| 1 | (***************************************************************************************************************)
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| 2 | (****** This is the FeynRules mod-file for 2 Gravitons coupled to Standard Model (2GravitonsSM). ******)
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| 3 | (****** ******)
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| 4 | (****** Authors: Tran Quang Loc, developed from SM file of N. Christensen, C. Duhr, B. Fuks ******)
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| 5 | (****** ******)
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| 6 | (****** Choose whether Feynman gauge is desired. ******)
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| 7 | (****** If set to False, unitary gauge is assumed. ****)
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| 8 | (****** Feynman gauge is especially useful for CalcHEP/CompHEP where the calculation is 10-100 times faster. ***)
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| 9 | (****** Feynman gauge is not supported in MadGraph and Sherpa. ****)
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| 10 | (***************************************************************************************************************)
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| 11 |
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| 12 | (* ************************** *)
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| 13 | (* ***** Information ***** *)
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| 14 | (* ************************** *)
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| 15 | M$ModelName = "2 Gravitons coupled to Standard Model";
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| 16 |
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| 17 | M$Information = {
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| 18 | Authors -> {"Tran Quang Loc"},
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| 19 | Version -> "1.0.0",
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| 20 | Date -> "05. 09. 2021",
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| 21 | Institutions -> {"DAMTP, Cambridge"},
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| 22 | Emails -> {"loctranq@gmail.com"},
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| 23 | URLs -> "https://feynrules.irmp.ucl.ac.be/wiki/2GravitonsSM"
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| 24 | };
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| 25 |
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| 26 | FeynmanGauge = True;
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| 27 |
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| 28 | (* ************************** *)
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| 29 | (* ***** NLO Variables ****** *)
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| 30 | (******************************)
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| 31 |
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| 32 | FR$LoopSwitches = {{Gf, MW}};
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| 33 | FR$RmDblExt = { ymb -> MB, ymc -> MC, ymdo -> MD, yme -> Me,
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| 34 | ymm -> MMU, yms -> MS, ymt -> MT, ymtau -> MTA, ymup -> MU};
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| 35 |
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| 36 | (* ************************** *)
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| 37 | (* ***** Change log ***** *)
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| 38 | (* ************************** *)
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| 39 |
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| 40 | (* v1.0.0: Implement the first model *)
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| 41 |
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| 42 | (* ************************** *)
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| 43 | (* ***** vevs ***** *)
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| 44 | (* ************************** *)
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| 45 | M$vevs = { {Phi[2],vev} };
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| 46 |
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| 47 | (* ************************** *)
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| 48 | (* ***** Gauge groups ***** *)
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| 49 | (* ************************** *)
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| 50 | M$GaugeGroups = {
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| 51 | U1Y == {
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| 52 | Abelian -> True,
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| 53 | CouplingConstant -> g1,
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| 54 | GaugeBoson -> B,
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| 55 | Charge -> Y
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| 56 | },
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| 57 | SU2L == {
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| 58 | Abelian -> False,
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| 59 | CouplingConstant -> gw,
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| 60 | GaugeBoson -> Wi,
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| 61 | StructureConstant -> Eps,
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| 62 | Representations -> {Ta,SU2D},
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| 63 | Definitions -> {Ta[a_,b_,c_]->PauliSigma[a,b,c]/2, FSU2L[i_,j_,k_]:> I Eps[i,j,k]}
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| 64 | },
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| 65 | SU3C == {
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| 66 | Abelian -> False,
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| 67 | CouplingConstant -> gs,
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| 68 | GaugeBoson -> G,
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| 69 | StructureConstant -> f,
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| 70 | Representations -> {T,Colour},
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| 71 | SymmetricTensor -> dSUN
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| 72 | }
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| 73 | };
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| 74 |
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| 75 |
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| 76 | (* ************************** *)
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| 77 | (* ***** Indices ***** *)
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| 78 | (* ************************** *)
