| 1 | (* ************************** *)
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| 2 | (* ***** Information ***** *)
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| 3 | (* ************************** *)
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| 4 | M$ModelName = "HELatNLO";
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| 5 |
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| 6 | M$Information = {
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| 7 | Authors -> {"B. Fuks"},
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| 8 | Version -> "0.1",
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| 9 | Date -> "05. 02. 2016",
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| 10 | Institutions -> {"LPTHE Paris / UPMC"},
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| 11 | Emails -> {"fuks@lpthe.jussieu.fr"},
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| 12 | References -> "",
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| 13 | URLs -> "https://feynrules.irmp.ucl.ac.be/wiki/SILH"
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| 14 | };
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| 15 |
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| 16 | FeynmanGauge = True;
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| 17 |
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| 18 | (* Change log *)
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| 19 | (* v0.1 (05.02.2016) KM: *)
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| 20 |
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| 21 |
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| 22 | (* ************************** *)
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| 23 | (* ***** Gauge groups ***** *)
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| 24 | (* ************************** *)
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| 25 | M$GaugeGroups = {
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| 26 | U1Y == {
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| 27 | Abelian -> True,
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| 28 | CouplingConstant -> g1,
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| 29 | GaugeBoson -> B,
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| 30 | Charge -> Y
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| 31 | },
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| 32 | SU2L == {
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| 33 | Abelian -> False,
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| 34 | CouplingConstant -> gw,
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| 35 | GaugeBoson -> Wi,
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| 36 | StructureConstant -> Eps,
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| 37 | Representations -> {Ta,SU2D},
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| 38 | Definitions -> {Ta[a_,b_,c_]->PauliSigma[a,b,c]/2, FSU2L[i_,j_,k_]:> I Eps[i,j,k]}
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| 39 | },
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| 40 | SU3C == {
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| 41 | Abelian -> False,
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| 42 | CouplingConstant -> gs,
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| 43 | GaugeBoson -> G,
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| 44 | StructureConstant -> f,
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| 45 | Representations -> {T,Colour},
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| 46 | SymmetricTensor -> dSUN
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| 47 | }
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| 48 | };
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| 49 |
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| 50 | (* ************************** *)
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| 51 | (* ***** Indices ***** *)
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| 52 | (* ************************** *)
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| 53 | IndexRange[Index[SU2W ]] = Unfold[Range[3]];
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| 54 | IndexRange[Index[SU2D ]] = Unfold[Range[2]];
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| 55 | IndexRange[Index[Gluon ]] = NoUnfold[Range[8]];
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| 56 | IndexRange[Index[Colour ]] = NoUnfold[Range[3]];
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| 57 | IndexRange[Index[Generation]] = Range[3];
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| 58 | IndexStyle[SU2W, j];
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| 59 | IndexStyle[SU2D, k];
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| 60 | IndexStyle[Gluon, a];
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| 61 | IndexStyle[Colour, m];
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| 62 | IndexStyle[Generation, f];
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| 63 |
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| 64 |
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| 65 | (* ************************** *)
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| 66 | (* ***** Orders ***** *)
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| 67 | (* ************************** *)
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| 68 | M$InteractionOrderHierarchy = { {QCD, 1}, {QED, 2}, {NP,2},{HIG,4},{HIW,6}};
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| 69 | M$InteractionOrderLimit = { {QCD, 99}, {QED, 99} , {NP,1}, {HIG,1},{HIW,1}};
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| 70 |
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| 71 |
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| 72 | (* ************************** *)
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| 73 | (* **** Particle classes **** *)
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| 74 | (* ************************** *)
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| 75 | M$ClassesDescription = {
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| 76 |
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| 77 | (* Gauge bosons: physical vector fields *)
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| 78 | V[1] == {
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| 79 | ClassName -> A,
