| 1 | (* ************************** *)
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| 2 | (* ***** Information ***** *)
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| 3 | (* ************************** *)
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| 4 | M$ModelName = "SM4LQ_MFV";
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| 5 |
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| 6 | M$Information = {
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| 7 | Authors -> {"M.Maltoni"},
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| 8 | Institutions -> {"CP3 (UCLouvain)"},
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| 9 | Emails -> {"matteo.maltoni@uclouvain.be"}
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| 10 | };
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| 11 |
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| 12 | FeynmanGauge = True;
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| 13 |
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| 14 | (* ************************** *)
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| 15 | (* ***** NLO Variables ****** *)
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| 16 | (******************************)
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| 17 |
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| 18 | FR$LoopSwitches = {{Gf, MW}};
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| 19 | FR$RmDblExt = { ymb -> MB, ymc -> MC, ymdo -> MD, yme -> Me,
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| 20 | ymm -> MMU, yms -> MS, ymt -> MT, ymtau -> MTA, ymup -> MU};
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| 21 |
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| 22 | (* ************************** *)
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| 23 | (* ***** vevs ***** *)
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| 24 | (* ************************** *)
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| 25 | M$vevs = { {Phi[2],vev} };
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| 26 |
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| 27 | (* ************************** *)
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| 28 | (* ***** Gauge groups ***** *)
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| 29 | (* ************************** *)
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| 30 | M$GaugeGroups = {
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| 31 | U1Y == {
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| 32 | Abelian -> True,
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| 33 | CouplingConstant -> g1,
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| 34 | GaugeBoson -> B,
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| 35 | Charge -> Y
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| 36 | },
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| 37 | SU2L == {
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| 38 | Abelian -> False,
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| 39 | CouplingConstant -> gw,
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| 40 | GaugeBoson -> Wi,
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| 41 | StructureConstant -> Eps,
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| 42 | Representations -> {Ta,SU2D},
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| 43 | Definitions -> {Ta[a_,b_,c_]->PauliSigma[a,b,c]/2, FSU2L[i_,j_,k_]:> I Eps[i,j,k]}
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| 44 | },
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| 45 | SU3C == {
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| 46 | Abelian -> False,
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| 47 | CouplingConstant -> gs,
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| 48 | GaugeBoson -> G,
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| 49 | StructureConstant -> f,
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| 50 | Representations -> {T,Colour},
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| 51 | SymmetricTensor -> dSUN
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| 52 | }
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| 53 | };
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| 54 |
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| 55 | (* ************************** *)
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| 56 | (* ***** Indices ***** *)
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| 57 | (* ************************** *)
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| 58 |
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| 59 | IndexRange[Index[SU2W ]] = Unfold[Range[3]];
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| 60 | IndexRange[Index[SU2D ]] = Unfold[Range[2]];
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| 61 | IndexRange[Index[Gluon ]] = NoUnfold[Range[8]];
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| 62 | IndexRange[Index[Colour ]] = NoUnfold[Range[3]];
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| 63 | IndexRange[Index[Generation]] = Range[3];
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| 64 |
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| 65 | IndexStyle[SU2W, j];
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| 66 | IndexStyle[SU2D, k];
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| 67 | IndexStyle[Gluon, a];
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| 68 | IndexStyle[Colour, m];
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| 69 | IndexStyle[Generation, f];
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| 70 |
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| 71 | (* ************************** *)
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| 72 | (* *** Interaction orders *** *)
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| 73 | (* *** (as used by mg5) *** *)
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| 74 | (* ************************** *)
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| 75 |
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| 76 | M$InteractionOrderHierarchy = {
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| 77 | {QCD,2},
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| 78 | {QED,4},
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| 79 | {NP,1}
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| 80 | };
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| 81 |
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| 82 | M$InteractionOrderLimit = {
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| 83 | {NP,2}
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| 84 | };
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| 85 |
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| 86 | (* ************************** *)
