| 1 | (***************************************************************************************************************)
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| 2 | (****** This is the FeynRules mod-file for the 4th generation model ******)
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| 3 | (****** ******)
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| 4 | (****** Authors: C. Duhr ******)
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| 5 | (****** ******)
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| 6 | (****** Choose whether Feynman gauge is desired. ******)
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| 7 | (****** If set to False, unitary gauge is assumed. ****)
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| 8 | (****** Feynman gauge is especially useful for CalcHEP/CompHEP where the calculation is 10-100 times faster. ***)
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| 9 | (****** Feynman gauge is not supported in MadGraph and Sherpa. ****)
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| 10 | (***************************************************************************************************************)
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| 11 |
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| 12 |
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| 13 | (*
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| 14 | This model is based on the SM implmentation of FeynRules,
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| 15 | and basically obtained by just increasing the range of the Index of type Generation from 3 to 4
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| 16 | *)
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| 17 |
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| 18 |
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| 19 |
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| 20 | M$ModelName = "4th_Generation_Complex_CKM";
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| 21 |
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| 22 |
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| 23 |
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| 24 | M$Information = {Authors -> {"C. Duhr"},
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| 25 | Version -> "1.1",
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| 26 | Date -> "02. 11. 2010",
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| 27 | Institutions -> {"IPPP, Durham"},
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| 28 | Emails -> {"claude.duhr@durham.ac.uk"}};
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| 29 |
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| 30 | (*V1.1 - Fixed yukawa couplings in Feynman gauge.
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| 31 | Changed yd[n] CKM[n,m] to yd[m] CKM[n,m].
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| 32 | Changed yu[n] Conjugate[CKM[m,n]] to yu[m] Conjugate[CKM[m,n]].
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| 33 | *)
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| 34 |
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| 35 | FeynmanGauge = False;
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| 36 |
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| 37 |
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| 38 | (******* Index definitions ********)
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| 39 |
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| 40 | IndexRange[ Index[Generation] ] = Range[3]
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| 41 |
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| 42 | IndexRange[ Index[QuarkGeneration] ] = Range[4]
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| 43 |
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| 44 | IndexRange[ Index[Colour] ] = NoUnfold[Range[3]]
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| 45 |
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| 46 | IndexRange[ Index[Gluon] ] = NoUnfold[Range[8]]
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| 47 |
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| 48 | IndexRange[ Index[SU2W] ] = Unfold[Range[3]]
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| 49 |
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| 50 |
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| 51 | IndexStyle[Colour, i]
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| 52 |
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| 53 | IndexStyle[Generation, f]
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| 54 |
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| 55 | IndexStyle[QuarkGeneration, q]
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| 56 |
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| 57 | IndexStyle[Gluon ,a]
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| 58 |
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| 59 | IndexStyle[SU2W ,k]
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| 60 |
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| 61 |
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| 62 | (******* Gauge parameters (for FeynArts) ********)
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| 63 |
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| 64 | GaugeXi[ V[1] ] = GaugeXi[A];
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| 65 | GaugeXi[ V[2] ] = GaugeXi[Z];
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| 66 | GaugeXi[ V[3] ] = GaugeXi[W];
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| 67 | GaugeXi[ V[4] ] = GaugeXi[G];
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| 68 | GaugeXi[ S[1] ] = 1;
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| 69 | GaugeXi[ S[2] ] = GaugeXi[Z];
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| 70 | GaugeXi[ S[3] ] = GaugeXi[W];
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| 71 | GaugeXi[ U[1] ] = GaugeXi[A];
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| 72 | GaugeXi[ U[2] ] = GaugeXi[Z];
