4.860E+00, 0.000E+00, 0.000E+00, 0.000E+00,
3-7.000E-03,-6.600E-02, 1.330E+00, 0.000E+00, 0.000E+00, 0.000E+00/
DATA ((CDO(IP,IS,1,2),IS=1,6),IP=1,3)/
1 3.740E-01, 3.330E+00, 6.030E+00, 0.000E+00, 0.000E+00, 0.000E+00,
2 1.400E-02, 7.530E-01,-6.220E+00, 0.000E+00, 0.000E+00, 0.000E+00,
3 0.000E+00,-7.600E-02, 1.560E+00, 0.000E+00, 0.000E+00, 0.000E+00/
C...Expansion coefficients for down valence quark distribution.
DATA ((CDO(IP,IS,2,1),IS=1,6),IP=1,3)/
1 7.630E-01, 4.000E+00, 0.000E+00, 0.000E+00, 0.000E+00, 0.000E+00,
2-2.370E-01, 6.270E-01,-4.210E-01, 0.000E+00, 0.000E+00, 0.000E+00,
3 2.600E-02,-1.900E-02, 3.300E-02, 0.000E+00, 0.000E+00, 0.000E+00/
DATA ((CDO(IP,IS,2,2),IS=1,6),IP=1,3)/
1 7.610E-01, 3.830E+00, 0.000E+00, 0.000E+00, 0.000E+00, 0.000E+00,
2-2.320E-01, 6.270E-01,-4.180E-01, 0.000E+00, 0.000E+00, 0.000E+00,
3 2.300E-02,-1.900E-02, 3.600E-02, 0.000E+00, 0.000E+00, 0.000E+00/
C...Expansion coefficients for (up+down+strange) sea quark distribution.
DATA ((CDO(IP,IS,3,1),IS=1,6),IP=1,3)/
1 1.265E+00, 0.000E+00, 8.050E+00, 0.000E+00, 0.000E+00, 0.000E+00,
2-1.132E+00,-3.720E-01, 1.590E+00, 6.310E+00,-1.050E+01, 1.470E+01,
3 2.930E-01,-2.900E-02,-1.530E-01,-2.730E-01,-3.170E+00, 9.800E+00/
DATA ((CDO(IP,IS,3,2),IS=1,6),IP=1,3)/
1 1.670E+00, 0.000E+00, 9.150E+00, 0.000E+00, 0.000E+00, 0.000E+00,
2-1.920E+00,-2.730E-01, 5.300E-01, 1.570E+01,-1.010E+02, 2.230E+02,
3 5.820E-01,-1.640E-01,-7.630E-01,-2.830E+00, 4.470E+01,-1.170E+02/
C...Expansion coefficients for charm sea quark distribution.
DATA ((CDO(IP,IS,4,1),IS=1,6),IP=1,3)/
1 0.000E+00,-3.600E-02, 6.350E+00, 0.000E+00, 0.000E+00, 0.000E+00,
2 1.350E-01,-2.220E-01, 3.260E+00,-3.030E+00, 1.740E+01,-1.790E+01,
3-7.500E-02,-5.800E-02,-9.090E-01, 1.500E+00,-1.130E+01, 1.560E+01/
DATA ((CDO(IP,IS,4,2),IS=1,6),IP=1,3)/
1 0.000E+00,-1.200E-01, 3.510E+00, 0.000E+00, 0.000E+00, 0.000E+00,
2 6.700E-02,-2.330E-01, 3.660E+00,-4.740E-01, 9.500E+00,-1.660E+01,
3-3.100E-02,-2.300E-02,-4.530E-01, 3.580E-01,-5.430E+00, 1.550E+01/
C...Expansion coefficients for gluon distribution.
DATA ((CDO(IP,IS,5,1),IS=1,6),IP=1,3)/
1 1.560E+00, 0.000E+00, 6.000E+00, 9.000E+00, 0.000E+00, 0.000E+00,
2-1.710E+00,-9.490E-01, 1.440E+00,-7.190E+00,-1.650E+01, 1.530E+01,
3 6.380E-01, 3.250E-01,-1.050E+00, 2.550E-01, 1.090E+01,-1.010E+01/
DATA ((CDO(IP,IS,5,2),IS=1,6),IP=1,3)/
1 8.790E-01, 0.000E+00, 4.000E+00, 9.000E+00, 0.000E+00, 0.000E+00,
2-9.710E-01,-1.160E+00, 1.230E+00,-5.640E+00,-7.540E+00,-5.960E-01,
3 4.340E-01, 4.760E-01,-2.540E-01,-8.170E-01, 5.500E+00, 1.260E-01/
C...The following data lines are coefficients needed in the
C...Owens pion structure function parametrizations, see below.