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| 79 |
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| 80 | IndexRange[Index[SU2W ]] = Unfold[Range[3]];
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| 81 | IndexRange[Index[SU2D ]] = Unfold[Range[2]];
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| 82 | IndexRange[Index[Gluon ]] = NoUnfold[Range[8]];
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| 83 | IndexRange[Index[Colour ]] = NoUnfold[Range[3]];
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| 84 | IndexRange[Index[Generation]] = Range[3];
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| 85 |
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| 86 | IndexStyle[SU2W, j];
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| 87 | IndexStyle[SU2D, k];
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| 88 | IndexStyle[Gluon, a];
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| 89 | IndexStyle[Colour, m];
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| 90 | IndexStyle[Generation, f];
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| 91 |
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| 92 |
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| 93 | (* ************************** *)
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| 94 | (* *** Interaction orders *** *)
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| 95 | (* *** (as used by mg5) *** *)
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| 96 | (* ************************** *)
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| 97 |
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| 98 | M$InteractionOrderHierarchy = {
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| 99 | {QCD, 1},
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| 100 | {QED, 2}
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| 101 | };
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| 102 |
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| 103 |
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| 104 | (* ************************** *)
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| 105 | (* **** Particle classes **** *)
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| 106 | (* ************************** *)
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| 107 | M$ClassesDescription = {
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| 108 |
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| 109 | (* Gauge bosons: physical vector fields *)
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| 110 | V[1] == {
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| 111 | ClassName -> A,
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| 112 | SelfConjugate -> True,
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| 113 | Mass -> 0,
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| 114 | Width -> 0,
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| 115 | ParticleName -> "A",
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| 116 | PDG -> 22,
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| 117 | PropagatorLabel -> "A",
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| 118 | PropagatorType -> W,
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| 119 | PropagatorArrow -> None,
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| 120 | FullName -> "Photon"
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| 121 | },
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| 122 | V[2] == {
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| 123 | ClassName -> Z,
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| 124 | SelfConjugate -> True,
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| 125 | Mass -> {MZ, 91.1876},
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| 126 | Width -> {WZ, 2.4952},
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| 127 | ParticleName -> "Z",
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| 128 | PDG -> 23,
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| 129 | PropagatorLabel -> "Z",
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| 130 | PropagatorType -> Sine,
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| 131 | PropagatorArrow -> None,
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| 132 | FullName -> "Z"
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| 133 | },
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| 134 | V[3] == {
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| 135 | ClassName -> W,
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| 136 | SelfConjugate -> False,
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| 137 | Mass -> {MW, Internal},
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| 138 | Width -> {WW, 2.085},
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| 139 | ParticleName -> "W+",
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| 140 | AntiParticleName -> "W-",
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| 141 | QuantumNumbers -> {Q -> 1},
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| 142 | PDG -> 24,
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| 143 | PropagatorLabel -> "W",
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| 144 | PropagatorType -> Sine,
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| 145 | PropagatorArrow -> Forward,
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| 146 | FullName -> "W"
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| 147 | },
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| 148 | V[4] == {
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| 149 | ClassName -> G,
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| 150 | SelfConjugate -> True,
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| 151 | Indices -> {Index[Gluon]},
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| 152 | Mass -> 0,
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| 153 | Width -> 0,
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| 154 | ParticleName -> "g",
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| 155 | PDG -> 21,
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| 156 | PropagatorLabel -> "G",
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| 157 | PropagatorType -> C,
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| 158 | PropagatorArrow -> None,
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| 159 | FullName -> "G"
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| 160 | },
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| 161 |
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| 162 | (* Ghosts: related to physical gauge bosons *)
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| 163 | U[1] == {
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| 164 | ClassName -> ghA,
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| 165 | SelfConjugate -> False,