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| 73 | GaugeXi[ U[31] ] = GaugeXi[W];
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| 74 | GaugeXi[ U[32] ] = GaugeXi[W];
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| 75 | GaugeXi[ U[4] ] = GaugeXi[G];
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| 76 |
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| 77 |
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| 78 | (**************** Parameters *************)
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| 79 |
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| 80 | M$Parameters = {
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| 81 |
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| 82 | (* External parameters *)
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| 83 |
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| 84 | \[Alpha]EWM1== {
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| 85 | ParameterType -> External,
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| 86 | BlockName -> SMINPUTS,
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| 87 | ParameterName -> aEWM1,
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| 88 | InteractionOrder -> {QED, -2},
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| 89 | Value -> 127.9,
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| 90 | Description -> "Inverse of the electroweak coupling constant"},
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| 91 |
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| 92 | Gf == {
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| 93 | ParameterType -> External,
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| 94 | BlockName -> SMINPUTS,
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| 95 | TeX -> Subscript[G, f],
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| 96 | InteractionOrder -> {QED, 2},
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| 97 | Value -> 1.16639 * 10^(-5),
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| 98 | Description -> "Fermi constant"},
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| 99 |
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| 100 | \[Alpha]S == {
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| 101 | ParameterType -> External,
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| 102 | BlockName -> SMINPUTS,
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| 103 | TeX -> Subscript[\[Alpha], s],
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| 104 | ParameterName -> aS,
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| 105 | InteractionOrder -> {QCD, 2},
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| 106 | Value -> 0.1172,
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| 107 | Description -> "Strong coupling constant at the Z pole."},
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| 108 |
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| 109 |
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| 110 | ymc == {
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| 111 | ParameterType -> External,
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| 112 | BlockName -> YUKAWA,
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| 113 | Value -> 1.42,
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| 114 | OrderBlock -> {4},
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| 115 | Description -> "Charm Yukawa mass"},
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| 116 |
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| 117 | ymb == {
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| 118 | ParameterType -> External,
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| 119 | BlockName -> YUKAWA,
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| 120 | Value -> 4.7,
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| 121 | OrderBlock -> {5},
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| 122 | Description -> "Bottom Yukawa mass"},
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| 123 |
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| 124 | ymbp == {
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| 125 | ParameterType -> External,
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| 126 | BlockName -> YUKAWA,
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| 127 | Value -> 500,
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| 128 | OrderBlock -> {7},
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| 129 | Description -> "Bottom-prime Yukawa mass"},
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| 130 |
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| 131 | ymt == {
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| 132 | ParameterType -> External,
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| 133 | BlockName -> YUKAWA,
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| 134 | Value -> 174.3,
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| 135 | OrderBlock -> {6},
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| 136 | Description -> "Top Yukawa mass"},
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| 137 |
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| 138 | ymtp == {
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| 139 | ParameterType -> External,
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| 140 | BlockName -> YUKAWA,
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| 141 | Value -> 700,
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| 142 | OrderBlock -> {8},
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| 143 | Description -> "Top-prime Yukawa mass"},
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| 144 |
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| 145 | ymtau == {
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| 146 | ParameterType -> External,
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| 147 | BlockName -> YUKAWA,
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| 148 | Value -> 1.777,
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| 149 | OrderBlock -> {15},