C...Expansion coefficients for up and down valence quark distributions.
DATA ((COW(IP,IS,1,1),IS=1,5),IP=1,3)/
1 4.0000E-01, 7.0000E-01, 0.0000E+00, 0.0000E+00, 0.0000E+00,
2 -6.2120E-02, 6.4780E-01, 0.0000E+00, 0.0000E+00, 0.0000E+00,
3 -7.1090E-03, 1.3350E-02, 0.0000E+00, 0.0000E+00, 0.0000E+00/
DATA ((COW(IP,IS,1,2),IS=1,5),IP=1,3)/
1 4.0000E-01, 6.2800E-01, 0.0000E+00, 0.0000E+00, 0.0000E+00,
2 -5.9090E-02, 6.4360E-01, 0.0000E+00, 0.0000E+00, 0.0000E+00,
3 -6.5240E-03, 1.4510E-02, 0.0000E+00, 0.0000E+00, 0.0000E+00/
C...Expansion coefficients for gluon distribution.
DATA ((COW(IP,IS,2,1),IS=1,5),IP=1,3)/
1 8.8800E-01, 0.0000E+00, 3.1100E+00, 6.0000E+00, 0.0000E+00,
2 -1.8020E+00, -1.5760E+00, -1.3170E-01, 2.8010E+00, -1.7280E+01,
3 1.8120E+00, 1.2000E+00, 5.0680E-01, -1.2160E+01, 2.0490E+01/
DATA ((COW(IP,IS,2,2),IS=1,5),IP=1,3)/
1 7.9400E-01, 0.0000E+00, 2.8900E+00, 6.0000E+00, 0.0000E+00,
2 -9.1440E-01, -1.2370E+00, 5.9660E-01, -3.6710E+00, -8.1910E+00,
3 5.9660E-01, 6.5820E-01, -2.5500E-01, -2.3040E+00, 7.7580E+00/
C...Expansion coefficients for (up+down+strange) quark sea distribution.
DATA ((COW(IP,IS,3,1),IS=1,5),IP=1,3)/
1 9.0000E-01, 0.0000E+00, 5.0000E+00, 0.0000E+00, 0.0000E+00,
2 -2.4280E-01, -2.1200E-01, 8.6730E-01, 1.2660E+00, 2.3820E+00,
3 1.3860E-01, 3.6710E-03, 4.7470E-02, -2.2150E+00, 3.4820E-01/
DATA ((COW(IP,IS,3,2),IS=1,5),IP=1,3)/
1 9.0000E-01, 0.0000E+00, 5.0000E+00, 0.0000E+00, 0.0000E+00,
2 -1.4170E-01, -1.6970E-01, -2.4740E+00, -2.5340E+00, 5.6210E-01,
3 -1.7400E-01, -9.6230E-02, 1.5750E+00, 1.3780E+00, -2.7010E-01/
C...Expansion coefficients for charm quark sea distribution.
DATA ((COW(IP,IS,4,1),IS=1,5),IP=1,3)/
1 0.0000E+00, -2.2120E-02, 2.8940E+00, 0.0000E+00, 0.0000E+00,
2 7.9280E-02, -3.7850E-01, 9.4330E+00, 5.2480E+00, 8.3880E+00,
3 -6.1340E-02, -1.0880E-01, -1.0852E+01, -7.1870E+00, -1.1610E+01/
DATA ((COW(IP,IS,4,2),IS=1,5),IP=1,3)/
1 0.0000E+00, -8.8200E-02, 1.9240E+00, 0.0000E+00, 0.0000E+00,
2 6.2290E-02, -2.8920E-01, 2.4240E-01, -4.4630E+00, -8.3670E-01,
3 -4.0990E-02, -1.0820E-01, 2.0360E+00, 5.2090E+00, -4.8400E-02/
C...Euler's beta function, requires ordinary Gamma function
EULBET(X,Y)=PYHIGAMM(X)*PYHIGAMM(Y)/PYHIGAMM(X+Y)
C...Reset structure functions, check x and hadron flavour.