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| 87 | (* **** Particle classes **** *)
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| 88 | (* ************************** *)
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| 89 | M$ClassesDescription = {
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| 90 |
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| 91 | (* Gauge bosons: physical vector fields *)
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| 92 | V[1] == {
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| 93 | ClassName -> A,
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| 94 | SelfConjugate -> True,
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| 95 | Mass -> 0,
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| 96 | Width -> 0,
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| 97 | ParticleName -> "a",
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| 98 | PDG -> 22,
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| 99 | PropagatorLabel -> "a",
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| 100 | PropagatorType -> W,
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| 101 | PropagatorArrow -> None,
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| 102 | FullName -> "Photon"
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| 103 | },
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| 104 | V[2] == {
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| 105 | ClassName -> Z,
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| 106 | SelfConjugate -> True,
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| 107 | Mass -> {MZ, 91.1876},
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| 108 | Width -> {WZ, 2.4952},
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| 109 | ParticleName -> "Z",
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| 110 | PDG -> 23,
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| 111 | PropagatorLabel -> "Z",
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| 112 | PropagatorType -> Sine,
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| 113 | PropagatorArrow -> None,
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| 114 | FullName -> "Z"
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| 115 | },
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| 116 | V[3] == {
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| 117 | ClassName -> W,
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| 118 | SelfConjugate -> False,
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| 119 | Mass -> {MW, Internal},
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| 120 | Width -> {WW, 2.085},
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| 121 | ParticleName -> "W+",
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| 122 | AntiParticleName -> "W-",
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| 123 | QuantumNumbers -> {Q -> 1},
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| 124 | PDG -> 24,
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| 125 | PropagatorLabel -> "W",
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| 126 | PropagatorType -> Sine,
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| 127 | PropagatorArrow -> Forward,
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| 128 | FullName -> "W"
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| 129 | },
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| 130 | V[4] == {
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| 131 | ClassName -> G,
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| 132 | SelfConjugate -> True,
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| 133 | Indices -> {Index[Gluon]},
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| 134 | Mass -> 0,
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| 135 | Width -> 0,
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| 136 | ParticleName -> "g",
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| 137 | PDG -> 21,
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| 138 | PropagatorLabel -> "G",
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| 139 | PropagatorType -> C,
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| 140 | PropagatorArrow -> None,
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| 141 | FullName -> "G"
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| 142 | },
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| 143 |
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| 144 | (* Ghosts: related to physical gauge bosons *)
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| 145 | U[1] == {
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| 146 | ClassName -> ghA,
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| 147 | SelfConjugate -> False,
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| 148 | Ghost -> A,
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| 149 | QuantumNumbers -> {GhostNumber -> 1},
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| 150 | Mass -> 0,
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| 151 | Width -> 0,
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| 152 | PropagatorLabel -> "uA",
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| 153 | PropagatorType -> GhostDash,
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| 154 | PropagatorArrow -> Forward
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| 155 | },
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| 156 | U[2] == {
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| 157 | ClassName -> ghZ,
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| 158 | SelfConjugate -> False,
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| 159 | Ghost -> Z,
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| 160 | QuantumNumbers -> {GhostNumber -> 1},
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| 161 | Mass -> {MZ,91.1876},
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| 162 | Width -> {WZ, 2.4952},
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| 163 | PropagatorLabel -> "uZ",
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| 164 | PropagatorType -> GhostDash,
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| 165 | PropagatorArrow -> Forward
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| 166 | },
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| 167 | U[31] == {
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| 168 | ClassName -> ghWp,
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| 169 | SelfConjugate -> False,
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| 170 | Ghost -> W,
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| 171 | QuantumNumbers -> {GhostNumber -> 1, Q -> 1},
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| 172 | Mass -> {MW,Internal},
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| 173 | Width -> {WW, 2.085},