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| 150 | Description -> "Tau Yukawa mass"},
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| 151 |
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| 152 |
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| 153 | (* Internal Parameters *)
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| 154 |
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| 155 | \[Alpha]EW == {
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| 156 | ParameterType -> Internal,
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| 157 | Value -> 1/\[Alpha]EWM1,
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| 158 | TeX -> Subscript[\[Alpha], EW],
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| 159 | ParameterName -> aEW,
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| 160 | InteractionOrder -> {QED, 2},
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| 161 | Description -> "Electroweak coupling contant"},
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| 162 |
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| 163 |
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| 164 | MW == {
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| 165 | ParameterType -> Internal,
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| 166 | Value -> Sqrt[MZ^2/2+Sqrt[MZ^4/4-Pi/Sqrt[2]*\[Alpha]EW/Gf*MZ^2]],
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| 167 | TeX -> Subscript[M, W],
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| 168 | Description -> "W mass"},
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| 169 |
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| 170 | sw2 == {
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| 171 | ParameterType -> Internal,
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| 172 | Value -> 1-(MW/MZ)^2,
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| 173 | Description -> "Squared Sin of the Weinberg angle"},
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| 174 |
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| 175 | ee == {
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| 176 | TeX -> e,
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| 177 | ParameterType -> Internal,
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| 178 | Value -> Sqrt[4 Pi \[Alpha]EW],
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| 179 | InteractionOrder -> {QED, 1},
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| 180 | Description -> "Electric coupling constant"},
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| 181 |
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| 182 | cw == {
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| 183 | TeX -> Subscript[c, w],
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| 184 | ParameterType -> Internal,
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| 185 | Value -> Sqrt[1 - sw2],
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| 186 | Description -> "Cos of the Weinberg angle"},
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| 187 |
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| 188 | sw == {
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| 189 | TeX -> Subscript[s, w],
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| 190 | ParameterType -> Internal,
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| 191 | Value -> Sqrt[sw2],
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| 192 | Description -> "Sin of the Weinberg angle"},
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| 193 |
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| 194 | gw == {
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| 195 | TeX -> Subscript[g, w],
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| 196 | ParameterType -> Internal,
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| 197 | Value -> ee / sw,
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| 198 | InteractionOrder -> {QED, 1},
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| 199 | Description -> "Weak coupling constant"},
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| 200 |
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| 201 | g1 == {
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| 202 | TeX -> Subscript[g, 1],
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| 203 | ParameterType -> Internal,
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| 204 | Value -> ee / cw,
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| 205 | InteractionOrder -> {QED, 1},
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| 206 | Description -> "U(1)Y coupling constant"},
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| 207 |
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| 208 | gs == {
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| 209 | TeX -> Subscript[g, s],
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| 210 | ParameterType -> Internal,
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| 211 | Value -> Sqrt[4 Pi \[Alpha]S],
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| 212 | InteractionOrder -> {QCD, 1},
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| 213 | ParameterName -> G,
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| 214 | Description -> "Strong coupling constant"},
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| 215 |
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| 216 |
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| 217 | v == {
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| 218 | ParameterType -> Internal,
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| 219 | Value -> 2*MW*sw/ee,
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| 220 | InteractionOrder -> {QED, -1},
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| 221 | Description -> "Higgs VEV"},
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| 222 |
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| 223 | \[Lambda] == {
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| 224 | ParameterType -> Internal,