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| 80 | SelfConjugate -> True,
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| 81 | Mass -> 0,
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| 82 | Width -> 0,
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| 83 | ParticleName -> "a",
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| 84 | PDG -> 22,
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| 85 | PropagatorLabel -> "a",
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| 86 | PropagatorType -> W,
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| 87 | PropagatorArrow -> None,
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| 88 | FullName -> "Photon"
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| 89 | },
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| 90 | V[2] == {
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| 91 | ClassName -> Z,
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| 92 | SelfConjugate -> True,
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| 93 | Mass -> {MZ, 91.1876},
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| 94 | Width -> {WZ, 2.4952},
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| 95 | ParticleName -> "Z",
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| 96 | PDG -> 23,
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| 97 | PropagatorLabel -> "Z",
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| 98 | PropagatorType -> Sine,
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| 99 | PropagatorArrow -> None,
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| 100 | FullName -> "Z"
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| 101 | },
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| 102 | V[3] == {
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| 103 | ClassName -> W,
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| 104 | SelfConjugate -> False,
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| 105 | Mass -> {MW, Internal},
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| 106 | Width -> {WW, 2.085},
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| 107 | ParticleName -> "W+",
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| 108 | AntiParticleName -> "W-",
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| 109 | QuantumNumbers -> {Q -> 1},
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| 110 | PDG -> 24,
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| 111 | PropagatorLabel -> "W",
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| 112 | PropagatorType -> Sine,
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| 113 | PropagatorArrow -> Forward,
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| 114 | FullName -> "W"
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| 115 | },
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| 116 | V[4] == {
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| 117 | ClassName -> G,
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| 118 | SelfConjugate -> True,
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| 119 | Indices -> {Index[Gluon]},
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| 120 | Mass -> 0,
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| 121 | Width -> 0,
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| 122 | ParticleName -> "g",
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| 123 | PDG -> 21,
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| 124 | PropagatorLabel -> "G",
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| 125 | PropagatorType -> C,
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| 126 | PropagatorArrow -> None,
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| 127 | FullName -> "G"
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| 128 | },
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| 129 |
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| 130 | (* Ghosts: related to physical gauge bosons *)
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| 131 | U[1] == {
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| 132 | ClassName -> ghA,
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| 133 | SelfConjugate -> False,
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| 134 | Ghost -> A,
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| 135 | QuantumNumbers -> {GhostNumber -> 1},
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| 136 | Mass -> 0,
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| 137 | Width -> 0,
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| 138 | PropagatorLabel -> "uA",
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| 139 | PropagatorType -> GhostDash,
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| 140 | PropagatorArrow -> Forward
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| 141 | },
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| 142 | U[2] == {
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| 143 | ClassName -> ghZ,
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| 144 | SelfConjugate -> False,
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| 145 | Ghost -> Z,
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| 146 | QuantumNumbers -> {GhostNumber -> 1},
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| 147 | Mass -> {MZ, 91.1876},
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| 148 | Width -> {WZ, 2.4952},
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| 149 | PropagatorLabel -> "uZ",
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| 150 | PropagatorType -> GhostDash,
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| 151 | PropagatorArrow -> Forward
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| 152 | },
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| 153 | U[31] == {
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| 154 | ClassName -> ghWp,
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| 155 | SelfConjugate -> False,
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| 156 | Ghost -> W,
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| 157 | QuantumNumbers -> {GhostNumber -> 1, Q -> 1},
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| 158 | Mass -> {MW,Internal},
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| 159 | Width -> {WW, 2.085},
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| 160 | PropagatorLabel -> "uWp",
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| 161 | PropagatorType -> GhostDash,