ALAM=0.
DO 100 KFL=-6,6
100 XPQ(KFL)=0.
IF(X.LT.0..OR.X.GT.1.) THEN
WRITE(MSTU(11),1000) X
RETURN
ENDIF
KFA=IABS(KF)
IF(KFA.NE.211.AND.KFA.NE.2212.AND.KFA.NE.2112) THEN
WRITE(MSTU(11),1100) KF
RETURN
ENDIF
C...Call user-supplied structure function. Select proton/neutron/pion.
IF(MSTP(51).EQ.0.OR.MSTP(52).GE.2) THEN
KFE=KFA
IF(KFA.EQ.2112) KFE=2212
CALL PYHISTFE(KFE,X,Q2,XPQ)
GOTO 230
ENDIF
IF(KFA.EQ.211) GOTO 200
IF(MSTP(51).EQ.1.OR.MSTP(51).EQ.2) THEN
C...Proton structure functions from Eichten, Hinchliffe, Lane, Quigg.
C...Allowed variable range: 5 GeV2 < Q2 < 1E8 GeV2; 1E-4 < x < 1
C...Determine set, Lamdba and x and t expansion variables.
NSET=MSTP(51)
IF(NSET.EQ.1) ALAM=0.2
IF(NSET.EQ.2) ALAM=0.29
TMIN=LOG(5./ALAM**2)
TMAX=LOG(1E8/ALAM**2)
IF(MSTP(52).EQ.0) THEN
T=TMIN
ELSE
T=LOG(Q2/ALAM**2)
ENDIF
VT=MAX(-1.,MIN(1.,(2.*T-TMAX-TMIN)/(TMAX-TMIN)))
NX=1
IF(X.LE.0.1) NX=2
IF(NX.EQ.1) VX=(2.*X-1.1)/0.9
IF(NX.EQ.2) VX=MAX(-1.,(2.*LOG(X)+11.51293)/6.90776)
CXS=1.
IF(X.LT.1E-4.AND.ABS(PARP(51)-1.).GT.0.01) CXS=
& (1E-4/X)**(PARP(51)-1.)
C...Chebyshev polynomials for x and t expansion.
TX(1)=1.
TX(2)=VX
TX(3)=2.*VX**2-1.
TX(4)=4.*VX**3-3.*VX
TX(5)=8.*VX**4-8.*VX**2+1.
TX(6)=16.*VX**5-20.*VX**3+5.*VX
TT(1)=1.
TT(2)=VT
TT(3)=2.*VT**2-1.
TT(4)=4.*VT**3-3.*VT
TT(5)=8.*VT**4-8.*VT**2+1.
TT(6)=16.*VT**5-20.*VT**3+5.*VT
C...Calculate structure functions.
DO 120 KFL=1,6
XQSUM=0.
DO 110 IT=1,6
DO 110 IX=1,6
110 XQSUM=XQSUM+CEHLQ(IX,IT,NX,KFL,NSET)*TX(IX)*TT(IT)
120 XQ(KFL)=XQSUM*(1.-X)**NEHLQ(KFL,NSET)*CXS
C...Put into output array.
XPQ(0)=XQ(4)
XPQ(1)=XQ(2)+XQ(3)
XPQ(2)=XQ(1)+XQ(3)
XPQ(3)=XQ(5)
XPQ(4)=XQ(6)
XPQ(-1)=XQ(3)
XPQ(-2)=XQ(3)
XPQ(-3)=XQ(5)
XPQ(-4)=XQ(6)
C...Special expansion for bottom (threshold effects).
IF(MSTP(54).GE.5) THEN
IF(NSET.EQ.1) TMIN=8.1905
IF(NSET.EQ.2) TMIN=7.4474
IF(T.LE.TMIN) GOTO 140
VT=MAX(-1.,MIN(1.,(2.*T-TMAX-TMIN)/(TMAX-TMIN)))
TT(1)=1.
TT(2)=VT
TT(3)=2.*VT**2-1.
TT(4)=4.*VT**3-3.*VT
TT(5)=8.*VT**4-8.*VT**2+1.
TT(6)=16.*VT**5-20.*VT**3+5.*VT
XQSUM=0.