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| 174 | PropagatorLabel -> "uWp",
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| 175 | PropagatorType -> GhostDash,
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| 176 | PropagatorArrow -> Forward
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| 177 | },
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| 178 | U[32] == {
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| 179 | ClassName -> ghWm,
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| 180 | SelfConjugate -> False,
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| 181 | Ghost -> Wbar,
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| 182 | QuantumNumbers -> {GhostNumber -> 1, Q -> -1},
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| 183 | Mass -> {MW,Internal},
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| 184 | Width -> {WW, 2.085},
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| 185 | PropagatorLabel -> "uWm",
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| 186 | PropagatorType -> GhostDash,
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| 187 | PropagatorArrow -> Forward
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| 188 | },
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| 189 | U[4] == {
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| 190 | ClassName -> ghG,
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| 191 | SelfConjugate -> False,
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| 192 | Indices -> {Index[Gluon]},
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| 193 | Ghost -> G,
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| 194 | PDG -> 82,
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| 195 | QuantumNumbers ->{GhostNumber -> 1},
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| 196 | Mass -> 0,
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| 197 | Width -> 0,
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| 198 | PropagatorLabel -> "uG",
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| 199 | PropagatorType -> GhostDash,
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| 200 | PropagatorArrow -> Forward
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| 201 | },
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| 202 |
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| 203 | (* Gauge bosons: unphysical vector fields *)
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| 204 | V[11] == {
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| 205 | ClassName -> B,
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| 206 | Unphysical -> True,
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| 207 | SelfConjugate -> True,
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| 208 | Definitions -> { B[mu_] -> -sw Z[mu]+cw A[mu]}
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| 209 | },
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| 210 | V[12] == {
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| 211 | ClassName -> Wi,
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| 212 | Unphysical -> True,
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| 213 | SelfConjugate -> True,
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| 214 | Indices -> {Index[SU2W]},
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| 215 | FlavorIndex -> SU2W,
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| 216 | 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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| 217 | },
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| 218 |
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| 219 | (* Ghosts: related to unphysical gauge bosons *)
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| 220 | U[11] == {
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| 221 | ClassName -> ghB,
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| 222 | Unphysical -> True,
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| 223 | SelfConjugate -> False,
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| 224 | Ghost -> B,
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| 225 | Definitions -> { ghB -> -sw ghZ + cw ghA}
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| 226 | },
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| 227 | U[12] == {
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| 228 | ClassName -> ghWi,
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| 229 | Unphysical -> True,
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| 230 | SelfConjugate -> False,
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| 231 | Ghost -> Wi,
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| 232 | Indices -> {Index[SU2W]},
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| 233 | FlavorIndex -> SU2W,
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| 234 | Definitions -> { ghWi[1] -> (ghWp+ghWm)/Sqrt[2], ghWi[2] -> (ghWm-ghWp)/(I*Sqrt[2]), ghWi[3] -> cw ghZ+sw ghA}
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| 235 | } ,
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| 236 |
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| 237 | (* Fermions: physical fields *)
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| 238 | F[1] == {
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| 239 | ClassName -> vl,
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| 240 | ClassMembers -> {ve,vm,vt},
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| 241 | Indices -> {Index[Generation]},
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| 242 | FlavorIndex -> Generation,
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| 243 | SelfConjugate -> False,
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| 244 | Mass -> 0,
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| 245 | Width -> 0,
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| 246 | QuantumNumbers -> {LeptonNumber -> 1},
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| 247 | PropagatorLabel -> {"v", "ve", "vm", "vt"} ,
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| 248 | PropagatorType -> S,
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| 249 | PropagatorArrow -> Forward,
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| 250 | PDG -> {12,14,16},
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| 251 | ParticleName -> {"ve","vm","vt"},
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| 252 | AntiParticleName -> {"ve~","vm~","vt~"},
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| 253 | FullName -> {"Electron-neutrino", "Mu-neutrino", "Tau-neutrino"}
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| 254 | },
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| 255 | F[2] == {
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| 256 | ClassName -> l,
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| 257 | ClassMembers -> {e, mu, ta},
