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Add SARAH model files for the SE6SSM
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Dylan Harries
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Mar 15, 2017
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| Off[General::spell] | ||
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| Model`Name = "SE6SSM"; | ||
| Model`NameLaTeX = "SE6SSM"; | ||
| Model`Authors = "P.Athron,D.Harries"; | ||
| Model`Date = "2013-11-10"; | ||
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| (*-------------------------------------------*) | ||
| (* Particle Content *) | ||
| (*-------------------------------------------*) | ||
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| (* Global symmetries *) | ||
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| Global[[1]] = {Z[2], HParity}; | ||
| HpM = {-1,-1,1}; | ||
| HpP = {1,1,-1}; | ||
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| Global[[2]] = {Z[2], EParity}; | ||
| EpM = -1; | ||
| EpP = 1; | ||
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| (* Vector Superfields *) | ||
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| Gauge[[1]] = {B, U[1], hypercharge, g1, False, HpM, EpP}; | ||
| Gauge[[2]] = {WB, SU[2], left, g2, True, HpM, EpP}; | ||
| Gauge[[3]] = {G, SU[3], color, g3, False, HpM, EpP}; | ||
| Gauge[[4]] = {Bp, U[1], Ncharge, g1p, False, HpM, EpP}; | ||
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| (* Chiral Superfields *) | ||
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| SuperFields[[1]] = {q, 3, {uL, dL}, 1/6, 2, 3, 1 / Sqrt[40], HpM, EpP}; | ||
| SuperFields[[2]] = {l, 3, {vL, eL}, -1/2, 2, 1, 2 / Sqrt[40], HpM, EpP}; | ||
| SuperFields[[3]] = {Hd, 1, {Hd0, Hdm}, -1/2, 2, 1, -3 / Sqrt[40], HpP, EpP}; | ||
| SuperFields[[4]] = {Hu, 1, {Hup, Hu0}, 1/2, 2, 1, -2 / Sqrt[40], HpP, EpP}; | ||
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| SuperFields[[5]] = {d, 3, conj[dR], 1/3, 1, -3, 2 / Sqrt[40], HpM, EpP}; | ||
| SuperFields[[6]] = {u, 3, conj[uR], -2/3, 1, -3, 1 / Sqrt[40], HpM, EpP}; | ||
| SuperFields[[7]] = {e, 3, conj[eR], 1, 1, 1, 1 / Sqrt[40], HpM, EpP}; | ||
| SuperFields[[8]] = {s, 1, sR, 0, 1, 1, 5 / Sqrt[40], HpP, EpP}; | ||
| SuperFields[[9]] = {sbar, 1, sbarR, 0, 1, 1, -5 / Sqrt[40], HpP, EpP}; | ||
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| SuperFields[[10]] = {H1I, 2, {H1I0, H1Im}, -1/2, 2, 1, -3 / Sqrt[40], HpM, EpM}; | ||
| SuperFields[[11]] = {H2I, 2, {H2Ip, H2I0}, 1/2, 2, 1, -2 / Sqrt[40], HpM, EpM}; | ||
| SuperFields[[12]] = {SI, 3, SIR, 0, 1, 1, 5 / Sqrt[40], HpM, EpM}; | ||
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| SuperFields[[13]] = {Dx, 3, DxL, -1/3, 1, 3, -2 / Sqrt[40], HpM, EpM}; | ||
| SuperFields[[14]] = {Dxbar, 3, conj[DxbarR], 1/3, 1, -3, -3 / Sqrt[40], HpM, EpM}; | ||
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| SuperFields[[15]] = {L4, 1, {L40, L4m}, -1/2, 2, 1, 2 / Sqrt[40], HpP, EpM}; | ||