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| 225 | Value -> MH^2/(2*v^2),
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| 226 | InteractionOrder -> {QED, 2},
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| 227 | ParameterName -> lam,
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| 228 | Description -> "Higgs quartic coupling"},
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| 229 |
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| 230 | muH == {
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| 231 | ParameterType -> Internal,
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| 232 | Value -> Sqrt[v^2 \[Lambda]],
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| 233 | TeX -> \[Mu],
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| 234 | Description -> "Coefficient of the quadratic piece of the Higgs potential"},
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| 235 |
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| 236 |
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| 237 | yl == {
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| 238 | TeX -> Superscript[y, l],
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| 239 | Indices -> {Index[Generation]},
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| 240 | AllowSummation -> True,
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| 241 | ParameterType -> Internal,
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| 242 | Value -> {yl[1] -> 0, yl[2] -> 0, yl[3] -> Sqrt[2] ymtau / v},
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| 243 | ParameterName -> {yl[1] -> ye, yl[2] -> ym, yl[3] -> ytau},
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| 244 | InteractionOrder -> {QED, 1},
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| 245 | ComplexParameter -> False,
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| 246 | Description -> "Lepton Yukawa coupling"},
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| 247 |
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| 248 | yu == {
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| 249 | TeX -> Superscript[y, u],
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| 250 | Indices -> {Index[QuarkGeneration]},
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| 251 | AllowSummation -> True,
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| 252 | ParameterType -> Internal,
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| 253 | Value -> {yu[1] -> 0, yu[2] -> Sqrt[2] ymc / v, yu[3] -> Sqrt[2] ymt / v, yu[4] -> Sqrt[2] ymtp / v},
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| 254 | ParameterName -> {yu[1] -> yup, yu[2] -> yc, yu[3] -> yt, yu[4] -> ytp},
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| 255 | InteractionOrder -> {QED, 1},
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| 256 | ComplexParameter -> False,
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| 257 | Description -> "U-quark Yukawa coupling"},
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| 258 |
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| 259 | yd == {
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| 260 | TeX -> Superscript[y, d],
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| 261 | Indices -> {Index[QuarkGeneration]},
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| 262 | AllowSummation -> True,
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| 263 | ParameterType -> Internal,
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| 264 | Value -> {yd[1] -> 0, yd[2] -> 0, yd[3] -> Sqrt[2] ymb / v, yd[4] -> Sqrt[2] ymbp / v},
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| 265 | ParameterName -> {yd[1] -> ydo, yd[2] -> ys, yd[3] -> yb, yd[4] -> ybp},
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| 266 | InteractionOrder -> {QED, 1},
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| 267 | ComplexParameter -> False,
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| 268 | Description -> "D-quark Yukawa coupling"},
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| 269 |
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| 270 | (* N. B. : only Cabibbo mixing! *)
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| 271 |
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| 272 |
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| 273 |
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| 274 | RCKM == {
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| 275 | ParameterType -> External,
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| 276 | Indices -> {Index[QuarkGeneration], Index[QuarkGeneration]},
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| 277 | BlockName -> RCKM,
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| 278 | ComplexParameter -> False,
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| 279 | Value -> {RCKM[1,1] :> 1,
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| 280 | RCKM[1,2] :> 0,
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| 281 | RCKM[1,3] :> 0,
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| 282 | RCKM[1,4] :> 0,
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| 283 | RCKM[2,1] :> 0,
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| 284 | RCKM[2,2] :> 0.99995,
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| 285 | RCKM[2,3] :> 0,
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| 286 | RCKM[2,4] :> 0.01,
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| 287 | RCKM[3,1] :> 0,
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| 288 | RCKM[3,2] :> -0.001,
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| 289 | RCKM[3,3] :> 0.995,
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| 290 | RCKM[3,4] :> 0.1,
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| 291 | RCKM[4,1] :> 0,
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| 292 | RCKM[4,2] :> -0.01,
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| 293 | RCKM[4,3] :> -0.1,
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| 294 | RCKM[4,4] :> 0.99495},
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| 295 | Description -> "Real Part of the CKM matrix"},