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| 258 | Indices -> {Index[Generation]},
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| 259 | FlavorIndex -> Generation,
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| 260 | SelfConjugate -> False,
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| 261 | Mass -> {Ml, {Me,5.11*^-4}, {MMU,0.10566}, {MTA,1.777}},
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| 262 | Width -> 0,
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| 263 | QuantumNumbers -> {Q -> -1, LeptonNumber -> 1},
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| 264 | PropagatorLabel -> {"l", "e", "mu", "ta"},
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| 265 | PropagatorType -> Straight,
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| 266 | PropagatorArrow -> Forward,
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| 267 | PDG -> {11, 13, 15},
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| 268 | ParticleName -> {"e-", "mu-", "ta-"},
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| 269 | AntiParticleName -> {"e+", "mu+", "ta+"},
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| 270 | FullName -> {"Electron", "Muon", "Tau"}
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| 271 | },
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| 272 | F[3] == {
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| 273 | ClassName -> uq,
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| 274 | ClassMembers -> {u, c, t},
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| 275 | Indices -> {Index[Generation], Index[Colour]},
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| 276 | FlavorIndex -> Generation,
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| 277 | SelfConjugate -> False,
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| 278 | Mass -> {Mu, {MU, 2.55*^-3}, {MC,1.27}, {MT,172}},
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| 279 | Width -> {0, 0, {WT,1.50833649}},
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| 280 | QuantumNumbers -> {Q -> 2/3},
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| 281 | PropagatorLabel -> {"uq", "u", "c", "t"},
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| 282 | PropagatorType -> Straight,
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| 283 | PropagatorArrow -> Forward,
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| 284 | PDG -> {2, 4, 6},
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| 285 | ParticleName -> {"u", "c", "t" },
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| 286 | AntiParticleName -> {"u~", "c~", "t~"},
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| 287 | FullName -> {"u-quark", "c-quark", "t-quark"}
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| 288 | },
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| 289 | F[4] == {
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| 290 | ClassName -> dq,
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| 291 | ClassMembers -> {d, s, b},
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| 292 | Indices -> {Index[Generation], Index[Colour]},
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| 293 | FlavorIndex -> Generation,
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| 294 | SelfConjugate -> False,
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| 295 | Mass -> {Md, {MD,5.04*^-3}, {MS,0.101}, {MB,4.7}},
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| 296 | Width -> 0,
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| 297 | QuantumNumbers -> {Q -> -1/3},
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| 298 | PropagatorLabel -> {"dq", "d", "s", "b"},
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| 299 | PropagatorType -> Straight,
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| 300 | PropagatorArrow -> Forward,
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| 301 | PDG -> {1,3,5},
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| 302 | ParticleName -> {"d", "s", "b" },
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| 303 | AntiParticleName -> {"d~", "s~", "b~"},
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| 304 | FullName -> {"d-quark", "s-quark", "b-quark"}
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| 305 | },
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| 306 |
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| 307 | (* Fermions: unphysical fields *)
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| 308 | F[11] == {
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| 309 | ClassName -> LL,
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| 310 | Unphysical -> True,
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| 311 | Indices -> {Index[SU2D], Index[Generation]},
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| 312 | FlavorIndex -> SU2D,
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| 313 | SelfConjugate -> False,
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| 314 | QuantumNumbers -> {Y -> -1/2},
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| 315 | 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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| 316 | },
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| 317 | F[12] == {
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| 318 | ClassName -> lR,
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| 319 | Unphysical -> True,
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| 320 | Indices -> {Index[Generation]},
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| 321 | FlavorIndex -> Generation,
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| 322 | SelfConjugate -> False,
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| 323 | QuantumNumbers -> {Y -> -1},
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| 324 | Definitions -> { lR[sp1_,ff_] :> Module[{sp2}, ProjP[sp1,sp2] l[sp2,ff]] }
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| 325 | },
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| 326 | F[13] == {
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| 327 | ClassName -> QL,
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| 328 | Unphysical -> True,
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| 329 | Indices -> {Index[SU2D], Index[Generation], Index[Colour]},
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| 330 | FlavorIndex -> SU2D,
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| 331 | SelfConjugate -> False,
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| 332 | QuantumNumbers -> {Y -> 1/6},
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| 333 | Definitions -> {
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| 334 | QL[sp1_,1,ff_,cc_] :> Module[{sp2}, ProjM[sp1,sp2] uq[sp2,ff,cc]],
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| 335 | QL[sp1_,2,ff_,cc_] :> Module[{sp2,ff2}, CKM[ff,ff2] ProjM[sp1,sp2] dq[sp2,ff2,cc]] }