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| 162 | PropagatorArrow -> Forward
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| 163 | },
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| 164 | U[32] == {
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| 165 | ClassName -> ghWm,
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| 166 | SelfConjugate -> False,
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| 167 | Ghost -> Wbar,
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| 168 | QuantumNumbers -> {GhostNumber -> 1, Q -> -1},
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| 169 | Mass -> {MW,Internal},
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| 170 | Width -> {WW, 2.085},
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| 171 | PropagatorLabel -> "uWm",
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| 172 | PropagatorType -> GhostDash,
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| 173 | PropagatorArrow -> Forward
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| 174 | },
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| 175 | U[4] == {
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| 176 | ClassName -> ghG,
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| 177 | SelfConjugate -> False,
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| 178 | Indices -> {Index[Gluon]},
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| 179 | Ghost -> G,
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| 180 | PDG -> 82,
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| 181 | QuantumNumbers ->{GhostNumber -> 1},
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| 182 | Mass -> 0,
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| 183 | Width -> 0,
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| 184 | PropagatorLabel -> "uG",
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| 185 | PropagatorType -> GhostDash,
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| 186 | PropagatorArrow -> Forward
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| 187 | },
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| 188 |
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| 189 | (* Gauge bosons: unphysical vector fields *)
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| 190 | V[11] == {
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| 191 | ClassName -> B,
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| 192 | Unphysical -> True,
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| 193 | SelfConjugate -> True,
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| 194 | Definitions -> { B[mu_] -> -sw Z[mu] + cw A[mu]}
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| 195 | },
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| 196 | V[12] == {
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| 197 | ClassName -> Wi,
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| 198 | Unphysical -> True,
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| 199 | SelfConjugate -> True,
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| 200 | Indices -> {Index[SU2W]},
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| 201 | FlavorIndex -> SU2W,
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| 202 | Definitions -> {
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| 203 | Wi[mu_,1] -> (Wbar[mu]+W[mu])/Sqrt[2],
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| 204 | Wi[mu_,2] -> (Wbar[mu]-W[mu])/(I*Sqrt[2]),
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| 205 | Wi[mu_,3] -> cw Z[mu] + sw A[mu]}
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| 206 | },
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| 207 |
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| 208 | (* Ghosts: related to unphysical gauge bosons *)
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| 209 | U[11] == {
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| 210 | ClassName -> ghB,
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| 211 | Unphysical -> True,
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| 212 | SelfConjugate -> False,
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| 213 | Ghost -> B,
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| 214 | Definitions -> { ghB -> -sw ghZ + cw ghA}
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| 215 | },
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| 216 | U[12] == {
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| 217 | ClassName -> ghWi,
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| 218 | Unphysical -> True,
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| 219 | SelfConjugate -> False,
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| 220 | Ghost -> Wi,
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| 221 | Indices -> {Index[SU2W]},
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| 222 | FlavorIndex -> SU2W,
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| 223 | Definitions -> { ghWi[1] -> (ghWp+ghWm)/Sqrt[2], ghWi[2] -> (ghWm-ghWp)/(I*Sqrt[2]), ghWi[3] -> cw ghZ+sw ghA}
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| 224 | } ,
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| 225 |
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| 226 | (* Fermions: physical fields *)
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| 227 | F[1] == {
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| 228 | ClassName -> vl,
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| 229 | ClassMembers -> {ve,vm,vt},
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| 230 | Indices -> {Index[Generation]},
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| 231 | FlavorIndex -> Generation,
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| 232 | SelfConjugate -> False,
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| 233 | Mass -> 0,
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| 234 | Width -> 0,
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| 235 | QuantumNumbers -> {LeptonNumber -> 1},
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| 236 | PropagatorLabel -> {"v", "ve", "vm", "vt"} ,
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| 237 | PropagatorType -> S,
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| 238 | PropagatorArrow -> Forward,
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| 239 | PDG -> {12,14,16},
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| 240 | ParticleName -> {"ve","vm","vt"},