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| 166 | Ghost -> A,
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| 167 | QuantumNumbers -> {GhostNumber -> 1},
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| 168 | Mass -> 0,
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| 169 | Width -> 0,
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| 170 | PropagatorLabel -> "uA",
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| 171 | PropagatorType -> GhostDash,
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| 172 | PropagatorArrow -> Forward
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| 173 | },
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| 174 | U[2] == {
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| 175 | ClassName -> ghZ,
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| 176 | SelfConjugate -> False,
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| 177 | Ghost -> Z,
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| 178 | QuantumNumbers -> {GhostNumber -> 1},
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| 179 | Mass -> {MZ,91.1876},
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| 180 | Width -> {WZ, 2.4952},
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| 181 | PropagatorLabel -> "uZ",
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| 182 | PropagatorType -> GhostDash,
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| 183 | PropagatorArrow -> Forward
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| 184 | },
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| 185 | U[31] == {
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| 186 | ClassName -> ghWp,
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| 187 | SelfConjugate -> False,
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| 188 | Ghost -> W,
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| 189 | QuantumNumbers -> {GhostNumber -> 1, Q -> 1},
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| 190 | Mass -> {MW,Internal},
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| 191 | Width -> {WW, 2.085},
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| 192 | PropagatorLabel -> "uWp",
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| 193 | PropagatorType -> GhostDash,
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| 194 | PropagatorArrow -> Forward
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| 195 | },
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| 196 | U[32] == {
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| 197 | ClassName -> ghWm,
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| 198 | SelfConjugate -> False,
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| 199 | Ghost -> Wbar,
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| 200 | QuantumNumbers -> {GhostNumber -> 1, Q -> -1},
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| 201 | Mass -> {MW,Internal},
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| 202 | Width -> {WW, 2.085},
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| 203 | PropagatorLabel -> "uWm",
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| 204 | PropagatorType -> GhostDash,
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| 205 | PropagatorArrow -> Forward
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| 206 | },
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| 207 | U[4] == {
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| 208 | ClassName -> ghG,
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| 209 | SelfConjugate -> False,
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| 210 | Indices -> {Index[Gluon]},
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| 211 | Ghost -> G,
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| 212 | PDG -> 82,
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| 213 | QuantumNumbers ->{GhostNumber -> 1},
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| 214 | Mass -> 0,
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| 215 | Width -> 0,
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| 216 | PropagatorLabel -> "uG",
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| 217 | PropagatorType -> GhostDash,
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| 218 | PropagatorArrow -> Forward
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| 219 | },
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| 220 |
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| 221 | (* Gauge bosons: unphysical vector fields *)
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| 222 | V[11] == {
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| 223 | ClassName -> B,
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| 224 | Unphysical -> True,
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| 225 | SelfConjugate -> True,
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| 226 | Definitions -> { B[mu_] -> -sw Z[mu]+cw A[mu]}
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| 227 | },
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| 228 | V[12] == {
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| 229 | ClassName -> Wi,
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| 230 | Unphysical -> True,
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| 231 | SelfConjugate -> True,
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| 232 | Indices -> {Index[SU2W]},
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| 233 | FlavorIndex -> SU2W,
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| 234 | Definitions -> { Wi[mu_,1] -> (Wbar[mu]+W[mu])/Sqrt[2], Wi[mu_,2] -> (Wbar[mu]-W[mu])/(I*Sqrt[2]), Wi[mu_,3] -> cw Z[mu] + sw A[mu]}
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| 235 | },
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| 236 |
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| 237 | (* Ghosts: related to unphysical gauge bosons *)
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| 238 | U[11] == {
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| 239 | ClassName -> ghB,
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| 240 | Unphysical -> True,
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| 241 | SelfConjugate -> False,
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| 242 | Ghost -> B,
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| 243 | Definitions -> { ghB -> -sw ghZ + cw ghA}
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| 244 | },
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| 245 | U[12] == {
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| 246 | ClassName -> ghWi,
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| 247 | Unphysical -> True,
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| 248 | SelfConjugate -> False,
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| 249 | Ghost -> Wi,