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| 336 | },
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| 337 | F[14] == {
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| 338 | ClassName -> uR,
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| 339 | Unphysical -> True,
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| 340 | Indices -> {Index[Generation], Index[Colour]},
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| 341 | FlavorIndex -> Generation,
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| 342 | SelfConjugate -> False,
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| 343 | QuantumNumbers -> {Y -> 2/3},
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| 344 | Definitions -> { uR[sp1_,ff_,cc_] :> Module[{sp2}, ProjP[sp1,sp2] uq[sp2,ff,cc]] }
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| 345 | },
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| 346 | F[15] == {
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| 347 | ClassName -> dR,
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| 348 | Unphysical -> True,
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| 349 | Indices -> {Index[Generation], Index[Colour]},
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| 350 | FlavorIndex -> Generation,
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| 351 | SelfConjugate -> False,
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| 352 | QuantumNumbers -> {Y -> -1/3},
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| 353 | Definitions -> { dR[sp1_,ff_,cc_] :> Module[{sp2}, ProjP[sp1,sp2] dq[sp2,ff,cc]] }
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| 354 | },
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| 355 |
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| 356 | (* Higgs: physical scalars *)
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| 357 | S[1] == {
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| 358 | ClassName -> H,
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| 359 | SelfConjugate -> True,
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| 360 | Mass -> {MH,125},
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| 361 | Width -> {WH,0.00407},
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| 362 | PropagatorLabel -> "H",
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| 363 | PropagatorType -> D,
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| 364 | PropagatorArrow -> None,
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| 365 | PDG -> 25,
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| 366 | ParticleName -> "H",
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| 367 | FullName -> "H"
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| 368 | },
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| 369 |
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| 370 | (* Higgs: physical scalars *)
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| 371 | S[2] == {
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| 372 | ClassName -> G0,
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| 373 | SelfConjugate -> True,
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| 374 | Goldstone -> Z,
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| 375 | Mass -> {MZ, 91.1876},
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| 376 | Width -> {WZ, 2.4952},
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| 377 | PropagatorLabel -> "Go",
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| 378 | PropagatorType -> D,
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| 379 | PropagatorArrow -> None,
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| 380 | PDG -> 250,
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| 381 | ParticleName -> "G0",
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| 382 | FullName -> "G0"
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| 383 | },
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| 384 | S[3] == {
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| 385 | ClassName -> GP,
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| 386 | SelfConjugate -> False,
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| 387 | Goldstone -> W,
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| 388 | Mass -> {MW, Internal},
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| 389 | QuantumNumbers -> {Q -> 1},
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| 390 | Width -> {WW, 2.085},
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| 391 | PropagatorLabel -> "GP",
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| 392 | PropagatorType -> D,
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| 393 | PropagatorArrow -> None,
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| 394 | PDG -> 251,
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| 395 | ParticleName -> "G+",
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| 396 | AntiParticleName -> "G-",
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| 397 | FullName -> "GP"
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| 398 | },
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| 399 |
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| 400 | (* Higgs: unphysical scalars *)
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| 401 | S[11] == {
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| 402 | ClassName -> Phi,
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| 403 | Unphysical -> True,
|
|---|
| 404 | Indices -> {Index[SU2D]},
|
|---|
| 405 | FlavorIndex -> SU2D,
|
|---|
| 406 | SelfConjugate -> False,
|
|---|
| 407 | QuantumNumbers -> {Y -> 1/2},
|
|---|
| 408 | Definitions -> { Phi[1] -> -I GP, Phi[2] -> (vev + H + I G0)/Sqrt[2] }
|
|---|
| 409 | }
|
|---|
| 410 | };
|
|---|
| 411 |
|
|---|
| 412 | (* ************************** *)
|
|---|
| 413 | (* ***** Gauge ***** *)
|
|---|
| 414 | (* ***** Parameters ***** *)
|
|---|
| 415 | (* ***** (FeynArts) ***** *)
|
|---|
| 416 | (* ************************** *)
|
|---|
| 417 |
|
|---|
| 418 | GaugeXi[ V[1] ] = GaugeXi[A];
|
|---|
| 419 | GaugeXi[ V[2] ] = GaugeXi[Z];
|
|---|
| 420 | GaugeXi[ V[3] ] = GaugeXi[W];
|
|---|
| 421 | GaugeXi[ V[4] ] = GaugeXi[G];
|
|---|
| 422 | GaugeXi[ S[1] ] = 1;
|
|---|
| 423 | GaugeXi[ S[2] ] = GaugeXi[Z];
|
|---|
| 424 | GaugeXi[ S[3] ] = GaugeXi[W];
|
|---|
| 425 | GaugeXi[ U[1] ] = GaugeXi[A];
|
|---|
| 426 | GaugeXi[ U[2] ] = GaugeXi[Z];
|
|---|
| 427 | GaugeXi[ U[31] ] = GaugeXi[W];
|
|---|
| 428 | GaugeXi[ U[32] ] = GaugeXi[W];
|
|---|
| 429 | GaugeXi[ U[4] ] = GaugeXi[G];
|
|---|
| 430 |
|
|---|
| 431 | (* ************************** *)
|
|---|
| 432 | (* ***** Parameters ***** *)
|
|---|
| 433 | (* ************************** *)
|
|---|
| 434 | M$Parameters = {
|
|---|
| 435 |
|
|---|
| 436 | (* External parameters *)
|
|---|
| 437 | LambdaSMEFT == {
|
|---|
| 438 | ParameterType -> External,
|
|---|