| SuperFields[[16]] = {L4bar, 1, {L4barp, L4bar0}, 1/2, 2, 1, -2 / Sqrt[40], HpP, EpM}; | ||
| SuperFields[[17]] = {phi, 1, phiR, 0, 1, 1, 0, HpP, EpP}; | ||
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| NoU1Mixing = True; | ||
| AddMixedSofts = False; | ||
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| (*------------------------------------------------------*) | ||
| (* Z_2^H Exact Superpotential *) | ||
| (*------------------------------------------------------*) | ||
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| SuperPotential = Yu u.q.Hu - Yd d.q.Hd - Ye e.l.Hd + \[Lambda] s.Hu.Hd + \[Lambda]12 s.H2I.H1I + \[Kappa] s.Dx.Dxbar + \[Mu]L L4bar.L4 - \[Sigma] phi.s.sbar + \[Kappa]Pr/3 phi.phi.phi + \[Mu]Phi/2 phi.phi + \[Xi]F phi + fu SI.H1I.Hu + fd SI.Hd.H2I + gD q.L4.Dxbar + hE e.H1I.L4 + \[Sigma]L phi.L4.L4bar; | ||
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| (*-------------------------------------------*) | ||
| (* Integrate Out or Delete Particles *) | ||
| (*-------------------------------------------*) | ||
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| IntegrateOut = {}; | ||
| DeleteParticles = {}; | ||
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| (*----------------------------------------------*) | ||
| (* ROTATIONS *) | ||
| (*----------------------------------------------*) | ||
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| NameOfStates = {GaugeES, EWSB}; | ||
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| (* ----- Before EWSB ----- *) | ||
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| DEFINITION[GaugeES][DiracSpinors] = { | ||
| Bino -> {fB, conj[fB]}, | ||
| Wino -> {fWB, conj[fWB]}, | ||
| Glu -> {fG, conj[fG]}, | ||
| (* H0 -> {FHd0, conj[FHu0]}, | ||
| HC -> {FHdm, conj[FHup]}, *) | ||
| H01 -> {FHd0, 0}, | ||
| H02 -> {0, conj[FHu0]}, | ||
| HC1 -> {FHdm, 0}, | ||
| HC2 -> {0, conj[FHup]}, | ||
| Fd1 -> {FdL, 0}, | ||
| Fd2 -> {0, FdR}, | ||
| Fu1 -> {FuL, 0}, | ||
| Fu2 -> {0, FuR}, | ||
| Fe1 -> {FeL, 0}, | ||
| Fe2 -> {0, FeR}, | ||
| Fv -> {FvL, 0}, | ||
| FS1 -> {FsR, 0}, | ||
| FS2 -> {0, conj[FsR]}, | ||
| FSbar1 -> {FsbarR, 0}, | ||
| FSbar2 -> {0, conj[FsbarR]}, | ||
| Fphi1 -> {FphiR, 0}, | ||
| Fphi2 -> {0, conj[FphiR]}, | ||
| FBp -> {fBp, conj[fBp]}, | ||
| H0I1 -> {FH1I0, 0}, | ||
| H0I2 -> {0, conj[FH2I0]}, | ||
| HCI1 -> {FH1Im, 0}, | ||
| HCI2 -> {0, conj[FH2Ip]}, | ||
| FSI1 -> {FSIR, 0}, | ||
| FSI2 -> {0, conj[FSIR]}, | ||
| FDx1 -> {FDxL, 0}, | ||
| FDx2 -> {0, FDxbarR}, | ||
| Hp01 -> {FL40, 0}, | ||
| Hp02 -> {0, conj[FL4bar0]} | ||
| }; | ||
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| (* ----- After EWSB ----- *) | ||
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| (* Gauge Sector *) | ||
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| DEFINITION[EWSB][GaugeSector] = { | ||
| {{VB, VWB[3], VBp}, {VP, VZ, VZp}, ZZ}, | ||