DO 130 IT=1,6
DO 130 IX=1,6
130 XQSUM=XQSUM+CEHLQ(IX,IT,NX,7,NSET)*TX(IX)*TT(IT)
XPQ(5)=XQSUM*(1.-X)**NEHLQ(7,NSET)
XPQ(-5)=XPQ(5)
140 CONTINUE
ENDIF
C...Special expansion for top (threshold effects).
IF(MSTP(54).GE.6) THEN
IF(NSET.EQ.1) TMIN=11.5528
IF(NSET.EQ.2) TMIN=10.8097
TMIN=TMIN+2.*LOG(PMAS(6,1)/30.)
TMAX=TMAX+2.*LOG(PMAS(6,1)/30.)
IF(T.LE.TMIN) GOTO 160
VT=MAX(-1.,MIN(1.,(2.*T-TMAX-TMIN)/(TMAX-TMIN)))
TT(1)=1.
TT(2)=VT
TT(3)=2.*VT**2-1.
TT(4)=4.*VT**3-3.*VT
TT(5)=8.*VT**4-8.*VT**2+1.
TT(6)=16.*VT**5-20.*VT**3+5.*VT
XQSUM=0.
DO 150 IT=1,6
DO 150 IX=1,6
150 XQSUM=XQSUM+CEHLQ(IX,IT,NX,8,NSET)*TX(IX)*TT(IT)
XPQ(6)=XQSUM*(1.-X)**NEHLQ(8,NSET)
XPQ(-6)=XPQ(6)
160 CONTINUE
ENDIF
ELSEIF(MSTP(51).EQ.3.OR.MSTP(51).EQ.4) THEN
C...Proton structure functions from Duke, Owens.
C...Allowed variable range: 4 GeV2 < Q2 < approx 1E6 GeV2.
C...Determine set, Lambda and s expansion parameter.
NSET=MSTP(51)-2
IF(NSET.EQ.1) ALAM=0.2
IF(NSET.EQ.2) ALAM=0.4
IF(MSTP(52).LE.0) THEN
SD=0.
ELSE
SD=LOG(LOG(MAX(Q2,4.)/ALAM**2)/LOG(4./ALAM**2))
ENDIF
C...Calculate structure functions.
DO 180 KFL=1,5
DO 170 IS=1,6
170 TS(IS)=CDO(1,IS,KFL,NSET)+CDO(2,IS,KFL,NSET)*SD+
& CDO(3,IS,KFL,NSET)*SD**2
IF(KFL.LE.2) THEN
XQ(KFL)=X**TS(1)*(1.-X)**TS(2)*(1.+TS(3)*X)/(EULBET(TS(1),
& TS(2)+1.)*(1.+TS(3)*TS(1)/(TS(1)+TS(2)+1.)))
ELSE
XQ(KFL)=TS(1)*X**TS(2)*(1.-X)**TS(3)*(1.+TS(4)*X+TS(5)*X**2+
& TS(6)*X**3)
ENDIF
180 CONTINUE
C...Put into output arrays.
XPQ(0)=XQ(5)
XPQ(1)=XQ(2)+XQ(3)/6.
XPQ(2)=3.*XQ(1)-XQ(2)+XQ(3)/6.
XPQ(3)=XQ(3)/6.
XPQ(4)=XQ(4)
XPQ(-1)=XQ(3)/6.
XPQ(-2)=XQ(3)/6.
XPQ(-3)=XQ(3)/6.
XPQ(-4)=XQ(4)
C...Proton structure functions from Diemoz, Ferroni, Longo, Martinelli.
C...These are accessed via PYHISTFE since the files needed may not always
C...available.
ELSEIF(MSTP(51).GE.11.AND.MSTP(51).LE.13) THEN
CALL PYHISTFE(2212,X,Q2,XPQ)
C...Unknown proton parametrization.
ELSE
WRITE(MSTU(11),1200) MSTP(51)
ENDIF
GOTO 230
200 IF((MSTP(51).GE.1.AND.MSTP(51).LE.4).OR.
&(MSTP(51).GE.11.AND.MSTP(51).LE.13)) THEN
C...Pion structure functions from Owens.
C...Allowed variable range: 4 GeV2 < Q2 < approx 2000 GeV2.
C...Determine set, Lambda and s expansion variable.