| 439 | BlockName -> SMEFTcutoff,
|
|---|
| 440 | Value -> 1000.0,
|
|---|
| 441 | TeX -> \[CapitalLambda],
|
|---|
| 442 | Description -> "Defining scale of the effective theory"
|
|---|
| 443 | },
|
|---|
| 444 |
|
|---|
| 445 | mueft == {
|
|---|
| 446 | ParameterType -> External,
|
|---|
| 447 | BlockName -> SMEFTLoop,
|
|---|
| 448 | Value -> 200.0,
|
|---|
| 449 | TeX -> Subscript[\[Mu],EFT],
|
|---|
| 450 | Description -> "scale defining the renormalisation scheme"
|
|---|
| 451 | },
|
|---|
| 452 |
|
|---|
| 453 | cqq1 == {
|
|---|
| 454 | ParameterType -> External,
|
|---|
| 455 | BlockName -> SMEFT,
|
|---|
| 456 | Value -> 0,
|
|---|
| 457 | InteractionOrder -> {NP,1},
|
|---|
| 458 | TeX -> Subsuperscript[c,qq,(1)]
|
|---|
| 459 | },
|
|---|
| 460 | cqq3 == {
|
|---|
| 461 | ParameterType -> External,
|
|---|
| 462 | BlockName -> SMEFT,
|
|---|
| 463 | Value -> 0,
|
|---|
| 464 | InteractionOrder -> {NP,1},
|
|---|
| 465 | TeX -> Subsuperscript[c,qq,(3)]
|
|---|
| 466 | },
|
|---|
| 467 | cuu == {
|
|---|
| 468 | ParameterType -> External,
|
|---|
| 469 | BlockName -> SMEFT,
|
|---|
| 470 | Value -> 0,
|
|---|
| 471 | InteractionOrder -> {NP,1},
|
|---|
| 472 | TeX -> Subscript[c,uu]
|
|---|
| 473 | },
|
|---|
| 474 | cdd == {
|
|---|
| 475 | ParameterType -> External,
|
|---|
| 476 | BlockName -> SMEFT,
|
|---|
| 477 | Value -> 0,
|
|---|
| 478 | InteractionOrder -> {NP,1},
|
|---|
| 479 | TeX -> Subscript[c,dd]
|
|---|
| 480 | },
|
|---|
| 481 | cud8 == {
|
|---|
| 482 | ParameterType -> External,
|
|---|
| 483 | BlockName -> SMEFT,
|
|---|
| 484 | Value -> 0,
|
|---|
| 485 | InteractionOrder -> {NP,1},
|
|---|
| 486 | TeX -> Subsuperscript[c,ud,(8)]
|
|---|
| 487 | },
|
|---|
| 488 |
|
|---|
| 489 | cud1 == {
|
|---|
| 490 | ParameterType -> External,
|
|---|
| 491 | BlockName -> SMEFT,
|
|---|
| 492 | Value -> 0,
|
|---|
| 493 | InteractionOrder -> {NP,1},
|
|---|
| 494 | TeX -> Subsuperscript[c,ud,(1)]
|
|---|
| 495 | },
|
|---|
| 496 | cqu1 == {
|
|---|
| 497 | ParameterType -> External,
|
|---|
| 498 | BlockName -> SMEFT,
|
|---|
| 499 | Value -> 0,
|
|---|
| 500 | InteractionOrder -> {NP,1},
|
|---|
| 501 | TeX -> Subsuperscript[c,qu,(1)]
|
|---|
| 502 | },
|
|---|
| 503 | cqd1 == {
|
|---|
| 504 | ParameterType -> External,
|
|---|
| 505 | BlockName -> SMEFT,
|
|---|
| 506 | Value -> 0,
|
|---|
| 507 | InteractionOrder -> {NP,1},
|
|---|
| 508 | TeX -> Subsuperscript[c,qd,(1)]
|
|---|
| 509 | },
|
|---|
| 510 |
|
|---|
| 511 | cqu8 == {
|
|---|
| 512 | ParameterType -> External,
|
|---|
| 513 | BlockName -> SMEFT,
|
|---|
| 514 | Value -> 0,
|
|---|
| 515 | InteractionOrder -> {NP,1},
|
|---|
| 516 | TeX -> Subsuperscript[c,qu,(8)]
|
|---|
| 517 | },
|
|---|
| 518 | cqd8 == {
|
|---|
| 519 | ParameterType -> External,
|
|---|
| 520 | BlockName -> SMEFT,
|
|---|
| 521 | Value -> 0,
|
|---|
| 522 | InteractionOrder -> {NP,1},
|
|---|
| 523 | TeX -> Subsuperscript[c,qd,(8)]
|
|---|
| 524 | },
|
|---|
| 525 | aEWM1 == {
|
|---|
| 526 | ParameterType -> External,
|
|---|
| 527 | BlockName -> SMINPUTS,
|
|---|
| 528 | OrderBlock -> 1,
|
|---|
| 529 | Value -> 127.9,
|
|---|
| 530 | InteractionOrder -> {QED,-2},
|
|---|
| 531 | Description -> "Inverse of the EW coupling constant at the Z pole"
|
|---|
| 532 | },
|
|---|
| 533 | Gf == {
|
|---|
| 534 | ParameterType -> External,
|
|---|
| 535 | BlockName -> SMINPUTS,
|
|---|
| 536 | OrderBlock -> 2,
|
|---|
| 537 | Value -> 1.16637*^-5,
|
|---|
| 538 | InteractionOrder -> {QED,2},
|
|---|
| 539 | TeX -> Subscript[G,f],
|
|---|
| 540 | Description -> "Fermi constant"
|
|---|
| 541 | },
|
|---|
| 542 | aS == {
|
|---|
| 543 | ParameterType -> External,
|
|---|
| 544 | BlockName -> SMINPUTS,
|
|---|
| 545 | OrderBlock -> 3,
|
|---|
| 546 | Value -> 0.1184,
|
|---|
| 547 | InteractionOrder -> {QCD,2},
|
|---|
| 548 | TeX -> Subscript[\[Alpha],s],
|
|---|
| 549 | Description -> "Strong coupling constant at the Z pole"
|
|---|
| 550 | },
|
|---|
| 551 | ymdo == {
|
|---|
| 552 | ParameterType -> External,
|
|---|
| 553 | BlockName -> YUKAWA,
|
|---|
| 554 | OrderBlock -> 1,
|
|---|
| 555 | Value -> 5.04*^-3,
|
|---|
| 556 | Description -> "Down Yukawa mass"
|
|---|
| 557 | },
|
|---|
| 558 | ymup == {
|
|---|
| 559 | ParameterType -> External,
|
|---|
| 560 | BlockName -> YUKAWA,
|
|---|
| 561 | OrderBlock -> 2,
|
|---|
| 562 | Value -> 2.55*^-3,
|
|---|
| 563 | Description -> "Up Yukawa mass"
|
|---|
| 564 | },
|
|---|
| 565 | yms == {
|
|---|
| 566 | ParameterType -> External,
|
|---|
| 567 | BlockName -> YUKAWA,
|
|---|
| 568 | OrderBlock -> 3,
|
|---|
| 569 | Value -> 0.101,
|
|---|
| 570 | Description -> "Strange Yukawa mass"
|
|---|
| 571 | },
|
|---|
| 572 | ymc == {
|
|---|
| 573 | ParameterType -> External,
|
|---|
| 574 | BlockName -> YUKAWA,
|
|---|
| 575 | OrderBlock -> 4,
|
|---|
| 576 | Value -> 1.27,
|
|---|
| 577 | Description -> "Charm Yukawa mass"
|
|---|
| 578 | },
|
|---|
| 579 | ymb == {
|
|---|
| 580 | ParameterType -> External,
|
|---|
| 581 | BlockName -> YUKAWA,
|
|---|
| 582 | OrderBlock -> 5,
|
|---|
| 583 | Value -> 4.7,
|
|---|
| 584 | Description -> "Bottom Yukawa mass"
|
|---|
| 585 | },
|
|---|
| 586 | ymt == {
|
|---|
| 587 | ParameterType -> External,
|
|---|
| 588 | BlockName -> YUKAWA,
|
|---|
| 589 | OrderBlock -> 6,
|
|---|
| 590 | Value -> 172,
|
|---|
| 591 | Description -> "Top Yukawa mass"
|
|---|
| 592 | },
|
|---|
| 593 | yme == {
|
|---|
| 594 | ParameterType -> External,
|
|---|
| 595 | BlockName -> YUKAWA,
|
|---|
| 596 | OrderBlock -> 11,
|
|---|
| 597 | Value -> 5.11*^-4,
|
|---|
| 598 | Description -> "Electron Yukawa mass"
|
|---|
| 599 | },
|
|---|
| 600 | ymm == {
|
|---|
| 601 | ParameterType -> External,
|
|---|
| 602 | BlockName -> YUKAWA,
|
|---|
| 603 | OrderBlock -> 13,
|
|---|
| 604 | Value -> 0.10566,
|
|---|
| 605 | Description -> "Muon Yukawa mass"
|
|---|
| 606 | },
|
|---|
| 607 | ymtau == {
|
|---|
| 608 | ParameterType -> External,
|
|---|
| 609 | BlockName -> YUKAWA,
|
|---|
| 610 | OrderBlock -> 15,
|
|---|
| 611 | Value -> 1.777,
|
|---|
| 612 | Description -> "Tau Yukawa mass"
|
|---|
| 613 | },
|
|---|
| 614 | cabi == {
|
|---|
| 615 | ParameterType -> External,
|
|---|
| 616 | BlockName -> CKMBLOCK,
|
|---|
| 617 | OrderBlock -> 1,
|
|---|
| 618 | Value -> 0.227736,
|
|---|
| 619 | TeX -> Subscript[\[Theta], c],
|
|---|
| 620 | Description -> "Cabibbo angle"
|
|---|
| 621 | },
|
|---|
| 622 |
|
|---|
| 623 | (* Internal Parameters *)
|
|---|
| 624 | aEW == {
|
|---|
| 625 | ParameterType -> Internal,
|
|---|
| 626 | Value -> 1/aEWM1,
|
|---|
| 627 | InteractionOrder -> {QED,2},
|
|---|
| 628 | TeX -> Subscript[\[Alpha], EW],
|
|---|
| 629 | Description -> "Electroweak coupling contant"
|
|---|
| 630 | },
|
|---|
| 631 | MW == {
|
|---|
| 632 | ParameterType -> Internal,
|
|---|
| 633 | Value -> Sqrt[MZ^2/2+Sqrt[MZ^4/4-Pi/Sqrt[2]*aEW/Gf*MZ^2]],
|
|---|
| 634 | TeX -> Subscript[M,W],
|
|---|
| 635 | Description -> "W mass"
|
|---|
| 636 | },
|
|---|