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| 250 | Indices -> {Index[SU2W]},
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| 251 | FlavorIndex -> SU2W,
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| 252 | Definitions -> { ghWi[1] -> (ghWp+ghWm)/Sqrt[2], ghWi[2] -> (ghWm-ghWp)/(I*Sqrt[2]), ghWi[3] -> cw ghZ+sw ghA}
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| 253 | } ,
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| 254 |
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| 255 | (* Fermions: physical fields *)
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| 256 | F[1] == {
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| 257 | ClassName -> vl,
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| 258 | ClassMembers -> {ve,vm,vt},
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| 259 | Indices -> {Index[Generation]},
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| 260 | FlavorIndex -> Generation,
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| 261 | SelfConjugate -> False,
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| 262 | Mass -> 0,
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| 263 | Width -> 0,
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| 264 | QuantumNumbers -> {LeptonNumber -> 1},
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| 265 | PropagatorLabel -> {"v", "ve", "vm", "vt"} ,
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| 266 | PropagatorType -> S,
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| 267 | PropagatorArrow -> Forward,
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| 268 | PDG -> {12,14,16},
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| 269 | ParticleName -> {"ve","vm","vt"},
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| 270 | AntiParticleName -> {"ve~","vm~","vt~"},
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| 271 | FullName -> {"Electron-neutrino", "Mu-neutrino", "Tau-neutrino"}
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| 272 | },
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| 273 | F[2] == {
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| 274 | ClassName -> l,
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| 275 | ClassMembers -> {e, mu, ta},
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| 276 | Indices -> {Index[Generation]},
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| 277 | FlavorIndex -> Generation,
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| 278 | SelfConjugate -> False,
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| 279 | Mass -> {Ml, {Me,5.11*^-4}, {MMU,0.10566}, {MTA,1.777}},
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| 280 | Width -> 0,
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| 281 | QuantumNumbers -> {Q -> -1, LeptonNumber -> 1},
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| 282 | PropagatorLabel -> {"l", "e", "mu", "ta"},
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| 283 | PropagatorType -> Straight,
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| 284 | PropagatorArrow -> Forward,
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| 285 | PDG -> {11, 13, 15},
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| 286 | ParticleName -> {"e-", "mu-", "ta-"},
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| 287 | AntiParticleName -> {"e+", "mu+", "ta+"},
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| 288 | FullName -> {"Electron", "Muon", "Tau"}
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| 289 | },
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| 290 | F[3] == {
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| 291 | ClassName -> uq,
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| 292 | ClassMembers -> {u, c, t},
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| 293 | Indices -> {Index[Generation], Index[Colour]},
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| 294 | FlavorIndex -> Generation,
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| 295 | SelfConjugate -> False,
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| 296 | Mass -> {Mu, {MU, 2.55*^-3}, {MC,1.27}, {MT,172}},
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| 297 | Width -> {0, 0, {WT,1.50833649}},
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| 298 | QuantumNumbers -> {Q -> 2/3},
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| 299 | PropagatorLabel -> {"uq", "u", "c", "t"},
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| 300 | PropagatorType -> Straight,
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| 301 | PropagatorArrow -> Forward,
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| 302 | PDG -> {2, 4, 6},
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| 303 | ParticleName -> {"u", "c", "t" },
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| 304 | AntiParticleName -> {"u~", "c~", "t~"},
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| 305 | FullName -> {"u-quark", "c-quark", "t-quark"}
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| 306 | },
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| 307 | F[4] == {
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| 308 | ClassName -> dq,
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| 309 | ClassMembers -> {d, s, b},
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| 310 | Indices -> {Index[Generation], Index[Colour]},
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| 311 | FlavorIndex -> Generation,
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| 312 | SelfConjugate -> False,
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| 313 | Mass -> {Md, {MD,5.04*^-3}, {MS,0.101}, {MB,4.7}},
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| 314 | Width -> 0,
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| 315 | QuantumNumbers -> {Q -> -1/3},
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| 316 | PropagatorLabel -> {"dq", "d", "s", "b"},
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| 317 | PropagatorType -> Straight,
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| 318 | PropagatorArrow -> Forward,
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| 319 | PDG -> {1,3,5},
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| 320 | ParticleName -> {"d", "s", "b" },
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| 321 | AntiParticleName -> {"d~", "s~", "b~"},
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| 322 | FullName -> {"d-quark", "s-quark", "b-quark"}
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| 323 | },
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| 324 |
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| 325 | (* Fermions: unphysical fields *)
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| 326 | F[11] == {
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| 327 | ClassName -> LL,