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| 241 | AntiParticleName -> {"ve~","vm~","vt~"},
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| 242 | FullName -> {"Electron-neutrino", "Mu-neutrino", "Tau-neutrino"}
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| 243 | },
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| 244 | F[2] == {
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| 245 | ClassName -> l,
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| 246 | ClassMembers -> {e, mu, ta},
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| 247 | Indices -> {Index[Generation]},
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| 248 | FlavorIndex -> Generation,
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| 249 | SelfConjugate -> False,
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| 250 | Mass -> {Ml, {Me,5.11*^-4}, {MMU,0.10566}, {MTA,1.777}},
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| 251 | Width -> 0,
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| 252 | QuantumNumbers -> {Q -> -1, LeptonNumber -> 1},
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| 253 | PropagatorLabel -> {"l", "e", "mu", "ta"},
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| 254 | PropagatorType -> Straight,
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| 255 | PropagatorArrow -> Forward,
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| 256 | PDG -> {11, 13, 15},
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| 257 | ParticleName -> {"e-", "mu-", "ta-"},
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| 258 | AntiParticleName -> {"e+", "mu+", "ta+"},
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| 259 | FullName -> {"Electron", "Muon", "Tau"}
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| 260 | },
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| 261 | F[3] == {
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| 262 | ClassName -> uq,
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| 263 | ClassMembers -> {u, c, t},
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| 264 | Indices -> {Index[Generation], Index[Colour]},
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| 265 | FlavorIndex -> Generation,
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| 266 | SelfConjugate -> False,
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| 267 | Mass -> {Mu, {MU, 2.55*^-3}, {MC,1.27}, {MT,172}},
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| 268 | Width -> {0, 0, {WT,1.50833649}},
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| 269 | QuantumNumbers -> {Q -> 2/3},
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| 270 | PropagatorLabel -> {"uq", "u", "c", "t"},
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| 271 | PropagatorType -> Straight,
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| 272 | PropagatorArrow -> Forward,
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| 273 | PDG -> {2, 4, 6},
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| 274 | ParticleName -> {"u", "c", "t" },
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| 275 | AntiParticleName -> {"u~", "c~", "t~"},
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| 276 | FullName -> {"u-quark", "c-quark", "t-quark"}
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| 277 | },
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| 278 | F[4] == {
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| 279 | ClassName -> dq,
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| 280 | ClassMembers -> {d, s, b},
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| 281 | Indices -> {Index[Generation], Index[Colour]},
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| 282 | FlavorIndex -> Generation,
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| 283 | SelfConjugate -> False,
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| 284 | Mass -> {Md, {MD,5.04*^-3}, {MS,0.101}, {MB,4.7}},
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| 285 | Width -> 0,
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| 286 | QuantumNumbers -> {Q -> -1/3},
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| 287 | PropagatorLabel -> {"dq", "d", "s", "b"},
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| 288 | PropagatorType -> Straight,
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| 289 | PropagatorArrow -> Forward,
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| 290 | PDG -> {1,3,5},
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| 291 | ParticleName -> {"d", "s", "b" },
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| 292 | AntiParticleName -> {"d~", "s~", "b~"},
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| 293 | FullName -> {"d-quark", "s-quark", "b-quark"}
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| 294 | },
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| 295 |
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| 296 | (* Fermions: unphysical fields *)
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| 297 | F[11] == {
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| 298 | ClassName -> LL,
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| 299 | Unphysical -> True,
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| 300 | Indices -> {Index[SU2D], Index[Generation]},
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| 301 | FlavorIndex -> SU2D,
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| 302 | SelfConjugate -> False,
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| 303 | QuantumNumbers -> {Y -> -1/2},
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| 304 | 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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| 305 | },
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| 306 | F[12] == {
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| 307 | ClassName -> lR,
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| 308 | Unphysical -> True,
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| 309 | Indices -> {Index[Generation]},
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| 310 | FlavorIndex -> Generation,
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| 311 | SelfConjugate -> False,
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| 312 | QuantumNumbers -> {Y -> -1},
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| 313 | Definitions -> { lR[sp1_,ff_] :> Module[{sp2}, ProjP[sp1,sp2] l[sp2,ff]] }