| {{VWB[1], VWB[2]}, {VWm, conj[VWm]}, ZW}, | ||
| {{fWB[1], fWB[2], fWB[3]}, {fWm, fWp, fW0}, ZfW} | ||
| }; | ||
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| (* ----- VEVs ---- *) | ||
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| DEFINITION[EWSB][VEVs]= { | ||
| {SHd0, {vd, 1 / Sqrt[2]}, {sigmad, \[ImaginaryI] / Sqrt[2]}, {phid, 1 / Sqrt[2]}}, | ||
| {SHu0, {vu, 1 / Sqrt[2]}, {sigmau, \[ImaginaryI] / Sqrt[2]}, {phiu, 1 / Sqrt[2]}}, | ||
| {SsR, {vs, 1 / Sqrt[2]}, {sigmaS, \[ImaginaryI] / Sqrt[2]}, {phiS, 1 / Sqrt[2]}}, | ||
| {SsbarR, {vsb, 1 / Sqrt[2]}, {sigmaSbar, \[ImaginaryI] / Sqrt[2]}, {phiSbar, 1 / Sqrt[2]}}, | ||
| {SphiR, {vphi, 1 / Sqrt[2]}, {sigmaPhi, \[ImaginaryI] / Sqrt[2]}, {phiPhi, 1 / Sqrt[2]}}, | ||
| {SH1I0, {0, 0}, {sigmaH1I0, \[ImaginaryI] / Sqrt[2]}, {phiH1I0, 1 / Sqrt[2]}}, | ||
| {SH2I0, {0, 0}, {sigmaH2I0, \[ImaginaryI] / Sqrt[2]}, {phiH2I0, 1 / Sqrt[2]}}, | ||
| {SSIR, {0, 0}, {sigmaSIR, \[ImaginaryI] / Sqrt[2]}, {phiSIR, 1 / Sqrt[2]}} | ||
| }; | ||
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| (* ---- Mixings ---- *) | ||
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| DEFINITION[EWSB][MatterSector] = { | ||
| {{SdL, SdR}, {Sd, ZD}}, | ||
| {{SuL, SuR}, {Su, ZU}}, | ||
| {{SeL, SeR}, {Se, ZE}}, | ||
| {{SvL}, {Sv, ZV}}, | ||
| {{SDxL, SDxbarR}, {SDX, ZDX}}, | ||
| {{phid, phiu, phiS, phiSbar, phiPhi}, {hh, ZH}}, | ||
| {{sigmad, sigmau, sigmaS, sigmaSbar, sigmaPhi}, {Ah, ZA}}, | ||
| {{SHdm, conj[SHup]}, {Hpm, ZP}}, | ||
| {{fB, fW0, FHd0, FHu0, FsR, FsbarR, FphiR, fBp}, {L0, ZN}}, | ||
| {{{fWm, FHdm}, {fWp, FHup}}, {{Lm, UM}, {Lp, UP}}}, | ||
| {{{FeL}, {conj[FeR]}}, {{FEL, ZEL}, {FER, ZER}}}, | ||
| {{{FdL}, {conj[FdR]}}, {{FDL, ZDL}, {FDR, ZDR}}}, | ||
| {{{FuL}, {conj[FuR]}}, {{FUL, ZUL}, {FUR, ZUR}}}, | ||
| {{{FDxL}, {conj[FDxbarR]}}, {{FDXL, ZDXL}, {FDXR, ZDXR}}}, | ||
| {{phiH1I0, phiH2I0, phiSIR}, {hhI, ZHI}}, | ||
| {{sigmaH1I0, sigmaH2I0, sigmaSIR}, {AhI, ZAI}}, | ||
| {{SH1Im, conj[SH2Ip]}, {SHIPM, ZPI}}, | ||
| {{{FH1Im}, {FH2Ip}}, {{LmI, UMI}, {LpI, UPI}}}, | ||
| {{FH1I0, FH2I0, FSIR}, {L0I, ZNI}}, | ||
| {{SL40, conj[SL4bar0]}, {SHp0, ZHp}}, | ||
| {{SL4m, conj[SL4barp]}, {SHpp, ZPp}}, | ||
| {{FL40, FL4bar0}, {L0p, ZNp}} | ||
| }; | ||
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| DEFINITION[EWSB][Phases] = { | ||
| {fG, PhaseGlu}, | ||
| {FL4m, PhaseChaP} | ||
| }; | ||
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| DEFINITION[EWSB][DiracSpinors] = { | ||
| Fd -> {FDL, conj[FDR]}, | ||
| Fe -> {FEL, conj[FER]}, | ||
| Fu -> {FUL, conj[FUR]}, | ||
| Fv -> {FvL, 0}, | ||
| Chi -> {L0, conj[L0]}, | ||
| Cha -> {Lm, conj[Lp]}, | ||
| Glu -> {fG, conj[fG]}, | ||
| ChiI -> {L0I, conj[L0I]}, | ||
| ChaI -> {LmI, conj[LpI]}, | ||
| ChiP -> {L0p, conj[L0p]}, | ||
| ChaP -> {FL4m, conj[FL4barp]}, | ||
| FDX -> {FDXL, conj[FDXR]} | ||
| }; |
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