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| 328 | Unphysical -> True,
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| 329 | Indices -> {Index[SU2D], Index[Generation]},
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| 330 | FlavorIndex -> SU2D,
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| 331 | SelfConjugate -> False,
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| 332 | QuantumNumbers -> {Y -> -1/2},
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| 333 | Definitions -> { LL[sp1_,1,ff_] :> Module[{sp2}, ProjM[sp1,sp2] vl[sp2,ff]], LL[sp1_,2,ff_] :> Module[{sp2}, ProjM[sp1,sp2] l[sp2,ff]] }
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| 334 | },
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| 335 | F[12] == {
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| 336 | ClassName -> lR,
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| 337 | Unphysical -> True,
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| 338 | Indices -> {Index[Generation]},
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| 339 | FlavorIndex -> Generation,
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| 340 | SelfConjugate -> False,
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| 341 | QuantumNumbers -> {Y -> -1},
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| 342 | Definitions -> { lR[sp1_,ff_] :> Module[{sp2}, ProjP[sp1,sp2] l[sp2,ff]] }
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| 343 | },
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| 344 | F[13] == {
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| 345 | ClassName -> QL,
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| 346 | Unphysical -> True,
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| 347 | Indices -> {Index[SU2D], Index[Generation], Index[Colour]},
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| 348 | FlavorIndex -> SU2D,
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| 349 | SelfConjugate -> False,
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| 350 | QuantumNumbers -> {Y -> 1/6},
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| 351 | Definitions -> {
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| 352 | QL[sp1_,1,ff_,cc_] :> Module[{sp2}, ProjM[sp1,sp2] uq[sp2,ff,cc]],
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| 353 | QL[sp1_,2,ff_,cc_] :> Module[{sp2,ff2}, CKM[ff,ff2] ProjM[sp1,sp2] dq[sp2,ff2,cc]] }
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| 354 | },
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| 355 | F[14] == {
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| 356 | ClassName -> uR,
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| 357 | Unphysical -> True,
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| 358 | Indices -> {Index[Generation], Index[Colour]},
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| 359 | FlavorIndex -> Generation,
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| 360 | SelfConjugate -> False,
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| 361 | QuantumNumbers -> {Y -> 2/3},
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| 362 | Definitions -> { uR[sp1_,ff_,cc_] :> Module[{sp2}, ProjP[sp1,sp2] uq[sp2,ff,cc]] }
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| 363 | },
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| 364 | F[15] == {
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| 365 | ClassName -> dR,
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| 366 | Unphysical -> True,
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| 367 | Indices -> {Index[Generation], Index[Colour]},
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| 368 | FlavorIndex -> Generation,
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| 369 | SelfConjugate -> False,
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| 370 | QuantumNumbers -> {Y -> -1/3},
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| 371 | Definitions -> { dR[sp1_,ff_,cc_] :> Module[{sp2}, ProjP[sp1,sp2] dq[sp2,ff,cc]] }
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| 372 | },
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| 373 |
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| 374 | (* Higgs: physical scalars *)
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| 375 | S[1] == {
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| 376 | ClassName -> H,
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| 377 | SelfConjugate -> True,
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| 378 | Mass -> {MH,125},
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| 379 | Width -> {WH,0.00407},
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| 380 | PropagatorLabel -> "H",
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| 381 | PropagatorType -> D,
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| 382 | PropagatorArrow -> None,
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| 383 | PDG -> 25,
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| 384 | ParticleName -> "H",
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| 385 | FullName -> "H"
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| 386 | },
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| 387 |
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| 388 | (* Higgs: physical scalars *)
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| 389 | S[2] == {
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| 390 | ClassName -> G0,
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| 391 | SelfConjugate -> True,
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| 392 | Goldstone -> Z,
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| 393 | Mass -> {MZ, 91.1876},
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| 394 | Width -> {WZ, 2.4952},
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| 395 | PropagatorLabel -> "Go",
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| 396 | PropagatorType -> D,
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| 397 | PropagatorArrow -> None,
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| 398 | PDG -> 250,
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| 399 | ParticleName -> "G0",
|
|---|
| 400 | FullName -> "G0"
|
|---|
| 401 | },
|
|---|
| 402 | S[3] == {
|
|---|
| 403 | ClassName -> GP,
|
|---|
| 404 | SelfConjugate -> False,
|
|---|
| 405 | Goldstone -> W,
|
|---|
| 406 | Mass -> {MW, Internal},
|
|---|
| 407 | QuantumNumbers -> {Q -> 1},
|
|---|
| 408 | Width -> {WW, 2.085},
|
|---|
| 409 | PropagatorLabel -> "GP",
|
|---|
| 410 | PropagatorType -> D,
|
|---|
| 411 | PropagatorArrow -> None,
|
|---|
| 412 | PDG -> 251,
|
|---|
| 413 | ParticleName -> "G+",
|
|---|
| 414 | AntiParticleName -> "G-",
|
|---|
| 415 | FullName -> "GP"
|
|---|
| 416 | },
|
|---|
| 417 |
|
|---|
| 418 | (* Higgs: unphysical scalars *)
|
|---|
| 419 | S[11] == {
|
|---|