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| 296 |
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| 297 | ICKM == {
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| 298 | ParameterType -> External,
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| 299 | Indices -> {Index[QuarkGeneration], Index[QuarkGeneration]},
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| 300 | BlockName -> ICKM,
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| 301 | ComplexParameter -> False,
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| 302 | Value -> {ICKM[1,1] :> 0,
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| 303 | ICKM[1,2] :> 0,
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| 304 | ICKM[1,3] :> 0,
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| 305 | ICKM[1,4] :> 0,
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| 306 | ICKM[2,1] :> 0,
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| 307 | ICKM[2,2] :> 0,
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| 308 | ICKM[2,3] :> 0,
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| 309 | ICKM[2,4] :> 0,
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| 310 | ICKM[3,1] :> 0,
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| 311 | ICKM[3,2] :> 0,
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| 312 | ICKM[3,3] :> 0,
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| 313 | ICKM[3,4] :> 0,
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| 314 | ICKM[4,1] :> 0,
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| 315 | ICKM[4,2] :> 0,
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| 316 | ICKM[4,3] :> 0,
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| 317 | ICKM[4,4] :> 0},
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| 318 | Description -> "Imaginary Part of the CKM matrix"},
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| 319 |
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| 320 |
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| 321 |
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| 322 | CKM == {
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| 323 | Indices -> {Index[QuarkGeneration], Index[QuarkGeneration]},
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| 324 | Unitary -> True,
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| 325 | Value -> {CKM[i_,j_] :> RCKM[i,j] + I ICKM[i,j]},
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| 326 | Description -> "CKM-Matrix"}
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| 327 | }
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| 328 |
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| 329 |
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| 330 | (************** Gauge Groups ******************)
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| 331 |
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| 332 | M$GaugeGroups = {
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| 333 |
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| 334 | U1Y == {
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| 335 | Abelian -> True,
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| 336 | GaugeBoson -> B,
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| 337 | Charge -> Y,
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| 338 | CouplingConstant -> g1},
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| 339 |
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| 340 | SU2L == {
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| 341 | Abelian -> False,
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| 342 | GaugeBoson -> Wi,
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| 343 | StructureConstant -> Eps,
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| 344 | CouplingConstant -> gw},
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| 345 |
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| 346 | SU3C == {
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| 347 | Abelian -> False,
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| 348 | GaugeBoson -> G,
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| 349 | StructureConstant -> f,
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| 350 | SymmetricTensor -> dSUN,
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| 351 | Representations -> {T, Colour},
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| 352 | CouplingConstant -> gs}
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| 353 | }
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| 354 |
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| 355 | (********* Particle Classes **********)
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| 356 |
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| 357 | M$ClassesDescription = {
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| 358 |
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| 359 | (********** Fermions ************)
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| 360 | (* Leptons (neutrino): I_3 = +1/2, Q = 0 *)
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| 361 | F[1] == {
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| 362 | ClassName -> vl,
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| 363 | ClassMembers -> {ve,vm,vt},
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| 364 | FlavorIndex -> Generation,
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| 365 | SelfConjugate -> False,
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| 366 | Indices -> {Index[Generation]},
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| 367 | Mass -> 0,
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| 368 | Width -> 0,
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| 369 | QuantumNumbers -> {LeptonNumber -> 1},
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| 370 | PropagatorLabel -> {"v", "ve", "vm", "vt"} ,
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| 371 | PropagatorType -> S,
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| 372 | PropagatorArrow -> Forward,