| 637 | sw2 == {
|
|---|
| 638 | ParameterType -> Internal,
|
|---|
| 639 | Value -> 1-(MW/MZ)^2,
|
|---|
| 640 | Description -> "Squared Sin of the Weinberg angle"
|
|---|
| 641 | },
|
|---|
| 642 | ee == {
|
|---|
| 643 | ParameterType -> Internal,
|
|---|
| 644 | Value -> Sqrt[4 Pi aEW],
|
|---|
| 645 | InteractionOrder -> {QED,1},
|
|---|
| 646 | TeX -> e,
|
|---|
| 647 | Description -> "Electric coupling constant"
|
|---|
| 648 | },
|
|---|
| 649 | cw == {
|
|---|
| 650 | ParameterType -> Internal,
|
|---|
| 651 | Value -> Sqrt[1-sw2],
|
|---|
| 652 | TeX -> Subscript[c,w],
|
|---|
| 653 | Description -> "Cosine of the Weinberg angle"
|
|---|
| 654 | },
|
|---|
| 655 | sw == {
|
|---|
| 656 | ParameterType -> Internal,
|
|---|
| 657 | Value -> Sqrt[sw2],
|
|---|
| 658 | TeX -> Subscript[s,w],
|
|---|
| 659 | Description -> "Sine of the Weinberg angle"
|
|---|
| 660 | },
|
|---|
| 661 | gw == {
|
|---|
| 662 | ParameterType -> Internal,
|
|---|
| 663 | Definitions -> {gw->ee/sw},
|
|---|
| 664 | InteractionOrder -> {QED,1},
|
|---|
| 665 | TeX -> Subscript[g,w],
|
|---|
| 666 | Description -> "Weak coupling constant at the Z pole"
|
|---|
| 667 | },
|
|---|
| 668 | g1 == {
|
|---|
| 669 | ParameterType -> Internal,
|
|---|
| 670 | Definitions -> {g1->ee/cw},
|
|---|
| 671 | InteractionOrder -> {QED,1},
|
|---|
| 672 | TeX -> Subscript[g,1],
|
|---|
| 673 | Description -> "U(1)Y coupling constant at the Z pole"
|
|---|
| 674 | },
|
|---|
| 675 | gs == {
|
|---|
| 676 | ParameterType -> Internal,
|
|---|
| 677 | Value -> Sqrt[4 Pi aS],
|
|---|
| 678 | InteractionOrder -> {QCD,1},
|
|---|
| 679 | TeX -> Subscript[g,s],
|
|---|
| 680 | ParameterName -> G,
|
|---|
| 681 | Description -> "Strong coupling constant at the Z pole"
|
|---|
| 682 | },
|
|---|
| 683 | vev == {
|
|---|
| 684 | ParameterType -> Internal,
|
|---|
| 685 | Value -> 2*MW*sw/ee,
|
|---|
| 686 | InteractionOrder -> {QED,-1},
|
|---|
| 687 | Description -> "Higgs vacuum expectation value"
|
|---|
| 688 | },
|
|---|
| 689 | lam == {
|
|---|
| 690 | ParameterType -> Internal,
|
|---|
| 691 | Value -> MH^2/(2*vev^2),
|
|---|
| 692 | InteractionOrder -> {QED, 2},
|
|---|
| 693 | Description -> "Higgs quartic coupling"
|
|---|
| 694 | },
|
|---|
| 695 | muH == {
|
|---|
| 696 | ParameterType -> Internal,
|
|---|
| 697 | Value -> Sqrt[vev^2 lam],
|
|---|
| 698 | TeX -> \[Mu],
|
|---|
| 699 | Description -> "Coefficient of the quadratic piece of the Higgs potential"
|
|---|
| 700 | },
|
|---|
| 701 | yl == {
|
|---|
| 702 | ParameterType -> Internal,
|
|---|
| 703 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 704 | Definitions -> {yl[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 705 | Value -> {yl[1,1] -> Sqrt[2] yme / vev, yl[2,2] -> Sqrt[2] ymm / vev, yl[3,3] -> Sqrt[2] ymtau / vev},
|
|---|
| 706 | InteractionOrder -> {QED, 1},
|
|---|
| 707 | ParameterName -> {yl[1,1] -> ye, yl[2,2] -> ym, yl[3,3] -> ytau},
|
|---|
| 708 | TeX -> Superscript[y, l],
|
|---|
| 709 | Description -> "Lepton Yukawa couplings"
|
|---|
| 710 | },
|
|---|
| 711 | yu == {
|
|---|
| 712 | ParameterType -> Internal,
|
|---|
| 713 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 714 | Definitions -> {yu[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 715 | Value -> {yu[1,1] -> Sqrt[2] ymup/vev, yu[2,2] -> Sqrt[2] ymc/vev, yu[3,3] -> Sqrt[2] ymt/vev},
|
|---|
| 716 | InteractionOrder -> {QED, 1},
|
|---|
| 717 | ParameterName -> {yu[1,1] -> yup, yu[2,2] -> yc, yu[3,3] -> yt},
|
|---|
| 718 | TeX -> Superscript[y, u],
|
|---|
| 719 | Description -> "Up-type Yukawa couplings"
|
|---|
| 720 | },
|
|---|
| 721 | yd == {
|
|---|
| 722 | ParameterType -> Internal,
|
|---|
| 723 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 724 | Definitions -> {yd[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 725 | Value -> {yd[1,1] -> Sqrt[2] ymdo/vev, yd[2,2] -> Sqrt[2] yms/vev, yd[3,3] -> Sqrt[2] ymb/vev},
|
|---|
| 726 | InteractionOrder -> {QED, 1},
|
|---|
| 727 | ParameterName -> {yd[1,1] -> ydo, yd[2,2] -> ys, yd[3,3] -> yb},
|
|---|
| 728 | TeX -> Superscript[y, d],
|
|---|
| 729 | Description -> "Down-type Yukawa couplings"
|
|---|
| 730 | },
|
|---|
| 731 | (* N. B. : only Cabibbo mixing! *)
|
|---|
| 732 | CKM == {
|
|---|
| 733 | ParameterType -> Internal,
|
|---|
| 734 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 735 | Unitary -> True,
|
|---|
| 736 | Value -> {CKM[1,1] -> Cos[cabi], CKM[1,2] -> Sin[cabi], CKM[1,3] -> 0,
|
|---|
| 737 | CKM[2,1] -> -Sin[cabi], CKM[2,2] -> Cos[cabi], CKM[2,3] -> 0,
|
|---|
| 738 | CKM[3,1] -> 0, CKM[3,2] -> 0, CKM[3,3] -> 1},
|
|---|
| 739 | TeX -> Superscript[V,CKM],
|
|---|
| 740 | Description -> "CKM-Matrix"}
|
|---|
| 741 | };
|
|---|
| 742 |
|
|---|
| 743 | (* ************************** *)
|
|---|
| 744 | (* ***** Lagrangian ***** *)
|
|---|
| 745 | (* ************************** *)
|
|---|
| 746 |
|
|---|
| 747 | (***** Dim-6 *****)
|
|---|
| 748 |
|
|---|
| 749 | Lqq1 := Block[{mu,sp1,sp2,sp3,sp4,ii,jj,ff1,ff2,cc1,cc2},
|
|---|
| 750 | op = ExpandIndices[
|
|---|
| 751 | QLbar[sp1,ii,ff1,cc1].QL[sp2,ii,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 752 | QLbar[sp3,jj,ff2,cc2].QL[sp4,jj,ff2,cc2] Ga[mu,sp3,sp4]
|
|---|
| 753 | +QLbar[sp1,ii,ff1,cc1].QL[sp2,ii,ff2,cc1] Ga[mu,sp1,sp2]
|
|---|
| 754 | QLbar[sp3,jj,ff2,cc2].QL[sp4,jj,ff1,cc2] Ga[mu,sp3,sp4]
|
|---|
| 755 | -Sum[QLbar[sp1,ii,ff1,cc1].QL[sp2,ii,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 756 | QLbar[sp3,jj,ff1,cc2].QL[sp4,jj,ff1,cc2] Ga[mu,sp3,sp4],{ff1,1,3}],
|
|---|
| 757 | FlavorExpand->{SU2W,SU2D}];
|
|---|
| 758 | Return[op cqq1/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 759 |
|
|---|
| 760 | Lqq3 := Block[{mu,sp1,sp2,sp3,sp4,cc1,cc2,ii1,jj1,ii2,jj2,kk,ff1,ff2},
|
|---|
| 761 | op = ExpandIndices[
|
|---|
| 762 | QLbar[sp1,ii1,ff1,cc1].QL[sp2,jj1,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 763 | QLbar[sp3,ii2,ff2,cc2].QL[sp4,jj2,ff2,cc2] Ga[mu,sp3,sp4]
|
|---|
| 764 | PauliSigma[kk,ii1,jj1] PauliSigma[kk,ii2,jj2]
|
|---|
| 765 | +QLbar[sp1,ii1,ff1,cc1].QL[sp2,jj1,ff2,cc1] Ga[mu,sp1,sp2]
|
|---|
| 766 | QLbar[sp3,ii2,ff2,cc2].QL[sp4,jj2,ff1,cc2] Ga[mu,sp3,sp4]
|
|---|
| 767 | PauliSigma[kk,ii1,jj1] PauliSigma[kk,ii2,jj2]
|
|---|
| 768 | -Sum[QLbar[sp1,ii1,ff1,cc1].QL[sp2,jj1,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 769 | QLbar[sp3,ii2,ff1,cc2].QL[sp4,jj2,ff1,cc2] Ga[mu,sp3,sp4]
|
|---|
| 770 | PauliSigma[kk,ii1,jj1] PauliSigma[kk,ii2,jj2],{ff1,1,3}],
|
|---|
| 771 | FlavorExpand->{SU2W,SU2D}];
|
|---|
| 772 | Return[op cqq3/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 773 |
|
|---|
| 774 | Luu := Block[{mu,sp1,sp2,sp3,sp4,cc1,cc2,ff1,ff2},
|
|---|
| 775 | op = ExpandIndices[
|
|---|
| 776 | uRbar[sp1,ff1,cc1].uR[sp2,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 777 | uRbar[sp3,ff2,cc2].uR[sp4,ff2,cc2] Ga[mu,sp3,sp4]
|
|---|
| 778 | +uRbar[sp1,ff1,cc1].uR[sp2,ff2,cc1] Ga[mu,sp1,sp2]
|
|---|
| 779 | uRbar[sp3,ff2,cc2].uR[sp4,ff1,cc2] Ga[mu,sp3,sp4]