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| 314 | },
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| 315 | F[13] == {
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| 316 | ClassName -> QL,
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| 317 | Unphysical -> True,
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| 318 | Indices -> {Index[SU2D], Index[Generation], Index[Colour]},
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| 319 | FlavorIndex -> SU2D,
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| 320 | SelfConjugate -> False,
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| 321 | QuantumNumbers -> {Y -> 1/6},
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| 322 | Definitions -> {
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| 323 | QL[sp1_,1,ff_,cc_] :> Module[{sp2}, ProjM[sp1,sp2] uq[sp2,ff,cc]],
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| 324 | QL[sp1_,2,ff_,cc_] :> Module[{sp2,ff2}, CKM[ff,ff2] ProjM[sp1,sp2] dq[sp2,ff2,cc]] }
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| 325 | },
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| 326 | F[14] == {
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| 327 | ClassName -> uR,
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| 328 | Unphysical -> True,
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| 329 | Indices -> {Index[Generation], Index[Colour]},
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| 330 | FlavorIndex -> Generation,
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| 331 | SelfConjugate -> False,
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| 332 | QuantumNumbers -> {Y -> 2/3},
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| 333 | Definitions -> { uR[sp1_,ff_,cc_] :> Module[{sp2}, ProjP[sp1,sp2] uq[sp2,ff,cc]] }
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| 334 | },
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| 335 | F[15] == {
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| 336 | ClassName -> dR,
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| 337 | Unphysical -> True,
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| 338 | Indices -> {Index[Generation], Index[Colour]},
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| 339 | FlavorIndex -> Generation,
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| 340 | SelfConjugate -> False,
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| 341 | QuantumNumbers -> {Y -> -1/3},
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| 342 | Definitions -> { dR[sp1_,ff_,cc_] :> Module[{sp2}, ProjP[sp1,sp2] dq[sp2,ff,cc]] }
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| 343 | },
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| 344 |
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| 345 | (* Higgs: physical scalars *)
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| 346 | S[1] == {
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| 347 | ClassName -> H,
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| 348 | SelfConjugate -> True,
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| 349 | Mass -> {MH,125},
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| 350 | Width -> {WH,0.00407},
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| 351 | PropagatorLabel -> "H",
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| 352 | PropagatorType -> D,
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| 353 | PropagatorArrow -> None,
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| 354 | PDG -> 25,
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| 355 | ParticleName -> "H",
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| 356 | FullName -> "H"
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| 357 | },
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| 358 |
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| 359 | (* Higgs: physical scalars *)
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| 360 | S[2] == {
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| 361 | ClassName -> G0,
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| 362 | SelfConjugate -> True,
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| 363 | Goldstone -> Z,
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| 364 | Mass -> {MZ, 91.1876},
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| 365 | Width -> {WZ, 2.4952},
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| 366 | PropagatorLabel -> "Go",
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| 367 | PropagatorType -> D,
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| 368 | PropagatorArrow -> None,
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| 369 | PDG -> 250,
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| 370 | ParticleName -> "G0",
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| 371 | FullName -> "G0"
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| 372 | },
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| 373 | S[3] == {
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| 374 | ClassName -> GP,
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| 375 | SelfConjugate -> False,
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| 376 | Goldstone -> W,
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| 377 | Mass -> {MW, Internal},
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| 378 | QuantumNumbers -> {Q -> 1},
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| 379 | Width -> {WW, 2.085},
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| 380 | PropagatorLabel -> "GP",
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| 381 | PropagatorType -> D,
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| 382 | PropagatorArrow -> None,
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| 383 | PDG -> 251,
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| 384 | ParticleName -> "G+",
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| 385 | AntiParticleName -> "G-",
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| 386 | FullName -> "GP"
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| 387 | },
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| 388 |
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| 389 | (* Higgs: unphysical scalars *)
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| 390 | S[11] == {
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| 391 | ClassName -> Phi,
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| 392 | Unphysical -> True,