| 420 | ClassName -> Phi,
|
|---|
| 421 | Unphysical -> True,
|
|---|
| 422 | Indices -> {Index[SU2D]},
|
|---|
| 423 | FlavorIndex -> SU2D,
|
|---|
| 424 | SelfConjugate -> False,
|
|---|
| 425 | QuantumNumbers -> {Y -> 1/2},
|
|---|
| 426 | Definitions -> { Phi[1] -> -I GP, Phi[2] -> (vev + H + I G0)/Sqrt[2] }
|
|---|
| 427 | },
|
|---|
| 428 | (******************************* Spin 2 particles: graviton *****************************)
|
|---|
| 429 |
|
|---|
| 430 | T[1] == {
|
|---|
| 431 | ClassName -> h,
|
|---|
| 432 | SelfConjugate -> True,
|
|---|
| 433 | Symmetric -> True,
|
|---|
| 434 | Mass -> {Mh, 500},
|
|---|
| 435 | Width -> {Wh, 10.},
|
|---|
| 436 | PropagatorLabel -> "h",
|
|---|
| 437 | PropagatorType -> GhostDash,
|
|---|
| 438 | PropagatorArrow -> None,
|
|---|
| 439 | PDG -> 5000002,
|
|---|
| 440 | TeX -> h,
|
|---|
| 441 | FullName -> "Graviton" }
|
|---|
| 442 | };
|
|---|
| 443 |
|
|---|
| 444 |
|
|---|
| 445 |
|
|---|
| 446 |
|
|---|
| 447 | (* ************************** *)
|
|---|
| 448 | (* ***** Gauge ***** *)
|
|---|
| 449 | (* ***** Parameters ***** *)
|
|---|
| 450 | (* ***** (FeynArts) ***** *)
|
|---|
| 451 | (* ************************** *)
|
|---|
| 452 |
|
|---|
| 453 | GaugeXi[ V[1] ] = GaugeXi[A];
|
|---|
| 454 | GaugeXi[ V[2] ] = GaugeXi[Z];
|
|---|
| 455 | GaugeXi[ V[3] ] = GaugeXi[W];
|
|---|
| 456 | GaugeXi[ V[4] ] = GaugeXi[G];
|
|---|
| 457 | GaugeXi[ S[1] ] = 1;
|
|---|
| 458 | GaugeXi[ S[2] ] = GaugeXi[Z];
|
|---|
| 459 | GaugeXi[ S[3] ] = GaugeXi[W];
|
|---|
| 460 | GaugeXi[ U[1] ] = GaugeXi[A];
|
|---|
| 461 | GaugeXi[ U[2] ] = GaugeXi[Z];
|
|---|
| 462 | GaugeXi[ U[31] ] = GaugeXi[W];
|
|---|
| 463 | GaugeXi[ U[32] ] = GaugeXi[W];
|
|---|
| 464 | GaugeXi[ U[4] ] = GaugeXi[G];
|
|---|
| 465 |
|
|---|
| 466 |
|
|---|
| 467 | (* ************************** *)
|
|---|
| 468 | (* ***** Parameters ***** *)
|
|---|
| 469 | (* ************************** *)
|
|---|
| 470 | M$Parameters = {
|
|---|
| 471 |
|
|---|
| 472 | (* External parameters *)
|
|---|
| 473 | aEWM1 == {
|
|---|
| 474 | ParameterType -> External,
|
|---|
| 475 | BlockName -> SMINPUTS,
|
|---|
| 476 | OrderBlock -> 1,
|
|---|
| 477 | Value -> 127.9,
|
|---|
| 478 | InteractionOrder -> {QED,-2},
|
|---|
| 479 | Description -> "Inverse of the EW coupling constant at the Z pole"
|
|---|
| 480 | },
|
|---|
| 481 | Gf == {
|
|---|
| 482 | ParameterType -> External,
|
|---|
| 483 | BlockName -> SMINPUTS,
|
|---|
| 484 | OrderBlock -> 2,
|
|---|
| 485 | Value -> 1.16637*^-5,
|
|---|
| 486 | InteractionOrder -> {QED,2},
|
|---|
| 487 | TeX -> Subscript[G,f],
|
|---|
| 488 | Description -> "Fermi constant"
|
|---|
| 489 | },
|
|---|
| 490 | aS == {
|
|---|
| 491 | ParameterType -> External,
|
|---|
| 492 | BlockName -> SMINPUTS,
|
|---|
| 493 | OrderBlock -> 3,
|
|---|
| 494 | Value -> 0.1184,
|
|---|
| 495 | InteractionOrder -> {QCD,2},
|
|---|
| 496 | TeX -> Subscript[\[Alpha],s],
|
|---|
| 497 | Description -> "Strong coupling constant at the Z pole"
|
|---|
| 498 | },
|
|---|
| 499 | ymdo == {
|
|---|
| 500 | ParameterType -> External,
|
|---|
| 501 | BlockName -> YUKAWA,
|
|---|
| 502 | OrderBlock -> 1,
|
|---|
| 503 | Value -> 5.04*^-3,
|
|---|
| 504 | Description -> "Down Yukawa mass"
|
|---|
| 505 | },
|
|---|
| 506 | ymup == {
|
|---|
| 507 | ParameterType -> External,
|
|---|
| 508 | BlockName -> YUKAWA,
|
|---|
| 509 | OrderBlock -> 2,
|
|---|
| 510 | Value -> 2.55*^-3,
|
|---|
| 511 | Description -> "Up Yukawa mass"
|
|---|
| 512 | },
|
|---|
| 513 | yms == {
|
|---|
| 514 | ParameterType -> External,
|
|---|
| 515 | BlockName -> YUKAWA,
|
|---|
| 516 | OrderBlock -> 3,
|
|---|
| 517 | Value -> 0.101,
|
|---|
| 518 | Description -> "Strange Yukawa mass"
|
|---|
| 519 | },
|
|---|
| 520 | ymc == {
|
|---|
| 521 | ParameterType -> External,
|
|---|
| 522 | BlockName -> YUKAWA,
|
|---|
| 523 | OrderBlock -> 4,
|
|---|
| 524 | Value -> 1.27,
|
|---|
| 525 | Description -> "Charm Yukawa mass"
|
|---|
| 526 | },
|
|---|
| 527 | ymb == {
|
|---|
| 528 | ParameterType -> External,
|
|---|
| 529 | BlockName -> YUKAWA,
|
|---|
| 530 | OrderBlock -> 5,
|
|---|
| 531 | Value -> 4.7,
|
|---|
| 532 | Description -> "Bottom Yukawa mass"
|
|---|
| 533 | },
|
|---|
| 534 | ymt == {
|
|---|
| 535 | ParameterType -> External,
|
|---|
| 536 | BlockName -> YUKAWA,
|
|---|
| 537 | OrderBlock -> 6,
|
|---|
| 538 | Value -> 172,
|
|---|
| 539 | Description -> "Top Yukawa mass"
|
|---|
| 540 | },
|
|---|
| 541 | yme == {
|
|---|
| 542 | ParameterType -> External,
|
|---|
| 543 | BlockName -> YUKAWA,
|
|---|
| 544 | OrderBlock -> 11,
|
|---|
| 545 | Value -> 5.11*^-4,
|
|---|
| 546 | Description -> "Electron Yukawa mass"
|
|---|
| 547 | },
|
|---|
| 548 | ymm == {
|
|---|
| 549 | ParameterType -> External,
|
|---|
| 550 | BlockName -> YUKAWA,
|
|---|
| 551 | OrderBlock -> 13,
|
|---|
| 552 | Value -> 0.10566,
|
|---|
| 553 | Description -> "Muon Yukawa mass"
|
|---|
| 554 | },
|
|---|
| 555 | ymtau == {
|
|---|
| 556 | ParameterType -> External,
|
|---|
| 557 | BlockName -> YUKAWA,
|
|---|
| 558 | OrderBlock -> 15,
|
|---|
| 559 | Value -> 1.777,
|
|---|
| 560 | Description -> "Tau Yukawa mass"
|
|---|
| 561 | },
|
|---|
| 562 | cabi == {
|
|---|
| 563 | ParameterType -> External,
|
|---|
| 564 | BlockName -> CKMBLOCK,
|
|---|
| 565 | OrderBlock -> 1,
|
|---|
| 566 | Value -> 0.227736,
|
|---|
| 567 | TeX -> Subscript[\[Theta], c],
|
|---|
| 568 | Description -> "Cabibbo angle"
|
|---|
| 569 | },
|
|---|
| 570 |
|
|---|
| 571 | GN == {
|
|---|
| 572 | ParameterType -> External,
|
|---|
| 573 | ParameterName -> GN,
|
|---|
| 574 | InteractionOrder -> {QCD, 2},
|
|---|
| 575 | Value -> 10^(-16),
|
|---|
| 576 | Description -> "Newton Constant"},
|
|---|
| 577 |
|
|---|
| 578 | (* Internal Parameters *)
|
|---|
| 579 | aEW == {
|
|---|
| 580 | ParameterType -> Internal,
|
|---|
| 581 | Value -> 1/aEWM1,
|
|---|
| 582 | InteractionOrder -> {QED,2},
|
|---|
| 583 | TeX -> Subscript[\[Alpha], EW],
|
|---|
| 584 | Description -> "Electroweak coupling contant"
|
|---|
| 585 | },
|
|---|
| 586 | MW == {
|
|---|
| 587 | ParameterType -> Internal,
|
|---|
| 588 | Value -> Sqrt[MZ^2/2+Sqrt[MZ^4/4-Pi/Sqrt[2]*aEW/Gf*MZ^2]],
|
|---|
| 589 | TeX -> Subscript[M,W],
|
|---|
| 590 | Description -> "W mass"
|
|---|
| 591 | },
|
|---|
| 592 | sw2 == {
|
|---|
| 593 | ParameterType -> Internal,
|
|---|
| 594 | Value -> 1-(MW/MZ)^2,
|
|---|
| 595 | Description -> "Squared Sin of the Weinberg angle"
|
|---|
| 596 | },
|
|---|
| 597 | ee == {
|
|---|
| 598 | ParameterType -> Internal,
|
|---|
| 599 | Value -> Sqrt[4 Pi aEW],
|
|---|
| 600 | InteractionOrder -> {QED,1},
|
|---|
| 601 | TeX -> e,
|
|---|
| 602 | Description -> "Electric coupling constant"
|
|---|
| 603 | },
|
|---|
| 604 | cw == {
|
|---|
| 605 | ParameterType -> Internal,
|
|---|
| 606 | Value -> Sqrt[1-sw2],
|
|---|
| 607 | TeX -> Subscript[c,w],
|
|---|
| 608 | Description -> "Cosine of the Weinberg angle"