NSET=1
IF(MSTP(51).EQ.2.OR.MSTP(51).EQ.4.OR.MSTP(51).EQ.13) NSET=2
IF(NSET.EQ.1) ALAM=0.2
IF(NSET.EQ.2) ALAM=0.4
IF(MSTP(52).LE.0) THEN
SD=0.
ELSE
SD=LOG(LOG(MAX(Q2,4.)/ALAM**2)/LOG(4./ALAM**2))
ENDIF
C...Calculate structure functions.
DO 220 KFL=1,4
DO 210 IS=1,5
210 TS(IS)=COW(1,IS,KFL,NSET)+COW(2,IS,KFL,NSET)*SD+
& COW(3,IS,KFL,NSET)*SD**2
IF(KFL.EQ.1) THEN
XQ(KFL)=X**TS(1)*(1.-X)**TS(2)/EULBET(TS(1),TS(2)+1.)
ELSE
XQ(KFL)=TS(1)*X**TS(2)*(1.-X)**TS(3)*(1.+TS(4)*X+TS(5)*X**2)
ENDIF
220 CONTINUE
C...Put into output arrays.
XPQ(0)=XQ(2)
XPQ(1)=XQ(3)/6.
XPQ(2)=XQ(1)+XQ(3)/6.
XPQ(3)=XQ(3)/6.
XPQ(4)=XQ(4)
XPQ(-1)=XQ(1)+XQ(3)/6.
XPQ(-2)=XQ(3)/6.
XPQ(-3)=XQ(3)/6.
XPQ(-4)=XQ(4)
C...Unknown pion parametrization.
ELSE
WRITE(MSTU(11),1200) MSTP(51)
ENDIF
C...Isospin conjugation for neutron, charge conjugation for antipart.
230 IF(KFA.EQ.2112) THEN
XPS=XPQ(1)
XPQ(1)=XPQ(2)
XPQ(2)=XPS
XPS=XPQ(-1)
XPQ(-1)=XPQ(-2)
XPQ(-2)=XPS
ENDIF
IF(KF.LT.0) THEN
DO 240 KFL=1,4
XPS=XPQ(KFL)
XPQ(KFL)=XPQ(-KFL)
240 XPQ(-KFL)=XPS
ENDIF
C...Check positivity and reset above maximum allowed flavour.
DO 250 KFL=-6,6
XPQ(KFL)=MAX(0.,XPQ(KFL))
250 IF(IABS(KFL).GT.MSTP(54)) XPQ(KFL)=0.
C...consider nuclear effect on the structure function
IF((JBT.NE.1.AND.JBT.NE.2).OR.IHPR2(6).EQ.0
& .OR.IHNT2(16).EQ.1) GO TO 400
ATNM=IHNT2(2*JBT-1)
IF(ATNM.LE.1.0) GO TO 400
IF(JBT.EQ.1) THEN
BBR2=(YP(1,IHNT2(11))**2+YP(2,IHNT2(11))**2)/1.44/ATNM**0.66666
ELSEIF(JBT.EQ.2) THEN
BBR2=(YT(1,IHNT2(12))**2+YT(2,IHNT2(12))**2)/1.44/ATNM**0.66666
ENDIF
BBR2=MIN(1.0,BBR2)
ABX=(ATNM**0.33333333-1.0)
APX=HIPR1(6)*4.0/3.0*ABX*SQRT(1.0-BBR2)
AAX=1.192*ALOG(ATNM)**0.1666666
RRX=AAX*(X**3-1.2*X**2+0.21*X)+1.0
& -(APX-1.079*ABX*SQRT(X)/ALOG(ATNM+1.0))*EXP(-X**2.0/0.01)
DO 300 KFL=-6,6
XPQ(KFL)=XPQ(KFL)*RRX
300 CONTINUE
C ********consider the nuclear effect on the structure
C fucntion which also depends on the impact
C parameter of the nuclear reaction
400 CONTINUE
C...Formats for error printouts.
1000 FORMAT(' Error: x value outside physical range, x =',1P,E12.3)
1100 FORMAT(' Error: illegal particle code for structure function,',
&' KF =',I5)
1200 FORMAT(' Error: bad value of parameter MSTP(51) in PYHISTFU,',
&' MSTP(51) =',I5)
RETURN
END