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| 393 | Indices -> {Index[SU2D]},
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| 394 | FlavorIndex -> SU2D,
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| 395 | SelfConjugate -> False,
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| 396 | QuantumNumbers -> {Y -> 1/2},
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| 397 | Definitions -> { Phi[1] -> -I GP, Phi[2] -> (vev + H + I G0)/Sqrt[2] }
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| 398 | }
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| 399 | };
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| 400 |
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| 401 |
|
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| 402 | (* ************************** *)
|
|---|
| 403 | (* ***** Gauge ***** *)
|
|---|
| 404 | (* ***** Parameters ***** *)
|
|---|
| 405 | (* ***** (FeynArts) ***** *)
|
|---|
| 406 | (* ************************** *)
|
|---|
| 407 |
|
|---|
| 408 | GaugeXi[ V[1] ] = GaugeXi[A];
|
|---|
| 409 | GaugeXi[ V[2] ] = GaugeXi[Z];
|
|---|
| 410 | GaugeXi[ V[3] ] = GaugeXi[W];
|
|---|
| 411 | GaugeXi[ V[4] ] = GaugeXi[G];
|
|---|
| 412 | GaugeXi[ S[1] ] = 1;
|
|---|
| 413 | GaugeXi[ S[2] ] = GaugeXi[Z];
|
|---|
| 414 | GaugeXi[ S[3] ] = GaugeXi[W];
|
|---|
| 415 | GaugeXi[ U[1] ] = GaugeXi[A];
|
|---|
| 416 | GaugeXi[ U[2] ] = GaugeXi[Z];
|
|---|
| 417 | GaugeXi[ U[31] ] = GaugeXi[W];
|
|---|
| 418 | GaugeXi[ U[32] ] = GaugeXi[W];
|
|---|
| 419 | GaugeXi[ U[4] ] = GaugeXi[G];
|
|---|
| 420 |
|
|---|
| 421 |
|
|---|
| 422 | (* ************************** *)
|
|---|
| 423 | (* ***** Parameters ***** *)
|
|---|
| 424 | (* ************************** *)
|
|---|
| 425 | (* The loop coefficients *)
|
|---|
| 426 | sert[x_] := 1+ 7/30 x + 2/21 x^2 + 26/525 x^3;
|
|---|
| 427 | serw[xw_, xt_] := 1 + xw * 66/235 +xw^2 * 228/1645 + xw^3 * 696/8225 +
|
|---|
| 428 | xw^4 * 5248/90475 +xw^5 * 1280/29939+ xw^6 * 54528/1646645-
|
|---|
| 429 | xt * 56/705 - xt^2 * 32/987;
|
|---|
| 430 |
|
|---|
| 431 | M$Parameters = {
|
|---|
| 432 | (* New physics parameters *)
|
|---|
| 433 | NPl == { TeX -> \[CapitalLambda], ParameterType -> External, Value -> 1000, BlockName -> NEWCOUP, OrderBlock -> 0 },
|
|---|
| 434 | cWW == { TeX -> Subscript[C,W], ParameterType -> External, Value -> 0.1, BlockName -> NEWCOUP, OrderBlock -> 1 , InteractionOrder -> {{NP,1},{QED,-1}} },
|
|---|
| 435 | cHW == { TeX -> Subscript[C,HW], ParameterType -> External, Value -> 0.1, BlockName -> NEWCOUP, OrderBlock -> 2 , InteractionOrder -> {{NP,1},{QED,-1}} },
|
|---|
| 436 | cB == { TeX -> Subscript[C,B], ParameterType -> External, Value -> 0.1, BlockName -> NEWCOUP, OrderBlock -> 3, InteractionOrder -> {{NP,1},{QED,-1}} },
|
|---|
| 437 |
|
|---|
| 438 | cHB == { TeX -> Subscript[C,HB],
|
|---|
| 439 | ParameterType -> External,
|
|---|
| 440 | Value -> 0.1,
|
|---|
| 441 | BlockName -> NEWCOUP, OrderBlock -> 4,
|
|---|
| 442 | InteractionOrder -> {{NP,1},{QED,-1}} },
|
|---|
| 443 |
|
|---|
| 444 | cBB == { TeX -> Subscript[C,BB],
|
|---|
| 445 | ParameterType -> External,
|
|---|
| 446 | Value -> 0.1,
|
|---|
| 447 | BlockName -> NEWCOUP, OrderBlock -> 5,
|
|---|
| 448 | InteractionOrder -> {{NP,1},{QED,-1}} },
|
|---|
| 449 |
|
|---|
| 450 | AH == { TeX->Subscript[A,H], ParameterType->Internal, Value -> ee^2/4/Pi/(Pi*vev)*(47/18)(*serw[(MH/2/MW)^2, (MH/2/MT)^2] comment to be consitent with hza*), InteractionOrder -> {HIW, 1}},
|
|---|
| 451 | gZAH == { (*TeX->Subscript[g,ZAH], *)
|
|---|
| 452 | ParameterType->Internal,
|
|---|
| 453 | Value -> Sqrt[aEW Gf MZ^2/(8 Pi Sqrt[2])](94 cw2-13)/(9 Pi vev),
|
|---|
| 454 | InteractionOrder -> {HIW, 1}},
|
|---|
| 455 | GH == { TeX->Subscript[G,H], ParameterType->Internal, Value -> -gs^2/(4Pi(3Pi vev)) (*sert[(MH/2/MT)^2]*), InteractionOrder -> {HIG, 1}},
|
|---|
| 456 |
|
|---|
| 457 | (* External parameters *)
|
|---|
| 458 |
|
|---|
| 459 | aEWM1 == {
|
|---|
| 460 | ParameterType -> External,
|
|---|
| 461 | BlockName -> SMINPUTS,
|
|---|
| 462 | OrderBlock -> 1,
|
|---|
| 463 | Value -> 127.9,
|
|---|
| 464 | InteractionOrder -> {QED,-2},
|
|---|
| 465 | Description -> "Inverse of the EW coupling constant at the Z pole"
|
|---|
| 466 | },
|
|---|
| 467 | Gf == {
|
|---|
| 468 | ParameterType -> External,
|
|---|
| 469 | BlockName -> SMINPUTS,
|
|---|
| 470 | OrderBlock -> 2,
|
|---|
| 471 | Value -> 1.16637*^-5,
|
|---|
| 472 | InteractionOrder -> {QED,2},
|
|---|
| 473 | TeX -> Subscript[G,f],
|
|---|
| 474 | Description -> "Fermi constant"
|
|---|
| 475 | },
|
|---|
| 476 | aS == {
|
|---|
| 477 | ParameterType -> External,
|
|---|
| 478 | BlockName -> SMINPUTS,
|
|---|
| 479 | OrderBlock -> 3,
|
|---|
| 480 | Value -> 0.1184,
|
|---|
| 481 | InteractionOrder -> {QCD,2},
|
|---|
| 482 | TeX -> Subscript[\[Alpha],s],
|
|---|
| 483 | Description -> "Strong coupling constant at the Z pole"
|
|---|
| 484 | },
|
|---|
| 485 | ymdo == {
|
|---|
| 486 | ParameterType -> External,
|
|---|
| 487 | BlockName -> YUKAWA,
|
|---|
| 488 | OrderBlock -> 1,
|
|---|
| 489 | Value -> 5.04*^-3,
|
|---|
| 490 | Description -> "Down Yukawa mass"
|
|---|
| 491 | },
|
|---|
| 492 | ymup == {
|
|---|
| 493 | ParameterType -> External,
|
|---|
| 494 | BlockName -> YUKAWA,
|
|---|
| 495 | OrderBlock -> 2,
|
|---|
| 496 | Value -> 2.55*^-3,
|
|---|
| 497 | Description -> "Up Yukawa mass"
|
|---|
| 498 | },
|
|---|
| 499 | yms == {
|
|---|
| 500 | ParameterType -> External,
|
|---|
| 501 | BlockName -> YUKAWA,
|
|---|
| 502 | OrderBlock -> 3,
|
|---|
| 503 | Value -> 0.101,
|
|---|
| 504 | Description -> "Strange Yukawa mass"
|
|---|
| 505 | },
|
|---|
| 506 | ymc == {
|
|---|
| 507 | ParameterType -> External,
|
|---|
| 508 | BlockName -> YUKAWA,
|
|---|
| 509 | OrderBlock -> 4,
|
|---|
| 510 | Value -> 1.27,
|
|---|
| 511 | Description -> "Charm Yukawa mass"
|
|---|
| 512 | },
|
|---|
| 513 | ymb == {
|
|---|
| 514 | ParameterType -> External,
|
|---|
| 515 | BlockName -> YUKAWA,
|
|---|
| 516 | OrderBlock -> 5,
|
|---|
| 517 | Value -> 4.7,
|
|---|
| 518 | Description -> "Bottom Yukawa mass"
|
|---|
| 519 | },
|
|---|
| 520 | ymt == {
|
|---|
| 521 | ParameterType -> External,
|
|---|
| 522 | BlockName -> YUKAWA,
|
|---|
| 523 | OrderBlock -> 6,
|
|---|
| 524 | Value -> 172,
|
|---|
| 525 | Description -> "Top Yukawa mass"
|
|---|
| 526 | },
|
|---|
| 527 | yme == {
|
|---|
| 528 | ParameterType -> External,
|
|---|
| 529 | BlockName -> YUKAWA,
|