|
|---|
| 609 | },
|
|---|
| 610 | sw == {
|
|---|
| 611 | ParameterType -> Internal,
|
|---|
| 612 | Value -> Sqrt[sw2],
|
|---|
| 613 | TeX -> Subscript[s,w],
|
|---|
| 614 | Description -> "Sine of the Weinberg angle"
|
|---|
| 615 | },
|
|---|
| 616 | gw == {
|
|---|
| 617 | ParameterType -> Internal,
|
|---|
| 618 | Definitions -> {gw->ee/sw},
|
|---|
| 619 | InteractionOrder -> {QED,1},
|
|---|
| 620 | TeX -> Subscript[g,w],
|
|---|
| 621 | Description -> "Weak coupling constant at the Z pole"
|
|---|
| 622 | },
|
|---|
| 623 | g1 == {
|
|---|
| 624 | ParameterType -> Internal,
|
|---|
| 625 | Definitions -> {g1->ee/cw},
|
|---|
| 626 | InteractionOrder -> {QED,1},
|
|---|
| 627 | TeX -> Subscript[g,1],
|
|---|
| 628 | Description -> "U(1)Y coupling constant at the Z pole"
|
|---|
| 629 | },
|
|---|
| 630 | gs == {
|
|---|
| 631 | ParameterType -> Internal,
|
|---|
| 632 | Value -> Sqrt[4 Pi aS],
|
|---|
| 633 | InteractionOrder -> {QCD,1},
|
|---|
| 634 | TeX -> Subscript[g,s],
|
|---|
| 635 | ParameterName -> G,
|
|---|
| 636 | Description -> "Strong coupling constant at the Z pole"
|
|---|
| 637 | },
|
|---|
| 638 | vev == {
|
|---|
| 639 | ParameterType -> Internal,
|
|---|
| 640 | Value -> 2*MW*sw/ee,
|
|---|
| 641 | InteractionOrder -> {QED,-1},
|
|---|
| 642 | Description -> "Higgs vacuum expectation value"
|
|---|
| 643 | },
|
|---|
| 644 | lam == {
|
|---|
| 645 | ParameterType -> Internal,
|
|---|
| 646 | Value -> MH^2/(2*vev^2),
|
|---|
| 647 | InteractionOrder -> {QED, 2},
|
|---|
| 648 | Description -> "Higgs quartic coupling"
|
|---|
| 649 | },
|
|---|
| 650 | muH == {
|
|---|
| 651 | ParameterType -> Internal,
|
|---|
| 652 | Value -> Sqrt[vev^2 lam],
|
|---|
| 653 | TeX -> \[Mu],
|
|---|
| 654 | Description -> "Coefficient of the quadratic piece of the Higgs potential"
|
|---|
| 655 | },
|
|---|
| 656 | yl == {
|
|---|
| 657 | ParameterType -> Internal,
|
|---|
| 658 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 659 | Definitions -> {yl[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 660 | Value -> {yl[1,1] -> Sqrt[2] yme / vev, yl[2,2] -> Sqrt[2] ymm / vev, yl[3,3] -> Sqrt[2] ymtau / vev},
|
|---|
| 661 | InteractionOrder -> {QED, 1},
|
|---|
| 662 | ParameterName -> {yl[1,1] -> ye, yl[2,2] -> ym, yl[3,3] -> ytau},
|
|---|
| 663 | TeX -> Superscript[y, l],
|
|---|
| 664 | Description -> "Lepton Yukawa couplings"
|
|---|
| 665 | },
|
|---|
| 666 | yu == {
|
|---|
| 667 | ParameterType -> Internal,
|
|---|
| 668 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 669 | Definitions -> {yu[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 670 | Value -> {yu[1,1] -> Sqrt[2] ymup/vev, yu[2,2] -> Sqrt[2] ymc/vev, yu[3,3] -> Sqrt[2] ymt/vev},
|
|---|
| 671 | InteractionOrder -> {QED, 1},
|
|---|
| 672 | ParameterName -> {yu[1,1] -> yup, yu[2,2] -> yc, yu[3,3] -> yt},
|
|---|
| 673 | TeX -> Superscript[y, u],
|
|---|
| 674 | Description -> "Up-type Yukawa couplings"
|
|---|
| 675 | },
|
|---|
| 676 | yd == {
|
|---|
| 677 | ParameterType -> Internal,
|
|---|
| 678 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 679 | Definitions -> {yd[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 680 | Value -> {yd[1,1] -> Sqrt[2] ymdo/vev, yd[2,2] -> Sqrt[2] yms/vev, yd[3,3] -> Sqrt[2] ymb/vev},
|
|---|
| 681 | InteractionOrder -> {QED, 1},
|
|---|
| 682 | ParameterName -> {yd[1,1] -> ydo, yd[2,2] -> ys, yd[3,3] -> yb},
|
|---|
| 683 | TeX -> Superscript[y, d],
|
|---|
| 684 | Description -> "Down-type Yukawa couplings"
|
|---|
| 685 | },
|
|---|
| 686 | (* N. B. : only Cabibbo mixing! *)
|
|---|
| 687 | CKM == {
|
|---|
| 688 | ParameterType -> Internal,
|
|---|
| 689 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 690 | Unitary -> True,
|
|---|
| 691 | Value -> {CKM[1,1] -> Cos[cabi], CKM[1,2] -> Sin[cabi], CKM[1,3] -> 0,
|
|---|
| 692 | CKM[2,1] -> -Sin[cabi], CKM[2,2] -> Cos[cabi], CKM[2,3] -> 0,
|
|---|
| 693 | CKM[3,1] -> 0, CKM[3,2] -> 0, CKM[3,3] -> 1},
|
|---|
| 694 | TeX -> Superscript[V,CKM],
|
|---|
| 695 | Description -> "CKM-Matrix"},
|
|---|
| 696 |
|
|---|
| 697 | (******************************* Spin 2 particles: graviton *****************************)
|
|---|
| 698 |
|
|---|
| 699 | kappa == {
|
|---|
| 700 | TeX -> \[Kappa],
|
|---|
| 701 | ParameterType -> Internal,
|
|---|
| 702 | Value -> Sqrt[16 Pi GN]}
|
|---|
| 703 | };
|
|---|
| 704 |
|
|---|
| 705 |
|
|---|
| 706 | (************************************************************************************************)
|
|---|
| 707 | (******************* 2 Gravitons coupled to SM Lagrangian ************************)
|
|---|
| 708 | (************************************************************************************************)
|
|---|
| 709 | SqrtdetG := Block[{muS,nuS},
|
|---|
| 710 | ExpandIndices[1 + kappa/2 h[muS,muS] - kappa^2/4 h[muS, nuS] h[muS, nuS] + kappa^2/8 h[muS, muS] h[nuS, nuS]]];
|
|---|
| 711 |
|
|---|
| 712 | G[mu_,nu_,rho_] := Block[{mu,nu,rho},
|
|---|
| 713 | ExpandIndices[ME[mu,nu] - kappa h[mu,nu] + kappa^2 h[mu,rho]h[rho,nu]]];
|
|---|
| 714 |
|
|---|
| 715 | Sigma[mu_,nu_] := Block[{mu,nu}, ExpandIndices[ I/2 (Ga[mu].Ga[nu] - Ga[nu].Ga[mu])]];
|
|---|
| 716 |
|
|---|
| 717 | Vielbein[a_, mu_, lambda_] := Block[{a, mu,lambda},
|
|---|
| 718 | ExpandIndices[ME[a, mu] - kappa/2 h[a, mu] + 3/8 kappa^2 h[a, lambda] h[lambda, mu]]];
|
|---|
| 719 |
|
|---|
| 720 | Lambda[mu_,a_,b_,lambda_,beta_] := Block[{a,b,mu,lambda,beta},
|
|---|
| 721 | ExpandIndices[Normal[Series[I/8 kappa Sigma[a,b](del[h[b,mu],a]-del[h[a,mu],b])-I/16 kappa^2 Sigma[a,b](h[b,lambda](del[h[lambda,a],mu]+del[h[lambda,mu],a]-del[h[mu,a],lambda])+h[a,beta](del[h[b,mu],beta]-del[h[mu,beta],b])),{kappa,0,2}]]]] ;
|
|---|
| 722 |
|
|---|
| 723 | LGGauge := Block[{mu, nu, alpha, beta, ii, aa, itn1, itn2},
|
|---|
| 724 | ExpandIndices[SqrtdetG * (-1/4 G[mu, nu, itn1] G[alpha, beta, itn2] FS[B, mu, alpha] FS[B, nu, beta] - 1/4 G[mu, nu, itn1] G[alpha, beta, itn2] FS[Wi, mu, alpha, ii] FS[Wi, nu, beta, ii] - 1/4 G[mu, nu, itn1] G[alpha, beta, itn2] FS[G, mu, alpha, aa] FS[G, nu, beta, aa]), FlavorExpand -> SU2W]];
|
|---|
| 725 |
|
|---|
| 726 | LGFermions := Block[{mu,a,b,c,alpha,beta,lambda,LGFermionsLL1,LGFermionsLL2,LGFermionslR1,LGFermionslR2},
|
|---|
| 727 | LGFermionsLL1 = ExpandIndices[I * SqrtdetG * LLbar.Ga[a].Vielbein[a,mu,alpha].DC[LL, mu], FlavorExpand->{SU2W,SU2D}];
|
|---|
| 728 | LGFermionsLL2 = ExpandIndices[I * SqrtdetG * LLbar.Ga[a].Vielbein[a,mu,alpha].Lambda[mu,b,c,lambda,beta].LL, FlavorExpand->{SU2W,SU2D}];
|
|---|
| 729 | LGFermionslR1 = ExpandIndices[I * SqrtdetG * lRbar.Ga[a].Vielbein[a,mu,alpha].DC[lR, mu], FlavorExpand->{SU2W,SU2D}];
|
|---|
| 730 | LGFermionslR2 = ExpandIndices[I * SqrtdetG * lRbar.Ga[a].Vielbein[a,mu,alpha].Lambda[mu,b,c,lambda,beta].lR, FlavorExpand->{SU2W,SU2D}];
|
|---|