|
|---|
| 780 | -Sum[uRbar[sp1,ff1,cc1].uR[sp2,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 781 | uRbar[sp3,ff1,cc2].uR[sp4,ff1,cc2] Ga[mu,sp3,sp4],{ff1,1,3}],
|
|---|
| 782 | FlavorExpand->{SU2W,SU2D}];
|
|---|
| 783 | Return[op cuu/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 784 |
|
|---|
| 785 | Ldd := Block[{mu,sp1,sp2,sp3,sp4,cc1,cc2,ff1,ff2},
|
|---|
| 786 | op = ExpandIndices[
|
|---|
| 787 | dRbar[sp1,ff1,cc1].dR[sp2,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 788 | dRbar[sp3,ff2,cc2].dR[sp4,ff2,cc2] Ga[mu,sp3,sp4]
|
|---|
| 789 | +dRbar[sp1,ff1,cc1].dR[sp2,ff2,cc1] Ga[mu,sp1,sp2]
|
|---|
| 790 | dRbar[sp3,ff2,cc2].dR[sp4,ff1,cc2] Ga[mu,sp3,sp4]
|
|---|
| 791 | -Sum[dRbar[sp1,ff1,cc1].dR[sp2,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 792 | dRbar[sp3,ff1,cc2].dR[sp4,ff1,cc2] Ga[mu,sp3,sp4],{ff1,1,3}],
|
|---|
| 793 | FlavorExpand->{SU2W,SU2D}];
|
|---|
| 794 | Return[op cdd/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 795 |
|
|---|
| 796 | Lud8 := Block[{mu,sp1,sp2,sp3,sp4,cc1,cc2,cc3,cc4,aa,ff1,ff2},
|
|---|
| 797 | op = ExpandIndices[
|
|---|
| 798 | uRbar[sp1,ff1,cc1].uR[sp2,ff1,cc2] Ga[mu,sp1,sp2]
|
|---|
| 799 | dRbar[sp3,ff2,cc3].dR[sp4,ff2,cc4] Ga[mu,sp3,sp4]
|
|---|
| 800 | T[aa,cc1,cc2] T[aa,cc3,cc4],
|
|---|
| 801 | FlavorExpand->{SU2D,SU2W}];
|
|---|
| 802 | Return[op cud8/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 803 |
|
|---|
| 804 | Lud1 := Block[{mu,sp1,sp2,sp3,sp4,cc1,cc2,ff1,ff2},
|
|---|
| 805 | op = ExpandIndices[
|
|---|
| 806 | uRbar[sp1,ff1,cc1].uR[sp2,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 807 | dRbar[sp3,ff2,cc2].dR[sp4,ff2,cc2] Ga[mu,sp3,sp4],
|
|---|
| 808 | FlavorExpand->{SU2D,SU2W}];
|
|---|
| 809 | Return[op cud1/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 810 |
|
|---|
| 811 | Lqu1 := Block[{mu,sp1,sp2,sp3,sp4,ii,cc1,cc2,ff1,ff2},
|
|---|
| 812 | op = ExpandIndices[
|
|---|
| 813 | QLbar[sp1,ii,ff1,cc1].QL[sp2,ii,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 814 | uRbar[sp3,ff2,cc2].uR[sp4,ff2,cc2] Ga[mu,sp3,sp4],
|
|---|
| 815 | FlavorExpand->{SU2W,SU2D}];
|
|---|
| 816 | Return[op cqu1/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 817 |
|
|---|
| 818 | Lqd1 := Block[{mu,sp1,sp2,sp3,sp4,ii,cc1,cc2,ff1,ff2},
|
|---|
| 819 | op = ExpandIndices[
|
|---|
| 820 | QLbar[sp1,ii,ff1,cc1].QL[sp2,ii,ff1,cc1] Ga[mu,sp1,sp2]
|
|---|
| 821 | dRbar[sp3,ff2,cc2].dR[sp4,ff2,cc2] Ga[mu,sp3,sp4],
|
|---|
| 822 | FlavorExpand->{SU2W,SU2D}];
|
|---|
| 823 | Return[op cqd1/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 824 |
|
|---|
| 825 | Lqu8 := Block[{mu,sp1,sp2,sp3,sp4,ii,cc1,cc2,cc3,cc4,aa,ff1,ff2},
|
|---|
| 826 | op = ExpandIndices[
|
|---|
| 827 | QLbar[sp1,ii,ff1,cc1].QL[sp2,ii,ff1,cc2] Ga[mu,sp1,sp2]
|
|---|
| 828 | uRbar[sp3,ff2,cc3].uR[sp4,ff2,cc4] Ga[mu,sp3,sp4]
|
|---|
| 829 | T[aa,cc1,cc2] T[aa,cc3,cc4],
|
|---|
| 830 | FlavorExpand->{SU2W,SU2D}];
|
|---|
| 831 | Return[op cqu8/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 832 |
|
|---|
| 833 | Lqd8 := Block[{mu,sp1,sp2,sp3,sp4,ii,cc1,cc2,cc3,cc4,aa,ff1,ff2},
|
|---|
| 834 | op = ExpandIndices[
|
|---|
| 835 | QLbar[sp1,ii,ff1,cc1].QL[sp2,ii,ff1,cc2] Ga[mu,sp1,sp2]
|
|---|
| 836 | dRbar[sp3,ff2,cc3].dR[sp4,ff2,cc4] Ga[mu,sp3,sp4]
|
|---|
| 837 | T[aa,cc1,cc2] T[aa,cc3,cc4],
|
|---|
| 838 | FlavorExpand->{SU2W,SU2D}];
|
|---|
| 839 | Return[op cqd8/LambdaSMEFT^2 /.CKM[a_,b_]->IndexDelta[a,b] //OptimizeIndex];];
|
|---|
| 840 |
|
|---|
| 841 | L4lq := Lqq1 + Lqq3 + Luu + Ldd + Lud8 + Lud1 + Lqu1 + Lqd1 + Lqu8 + Lqd8;
|
|---|
| 842 |
|
|---|
| 843 | (***** SM *****)
|
|---|
| 844 |
|
|---|
| 845 | LGauge := Block[{mu,nu,ii,aa},
|
|---|
| 846 | ExpandIndices[-1/4 FS[B,mu,nu] FS[B,mu,nu] - 1/4 FS[Wi,mu,nu,ii] FS[Wi,mu,nu,ii] - 1/4 FS[G,mu,nu,aa] FS[G,mu,nu,aa], FlavorExpand->SU2W]];
|
|---|
| 847 |
|
|---|
| 848 | LFermions := Block[{mu},
|
|---|
| 849 | ExpandIndices[I*(
|
|---|
| 850 | QLbar.Ga[mu].DC[QL, mu] + LLbar.Ga[mu].DC[LL, mu] + uRbar.Ga[mu].DC[uR, mu] + dRbar.Ga[mu].DC[dR, mu] + lRbar.Ga[mu].DC[lR, mu]),
|
|---|
| 851 | FlavorExpand->{SU2W,SU2D}]/.{CKM[a_,b_] Conjugate[CKM[a_,c_]]->IndexDelta[b,c], CKM[b_,a_] Conjugate[CKM[c_,a_]]->IndexDelta[b,c]}];
|
|---|
| 852 |
|
|---|
| 853 | LHiggs := Block[{ii,mu, feynmangaugerules},
|
|---|
| 854 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar ->0}, {}];
|
|---|
| 855 |
|
|---|
| 856 | ExpandIndices[DC[Phibar[ii],mu] DC[Phi[ii],mu] + muH^2 Phibar[ii] Phi[ii] - lam Phibar[ii] Phi[ii] Phibar[jj] Phi[jj], FlavorExpand->{SU2D,SU2W}]/.feynmangaugerules
|
|---|
| 857 | ];
|
|---|
| 858 |
|
|---|
| 859 | LYukawa := Block[{sp,ii,jj,cc,ff1,ff2,ff3,yuk,feynmangaugerules},
|
|---|
| 860 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar ->0}, {}];
|
|---|
| 861 |
|
|---|
| 862 | yuk = ExpandIndices[
|
|---|
| 863 | -yd[ff2, ff3] CKM[ff1, ff2] QLbar[sp, ii, ff1, cc].dR [sp, ff3, cc] Phi[ii] -
|
|---|
| 864 | yl[ff1, ff3] LLbar[sp, ii, ff1].lR [sp, ff3] Phi[ii] -
|
|---|
| 865 | yu[ff1, ff2] QLbar[sp, ii, ff1, cc].uR [sp, ff2, cc] Phibar[jj] Eps[ii, jj], FlavorExpand -> SU2D];
|
|---|
| 866 | yuk = yuk /. { CKM[a_, b_] Conjugate[CKM[a_, c_]] -> IndexDelta[b, c], CKM[b_, a_] Conjugate[CKM[c_, a_]] -> IndexDelta[b, c]};
|
|---|
| 867 | yuk+HC[yuk]/.feynmangaugerules
|
|---|
| 868 | ];
|
|---|
| 869 |
|
|---|
| 870 | LGhost := Block[{LGh1,LGhw,LGhs,LGhphi,mu, generators,gh,ghbar,Vectorize,phi1,phi2,togoldstones,doublet,doublet0},
|
|---|
| 871 | (* Pure gauge piece *)
|
|---|
| 872 | LGh1 = -ghBbar.del[DC[ghB,mu],mu];
|
|---|
| 873 | LGhw = -ghWibar[ii].del[DC[ghWi[ii],mu],mu];
|
|---|
| 874 | LGhs = -ghGbar[ii].del[DC[ghG[ii],mu],mu];
|
|---|
| 875 |
|
|---|
| 876 | (* Scalar pieces: see Peskin pages 739-742 *)
|
|---|
| 877 | (* phi1 and phi2 are the real degrees of freedom of GP *)
|
|---|
| 878 | (* Vectorize transforms a doublet in a vector in the phi-basis, i.e. the basis of real degrees of freedom *)
|
|---|
| 879 | gh = {ghB, ghWi[1], ghWi[2], ghWi[3]};
|
|---|
| 880 | ghbar = {ghBbar, ghWibar[1], ghWibar[2], ghWibar[3]};
|
|---|
| 881 | generators = {-I/2 g1 IdentityMatrix[2], -I/2 gw PauliSigma[1], -I/2 gw PauliSigma[2], -I/2 gw PauliSigma[3]};
|
|---|
| 882 | doublet = Expand[{(-I phi1 - phi2)/Sqrt[2], Phi[2]} /. MR$Definitions /. vev -> 0];
|
|---|
| 883 | doublet0 = {0, vev/Sqrt[2]};
|
|---|
| 884 | 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}];
|
|---|
| 885 | togoldstones := {phi1 -> (GP + GPbar)/Sqrt[2], phi2 -> (-GP + GPbar)/(I Sqrt[2])};
|
|---|
| 886 | LGhphi=Plus@@Flatten[Table[-ghbar[[kkk]].gh[[lll]] Vectorize[generators[[kkk]].doublet0].Vectorize[generators[[lll]].(doublet+doublet0)],{kkk,4},{lll,4}]] /.togoldstones;
|
|---|
| 887 |
|
|---|
| 888 | ExpandIndices[ LGhs + If[FeynmanGauge, LGh1 + LGhw + LGhphi,0], FlavorExpand->SU2W]];
|
|---|
| 889 |
|
|---|
| 890 | LSM:= LGauge + LFermions + LHiggs + LYukawa + LGhost;
|
|---|
| 891 |
|
|---|
| 892 | L6:= LSM + L4lq;
|
|---|
| 893 |
|
|---|