|---|
| 530 | OrderBlock -> 11,
|
|---|
| 531 | Value -> 5.11*^-4,
|
|---|
| 532 | Description -> "Electron Yukawa mass"
|
|---|
| 533 | },
|
|---|
| 534 | ymm == {
|
|---|
| 535 | ParameterType -> External,
|
|---|
| 536 | BlockName -> YUKAWA,
|
|---|
| 537 | OrderBlock -> 13,
|
|---|
| 538 | Value -> 0.10566,
|
|---|
| 539 | Description -> "Muon Yukawa mass"
|
|---|
| 540 | },
|
|---|
| 541 | ymtau == {
|
|---|
| 542 | ParameterType -> External,
|
|---|
| 543 | BlockName -> YUKAWA,
|
|---|
| 544 | OrderBlock -> 15,
|
|---|
| 545 | Value -> 1.777,
|
|---|
| 546 | Description -> "Tau Yukawa mass"
|
|---|
| 547 | },
|
|---|
| 548 | cabi == {
|
|---|
| 549 | ParameterType -> External,
|
|---|
| 550 | BlockName -> CKMBLOCK,
|
|---|
| 551 | OrderBlock -> 1,
|
|---|
| 552 | Value -> 0.227736,
|
|---|
| 553 | TeX -> Subscript[\[Theta], c],
|
|---|
| 554 | Description -> "Cabibbo angle"
|
|---|
| 555 | },
|
|---|
| 556 |
|
|---|
| 557 | (* Internal Parameters *)
|
|---|
| 558 | aEW == {
|
|---|
| 559 | ParameterType -> Internal,
|
|---|
| 560 | Value -> 1/aEWM1,
|
|---|
| 561 | InteractionOrder -> {QED,2},
|
|---|
| 562 | TeX -> Subscript[\[Alpha], EW],
|
|---|
| 563 | Description -> "Electroweak coupling constant"
|
|---|
| 564 | },
|
|---|
| 565 |
|
|---|
| 566 | vev == {
|
|---|
| 567 | ParameterType -> Internal,
|
|---|
| 568 | Value -> Sqrt[1/(Sqrt[2] Gf)],
|
|---|
| 569 | InteractionOrder -> {QED,-1},
|
|---|
| 570 | Description -> "Higgs vacuum expectation value"
|
|---|
| 571 | },
|
|---|
| 572 |
|
|---|
| 573 | ee == {
|
|---|
| 574 | ParameterType -> Internal,
|
|---|
| 575 | Value -> Sqrt[4 Pi aEW] (1+cWW Pi aEW vev^2/2 /NPl^2 ),
|
|---|
| 576 | InteractionOrder -> {QED,1},
|
|---|
| 577 | TeX -> e,
|
|---|
| 578 | Description -> "Electric coupling constant"
|
|---|
| 579 | },
|
|---|
| 580 |
|
|---|
| 581 | cw2 == {
|
|---|
| 582 | ParameterType -> Internal,
|
|---|
| 583 | Value ->(MZ^2*(8*NPl^2 - 4*cB*ee^2*vev^2) + 4*MZ*Sqrt[(MZ - ee*vev)*(MZ + ee*vev)]*(2*NPl^2 + cB*ee^2*vev^2) - ee^2*vev^2*(8*NPl^2 + cWW*ee^2*vev^2))/ (16*MZ*NPl^2*Sqrt[(MZ - ee*vev)*(MZ + ee*vev)])
|
|---|
| 584 | },
|
|---|
| 585 |
|
|---|
| 586 | cw == {
|
|---|
| 587 | ParameterType -> Internal,
|
|---|
| 588 | Value -> Sqrt[cw2],
|
|---|
| 589 | TeX -> Subscript[c,w],
|
|---|
| 590 | Description -> "Cosine of the Weinberg angle"
|
|---|
| 591 | },
|
|---|
| 592 | sw2 == {
|
|---|
| 593 | ParameterType -> Internal,
|
|---|
| 594 | Value -> 1-(cw)^2,
|
|---|
| 595 | Description -> "Squared Sin of the Weinberg angle"
|
|---|
| 596 | },
|
|---|
| 597 |
|
|---|
| 598 | sw == {
|
|---|
| 599 | ParameterType -> Internal,
|
|---|
| 600 | Value -> Sqrt[sw2],
|
|---|
| 601 | TeX -> Subscript[s,w],
|
|---|
| 602 | Description -> "Sine of the Weinberg angle"
|
|---|
| 603 | },
|
|---|
| 604 |
|
|---|
| 605 | MW == {
|
|---|
| 606 | ParameterType -> Internal,
|
|---|
| 607 | Value -> (ee*vev)/(2*sw) ,
|
|---|
| 608 | TeX -> Subscript[M,W],
|
|---|
| 609 | Description -> "W mass"
|
|---|
| 610 | },
|
|---|
| 611 | gw == {
|
|---|
| 612 | ParameterType -> Internal,
|
|---|
| 613 | Definitions -> {gw->ee/sw/(1 + ( cWW ee^2/sw^2 vev^2)/(8 NPl^2))},
|
|---|
| 614 | InteractionOrder -> {QED,1},
|
|---|
| 615 | TeX -> Subscript[g,w],
|
|---|
| 616 | Description -> "Weak coupling constant at the Z pole"
|
|---|
| 617 | },
|
|---|
| 618 | g1 == {
|
|---|
| 619 | ParameterType -> Internal,
|
|---|
| 620 | Definitions -> {g1->1/(1 + (cBB ee^2 vev^2)/(4 NPl^2 cw^2) )ee/cw},
|
|---|
| 621 | InteractionOrder -> {QED,1},
|
|---|
| 622 | TeX -> Subscript[g,1],
|
|---|
| 623 | Description -> "U(1)Y coupling constant at the Z pole"
|
|---|
| 624 | },
|
|---|
| 625 | gs == {
|
|---|
| 626 | ParameterType -> Internal,
|
|---|
| 627 | Value -> Sqrt[4 Pi aS],
|
|---|
| 628 | InteractionOrder -> {QCD,1},
|
|---|
| 629 | TeX -> Subscript[g,s],
|
|---|
| 630 | ParameterName -> G,
|
|---|
| 631 | Description -> "Strong coupling constant at the Z pole"
|
|---|
| 632 | },
|
|---|
| 633 | lam == {
|
|---|
| 634 | ParameterType -> Internal,
|
|---|
| 635 | Value -> MH^2/(2*vev^2),
|
|---|
| 636 | InteractionOrder -> {QED, 2},
|
|---|
| 637 | Description -> "Higgs quartic coupling"
|
|---|
| 638 | },
|
|---|
| 639 | muH == {
|
|---|
| 640 | ParameterType -> Internal,
|
|---|
| 641 | Value -> Sqrt[vev^2 lam],
|
|---|
| 642 | TeX -> \[Mu],
|
|---|
| 643 | Description -> "Coefficient of the quadratic piece of the Higgs potential"
|
|---|
| 644 | },
|
|---|
| 645 | yl == {
|
|---|
| 646 | ParameterType -> Internal,
|
|---|
| 647 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 648 | Definitions -> {yl[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 649 | Value -> {yl[1,1] -> Sqrt[2] yme / vev, yl[2,2] -> Sqrt[2] ymm / vev, yl[3,3] -> Sqrt[2] ymtau / vev},
|
|---|
| 650 | InteractionOrder -> {QED, 1},
|
|---|
| 651 | ParameterName -> {yl[1,1] -> ye, yl[2,2] -> ym, yl[3,3] -> ytau},
|
|---|
| 652 | TeX -> Superscript[y, l],
|
|---|
| 653 | Description -> "Lepton Yukawa couplings"
|
|---|
| 654 | },
|
|---|
| 655 | yu == {
|
|---|
| 656 | ParameterType -> Internal,
|
|---|
| 657 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 658 | Definitions -> {yu[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 659 | Value -> {yu[1,1] -> Sqrt[2] ymup/vev, yu[2,2] -> Sqrt[2] ymc/vev, yu[3,3] -> Sqrt[2] ymt/vev},
|
|---|
| 660 | InteractionOrder -> {QED, 1},
|
|---|
| 661 | ParameterName -> {yu[1,1] -> yup, yu[2,2] -> yc, yu[3,3] -> yt},
|
|---|
| 662 | TeX -> Superscript[y, u],
|
|---|
| 663 | Description -> "Up-type Yukawa couplings"
|
|---|
| 664 | },
|
|---|
| 665 | yd == {
|
|---|
| 666 | ParameterType -> Internal,
|
|---|
| 667 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 668 | Definitions -> {yd[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 669 | Value -> {yd[1,1] -> Sqrt[2] ymdo/vev, yd[2,2] -> Sqrt[2] yms/vev, yd[3,3] -> Sqrt[2] ymb/vev},
|
|---|
| 670 | InteractionOrder -> {QED, 1},
|
|---|
| 671 | ParameterName -> {yd[1,1] -> ydo, yd[2,2] -> ys, yd[3,3] -> yb},
|
|---|
| 672 | TeX -> Superscript[y, d],
|
|---|
| 673 | Description -> "Down-type Yukawa couplings"
|
|---|
| 674 | },
|
|---|
| 675 | (* N. B. : only Cabibbo mixing! *)
|
|---|
| 676 | CKM == {
|
|---|
| 677 | ParameterType -> Internal,
|
|---|
| 678 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 679 | Unitary -> True,
|
|---|
| 680 | Value -> {CKM[1,1] -> Cos[cabi], CKM[1,2] -> Sin[cabi], CKM[1,3] -> 0,
|
|---|
| 681 | CKM[2,1] -> -Sin[cabi], CKM[2,2] -> Cos[cabi], CKM[2,3] -> 0,
|
|---|