| 731 | LGFermionsQL1 = ExpandIndices[I * SqrtdetG * QLbar.Ga[a].Vielbein[a,mu,alpha].DC[QL, mu], FlavorExpand->{SU2W,SU2D}]/.{CKM[a_,b_] Conjugate[CKM[a_,c_]]->IndexDelta[b,c], CKM[b_,a_] Conjugate[CKM[c_,a_]]->IndexDelta[b,c]};
|
|---|
| 732 | LGFermionsQL2 = ExpandIndices[I * SqrtdetG * QLbar.Ga[a].Vielbein[a,mu,alpha].Lambda[mu,b,c,lambda,beta].QL, FlavorExpand->{SU2W,SU2D}]/.{CKM[a_,b_] Conjugate[CKM[a_,c_]]->IndexDelta[b,c], CKM[b_,a_] Conjugate[CKM[c_,a_]]->IndexDelta[b,c]};
|
|---|
| 733 | LGFermionsuR1 = ExpandIndices[I * SqrtdetG * uRbar.Ga[a].Vielbein[a,mu,alpha].DC[uR, mu], FlavorExpand->{SU2W,SU2D}]/.{CKM[a_,b_] Conjugate[CKM[a_,c_]]->IndexDelta[b,c], CKM[b_,a_] Conjugate[CKM[c_,a_]]->IndexDelta[b,c]};
|
|---|
| 734 | LGFermionsuR2 = ExpandIndices[I * SqrtdetG * uRbar.Ga[a].Vielbein[a,mu,alpha].Lambda[mu,b,c,lambda,beta].uR, FlavorExpand->{SU2W,SU2D}]/.{CKM[a_,b_] Conjugate[CKM[a_,c_]]->IndexDelta[b,c], CKM[b_,a_] Conjugate[CKM[c_,a_]]->IndexDelta[b,c]};
|
|---|
| 735 | LGFermionsdR1 = ExpandIndices[I * SqrtdetG * dRbar.Ga[a].Vielbein[a,mu,alpha].DC[dR, mu], FlavorExpand->{SU2W,SU2D}]/.{CKM[a_,b_] Conjugate[CKM[a_,c_]]->IndexDelta[b,c], CKM[b_,a_] Conjugate[CKM[c_,a_]]->IndexDelta[b,c]};
|
|---|
| 736 | LGFermionsdR2 = ExpandIndices[I * SqrtdetG * dRbar.Ga[a].Vielbein[a,mu,alpha].Lambda[mu,b,c,lambda,beta].dR, FlavorExpand->{SU2W,SU2D}]/.{CKM[a_,b_] Conjugate[CKM[a_,c_]]->IndexDelta[b,c], CKM[b_,a_] Conjugate[CKM[c_,a_]]->IndexDelta[b,c]};
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| 737 | LGFermionsLL1 + LGFermionsLL2 + LGFermionslR1 + LGFermionslR2 + LGFermionsQL1 + LGFermionsQL2 + LGFermionsuR1 + LGFermionsuR2 + LGFermionsdR1 + LGFermionsdR2];
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| 738 |
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| 739 | LGHiggs := Block[{ii,mu,nu,rho,feynmangaugerules},
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| 740 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar ->0}, {}];
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| 741 |
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| 742 | ExpandIndices[SqrtdetG * (G[mu,nu,rho] DC[Phibar[ii],mu] DC[Phi[ii],nu] + muH^2 Phibar[ii] Phi[ii] - lam Phibar[ii] Phi[ii] Phibar[jj] Phi[jj]), FlavorExpand->{SU2D,SU2W}]/.feynmangaugerules
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| 743 | ];
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| 744 |
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| 745 | LGYukawa := Block[{sp,ii,jj,cc,ff1,ff2,ff3,yuk,feynmangaugerules},
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| 746 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar ->0}, {}];
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| 747 |
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| 748 | yuk = ExpandIndices[
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| 749 | SqrtdetG * (-yd[ff2, ff3] CKM[ff1, ff2] QLbar[sp, ii, ff1, cc].dR [sp, ff3, cc] Phi[ii] -
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| 750 | yl[ff1, ff3] LLbar[sp, ii, ff1].lR [sp, ff3] Phi[ii] -
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| 751 | yu[ff1, ff2] QLbar[sp, ii, ff1, cc].uR [sp, ff2, cc] Phibar[jj] Eps[ii, jj]), FlavorExpand -> SU2D];
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| 752 | yuk = yuk /. { CKM[a_, b_] Conjugate[CKM[a_, c_]] -> IndexDelta[b, c], CKM[b_, a_] Conjugate[CKM[c_, a_]] -> IndexDelta[b, c]};
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| 753 | SqrtdetG *(yuk+HC[yuk])/.feynmangaugerules
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| 754 | ];
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| 755 |
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| 756 | LGGhost := Block[{LGh1,LGhw,LGhs,LGhphi,mu,nu,rho,generators,gh,ghbar,Vectorize,phi1,phi2,togoldstones,doublet,doublet0},
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| 757 | (* Pure gauge piece *)
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| 758 | LGh1 = -ghBbar.G[mu,nu,rho].del[DC[ghB,mu],nu];
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| 759 | LGhw = -ghWibar[ii].G[mu,nu,rho].del[DC[ghWi[ii],mu],nu];
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| 760 | LGhs = -ghGbar[ii].G[mu,nu,rho].del[DC[ghG[ii],mu],nu];
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| 761 |
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| 762 | (* Scalar pieces: see Peskin pages 739-742 *)
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| 763 | (* phi1 and phi2 are the real degrees of freedom of GP *)
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| 764 | (* Vectorize transforms a doublet in a vector in the phi-basis, i.e. the basis of real degrees of freedom *)
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| 765 | gh = {ghB, ghWi[1], ghWi[2], ghWi[3]};
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| 766 | ghbar = {ghBbar, ghWibar[1], ghWibar[2], ghWibar[3]};
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| 767 | generators = {-I/2 g1 IdentityMatrix[2], -I/2 gw PauliSigma[1], -I/2 gw PauliSigma[2], -I/2 gw PauliSigma[3]};
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| 768 | doublet = Expand[{(-I phi1 - phi2)/Sqrt[2], Phi[2]} /. MR$Definitions /. vev -> 0];
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| 769 | doublet0 = {0, vev/Sqrt[2]};
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| 770 | Vectorize[{a_, b_}]:= Simplify[{Sqrt[2] Re[Expand[a]], Sqrt[2] Im[Expand[a]], Sqrt[2] Re[Expand[b]], Sqrt[2] Im[Expand[b]]}/.{Im[_]->0, Re[num_]->num}];
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| 771 | togoldstones := {phi1 -> (GP + GPbar)/Sqrt[2], phi2 -> (-GP + GPbar)/(I Sqrt[2])};
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| 772 | LGhphi=Plus@@Flatten[Table[-ghbar[[kkk]].gh[[lll]] Vectorize[generators[[kkk]].doublet0].Vectorize[generators[[lll]].(doublet+doublet0)],{kkk,4},{lll,4}]] /.togoldstones;
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| 773 |
|
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| 774 | ExpandIndices[SqrtdetG * LGhs + If[FeynmanGauge, SqrtdetG * (LGh1 + LGhw + LGhphi),0], FlavorExpand->SU2W]];
|
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| 775 |
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| 776 | LGGaugeO2:= Normal[Series[LGGauge,{kappa,0,2}]];
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| 777 | LGFermionsO2:= Normal[Series[LGFermions,{kappa,0,2}]];
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| 778 | LGHiggsO2:= Normal[Series[LGHiggs,{kappa,0,2}]];
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| 779 | LGYukawaO2:= Normal[Series[LGYukawa,{kappa,0,2}]];
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| 780 | LGGhostO2:= Normal[Series[LGGhost,{kappa,0,2}]];
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| 781 |
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| 782 | LGTotal:= LGGaugeO2 + LGFermionsO2 + LGHiggsO2 + LGYukawaO2 + LGGhostO2;
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