| 682 | CKM[3,1] -> 0, CKM[3,2] -> 0, CKM[3,3] -> 1},
|
|---|
| 683 | TeX -> Superscript[V,CKM],
|
|---|
| 684 | Description -> "CKM-Matrix"}
|
|---|
| 685 |
|
|---|
| 686 | };
|
|---|
| 687 |
|
|---|
| 688 | (* ************************** *)
|
|---|
| 689 | (* ***** Lagrangian ***** *)
|
|---|
| 690 | (* ************************** *)
|
|---|
| 691 |
|
|---|
| 692 |
|
|---|
| 693 | LGauge := Block[{mu,nu,ii,aa},
|
|---|
| 694 | 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]];
|
|---|
| 695 |
|
|---|
| 696 | LFermions := Block[{mu},
|
|---|
| 697 | ExpandIndices[I*(
|
|---|
| 698 | 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]),
|
|---|
| 699 | FlavorExpand->{SU2W,SU2D}]/.{CKM[a_,b_] Conjugate[CKM[a_,c_]]->IndexDelta[b,c], CKM[b_,a_] Conjugate[CKM[c_,a_]]->IndexDelta[b,c]}];
|
|---|
| 700 |
|
|---|
| 701 | LHiggs := Block[{ii,mu, feynmangaugerules},
|
|---|
| 702 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar ->0}, {}];
|
|---|
| 703 |
|
|---|
| 704 | 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
|
|---|
| 705 | ];
|
|---|
| 706 |
|
|---|
| 707 | LYukawa := Block[{sp,ii,jj,cc,ff1,ff2,ff3,yuk,feynmangaugerules},
|
|---|
| 708 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar ->0}, {}];
|
|---|
| 709 |
|
|---|
| 710 | yuk = ExpandIndices[
|
|---|
| 711 | -yd[ff2, ff3] CKM[ff1, ff2] QLbar[sp, ii, ff1, cc].dR [sp, ff3, cc] Phi[ii] -
|
|---|
| 712 | yl[ff1, ff3] LLbar[sp, ii, ff1].lR [sp, ff3] Phi[ii] -
|
|---|
| 713 | yu[ff1, ff2] QLbar[sp, ii, ff1, cc].uR [sp, ff2, cc] Phibar[jj] Eps[ii, jj], FlavorExpand -> SU2D];
|
|---|
| 714 | yuk = yuk /. { CKM[a_, b_] Conjugate[CKM[a_, c_]] -> IndexDelta[b, c], CKM[b_, a_] Conjugate[CKM[c_, a_]] -> IndexDelta[b, c]};
|
|---|
| 715 | yuk+HC[yuk]/.feynmangaugerules
|
|---|
| 716 | ];
|
|---|
| 717 |
|
|---|
| 718 | LGhost := Block[{LGh1,LGhw,LGhs,LGhphi,mu, generators,gh,ghbar,Vectorize,phi1,phi2,togoldstones,doublet,doublet0},
|
|---|
| 719 | (* Pure gauge piece *)
|
|---|
| 720 | LGh1 = -ghBbar.del[DC[ghB,mu],mu];
|
|---|
| 721 | LGhw = -ghWibar.del[DC[ghWi,mu],mu];
|
|---|
| 722 | LGhs = -ghGbar.del[DC[ghG,mu],mu];
|
|---|
| 723 |
|
|---|
| 724 | (* Scalar pieces: see Peskin pages 739-742 *)
|
|---|
| 725 | (* phi1 and phi2 are the real degrees of freedom of GP *)
|
|---|
| 726 | (* Vectorize transforms a doublet in a vector in the phi-basis, i.e. the basis of real degrees of freedom *)
|
|---|
| 727 | gh = {ghB, ghWi[1], ghWi[2], ghWi[3]};
|
|---|
| 728 | ghbar = {ghBbar, ghWibar[1], ghWibar[2], ghWibar[3]};
|
|---|
| 729 | generators = {-I/2 g1 IdentityMatrix[2], -I/2 gw PauliSigma[1], -I/2 gw PauliSigma[2], -I/2 gw PauliSigma[3]};
|
|---|
| 730 | doublet = Expand[{(-I phi1 - phi2)/Sqrt[2], Phi[2]} /. MR$Definitions /. vev -> 0];
|
|---|
| 731 | doublet0 = {0, vev/Sqrt[2]};
|
|---|
| 732 | 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}];
|
|---|
| 733 | togoldstones := {phi1 -> (GP + GPbar)/Sqrt[2], phi2 -> (-GP + GPbar)/(I Sqrt[2])};
|
|---|
| 734 | 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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| 735 |
|
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| 736 | ExpandIndices[ LGhs + If[FeynmanGauge, LGh1 + LGhw + LGhphi,0], FlavorExpand->SU2W]];
|
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| 737 |
|
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| 738 | LSM:= LGauge + LFermions + LHiggs + LYukawa + LGhost;
|
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| 739 |
|
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| 740 | Wvec[mu_,nu_,ii_,jj_]:= Module[{aa},Ta[aa,ii,jj] FS[Wi,mu,nu,aa]];
|
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| 741 |
|
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| 742 | LSILH := Block[{ii,jj,mu,nu, OW, OB, OHW, OHBi, OBB},
|
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| 743 |
|
|---|
| 744 | OW = I cWW gw/2 (Phibar[ii] DC[Phi[jj],mu] - DC[Phibar[ii],mu] Phi[jj]) DC[Wvec[mu,nu,ii,jj],nu];
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| 745 | OB = I cB g1/2 (Phibar[ii] DC[Phi[ii],mu] - DC[Phibar[ii],mu] Phi[ii]) del[FS[B,mu,nu],nu];
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| 746 | OHW= I cHW gw DC[Phibar[ii],mu] DC[Phi[jj],nu] Wvec[mu,nu,ii,jj];
|
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| 747 | OHB= I cHB g1 DC[Phibar[ii],mu] DC[Phi[ii],nu] FS[B,mu,nu];
|
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| 748 | OBB= cBB g1^2/4 Phibar[ii] Phi[ii] FS[B,mu,nu] FS[B,mu,nu];
|
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| 749 |
|
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| 750 | 1/NPl^2 (OW+OB+OHB+OHW+OBB)
|
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| 751 | ];
|
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| 752 |
|
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| 753 | RedefineSMP[lag_]:=Block[{mylag},
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| 754 | mylag := ExpandIndices[lag,FlavorExpand->{SU2D,SU2W}];
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| 755 | (* Field redefinitions *)
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| 756 | mylag = mylag/. {A[mu_] :> A[mu] (1 + ( cBB g1^2 cw^2 vev^2)/(4 NPl^2)) -
|
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| 757 | Z[mu] ((2* cB*cw^2*g1^2 + (2*cBB*cw^2*g1^2 - (1-cw^2) cWW*gw^2)*sw^2)*vev^2)/(8*cw*NPl^2*sw),
|
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| 758 | Z[mu_] :> Z[mu] (1 + ( cWW gw^2 vev^2)/(8 NPl^2) + (cB g1^2 vev^2)/(4 NPl^2) + (cBB g1^2 sw^2 vev^2)/(4 NPl^2)) -
|
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| 759 | A[mu] ((2* cB *cw^2*g1^2 0 + (2*cBB*cw^2*g1^2 - cw^2 cWW*gw^2)*sw^2)*vev^2)/(8*cw*NPl^2*sw),
|
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| 760 | W[mu_] -> W[mu] (1 + (cWW gw^2 vev^2)/(8 NPl^2)),
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| 761 | Wbar[mu_] -> Wbar[mu] (1 + (cWW gw^2 vev^2)/(8 NPl^2))}//.MR$Definitions(*for g1 before series and the other ???*);
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| 762 | (Normal[Series[#,{NPl,Infinity,2}]]&)/@ mylag
|
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| 763 | ];
|
|---|
| 764 |
|
|---|
| 765 | LLOPP := -1/4 GH FS[G, mu, nu, b] FS[G, mu, nu, b] H (1-0*H/(2 vev)) - 1/4 AH FS[A, mu, nu] FS[A, mu, nu] H- 1/2 gZAH FS[Z, mu, nu] FS[A, mu, nu] H;
|
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| 766 |
|
|---|
| 767 | Lag:=RedefineSMP[LSM+LSILH] + LLOPP;
|
|---|
| 768 |
|
|---|
| 769 |
|
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