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| 373 | PDG -> {12,14,16},
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| 374 | FullName -> {"Electron-neutrino", "Mu-neutrino", "Tau-neutrino"} },
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| 375 |
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| 376 | (* Leptons (electron): I_3 = -1/2, Q = -1 *)
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| 377 | F[2] == {
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| 378 | ClassName -> l,
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| 379 | ClassMembers -> {e, m, tt},
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| 380 | FlavorIndex -> Generation,
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| 381 | SelfConjugate -> False,
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| 382 | Indices -> {Index[Generation]},
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| 383 | Mass -> {Ml, {Me, 5.11 * 10^(-4)}, {MM, 0.10566}, {MTA, 1.777}},
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| 384 | Width -> 0,
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| 385 | QuantumNumbers -> {Q -> -1, LeptonNumber -> 1},
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| 386 | PropagatorLabel -> {"l", "e", "m", "tt"},
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| 387 | PropagatorType -> Straight,
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| 388 | ParticleName -> {"e-", "m-", "tt-"},
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| 389 | AntiParticleName -> {"e+", "m+", "tt+"},
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| 390 | PropagatorArrow -> Forward,
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| 391 | PDG -> {11, 13, 15},
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| 392 | FullName -> {"Electron", "Muon", "Tau"} },
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| 393 |
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| 394 | (* Quarks (u): I_3 = +1/2, Q = +2/3 *)
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| 395 | F[3] == {
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| 396 | ClassMembers -> {u, c, t, tp},
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| 397 | ClassName -> uq,
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| 398 | FlavorIndex -> QuarkGeneration,
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| 399 | SelfConjugate -> False,
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| 400 | Indices -> {Index[QuarkGeneration], Index[Colour]},
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| 401 | Mass -> {Mu, {MU, 2.55*10^(-3)}, {MC, 1.42}, {MT, 172}, {MTp, 700}},
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| 402 | Width -> {0, 0, {WT, 1.4516}, {WTp, 14.109}},
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| 403 | QuantumNumbers -> {Q -> 2/3},
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| 404 | PropagatorLabel -> {"uq", "u", "c", "t", "tp"},
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| 405 | PropagatorType -> Straight,
|
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| 406 | PropagatorArrow -> Forward,
|
|---|
| 407 | PDG -> {2, 4, 6, 8},
|
|---|
| 408 | FullName -> {"u-quark", "c-quark", "t-quark", "t-prime-quark"}},
|
|---|
| 409 |
|
|---|
| 410 | (* Quarks (d): I_3 = -1/2, Q = -1/3 *)
|
|---|
| 411 | F[4] == {
|
|---|
| 412 | ClassMembers -> {d, s, b, bp},
|
|---|
| 413 | ClassName -> dq,
|
|---|
| 414 | FlavorIndex -> QuarkGeneration,
|
|---|
| 415 | SelfConjugate -> False,
|
|---|
| 416 | Indices -> {Index[QuarkGeneration], Index[Colour]},
|
|---|
| 417 | Mass -> {Md, {MD, 5.04*10^(-3)}, {MS, 0.104}, {MB, 4.7}, {MBp, 500}},
|
|---|
| 418 | Width -> {0,0,0,{WBp,0.28454}},
|
|---|
| 419 | QuantumNumbers -> {Q -> -1/3},
|
|---|
| 420 | PropagatorLabel -> {"dq", "d", "s", "b", "bp"},
|
|---|
| 421 | PropagatorType -> Straight,
|
|---|
| 422 | PropagatorArrow -> Forward,
|
|---|
| 423 | PDG -> {1,3,5,7},
|
|---|
| 424 | FullName -> {"d-quark", "s-quark", "b-quark", "b-prime-quark"} },
|
|---|
| 425 |
|
|---|
| 426 | (********** Ghosts **********)
|
|---|
| 427 | U[1] == {
|
|---|
| 428 | ClassName -> ghA,
|
|---|
| 429 | SelfConjugate -> False,
|
|---|
| 430 | Indices -> {},
|
|---|
| 431 | Ghost -> A,
|
|---|
| 432 | Mass -> 0,
|
|---|
| 433 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 434 | PropagatorLabel -> uA,
|
|---|
| 435 | PropagatorType -> GhostDash,
|
|---|
| 436 | PropagatorArrow -> Forward},
|
|---|
| 437 |
|
|---|
| 438 | U[2] == {
|
|---|
| 439 | ClassName -> ghZ,
|
|---|
| 440 | SelfConjugate -> False,
|
|---|
| 441 | Indices -> {},
|
|---|
| 442 | Mass -> {MZ, 91.188},
|
|---|
| 443 | Ghost -> Z,
|
|---|
| 444 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 445 | PropagatorLabel -> uZ,
|
|---|
| 446 | PropagatorType -> GhostDash,
|
|---|
| 447 | PropagatorArrow -> Forward},
|
|---|
| 448 |
|
|---|
| 449 | U[31] == {
|
|---|
| 450 | ClassName -> ghWp,
|
|---|
| 451 | SelfConjugate -> False,
|
|---|
| 452 | Indices -> {},
|
|---|
| 453 | Mass -> {MW, Internal},
|
|---|
| 454 | Ghost -> W,
|
|---|
| 455 | QuantumNumbers -> {Q-> 1, GhostNumber -> 1},
|
|---|
| 456 | PropagatorLabel -> uWp,
|
|---|
| 457 | PropagatorType -> GhostDash,
|
|---|
| 458 | PropagatorArrow -> Forward},
|
|---|
| 459 |
|
|---|
| 460 | U[32] == {
|
|---|
| 461 | ClassName -> ghWm,
|
|---|
| 462 | SelfConjugate -> False,
|
|---|
| 463 | Indices -> {},
|
|---|
| 464 | Mass -> {MW, Internal},
|
|---|
| 465 | Ghost -> Wbar,
|
|---|
| 466 | QuantumNumbers -> {Q-> -1, GhostNumber -> 1},
|
|---|
| 467 | PropagatorLabel -> uWm,
|
|---|
| 468 | PropagatorType -> GhostDash,
|
|---|
| 469 | PropagatorArrow -> Forward},
|
|---|
| 470 |
|
|---|
| 471 | U[4] == {
|
|---|
| 472 | ClassName -> ghG,
|
|---|
| 473 | SelfConjugate -> False,
|
|---|
| 474 | Indices -> {Index[Gluon]},
|
|---|
| 475 | Ghost -> G,
|
|---|
| 476 | Mass -> 0,
|
|---|
| 477 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 478 | PropagatorLabel -> uG,
|
|---|
| 479 | PropagatorType -> GhostDash,
|
|---|
| 480 | PropagatorArrow -> Forward},
|
|---|
| 481 |
|
|---|
| 482 | U[5] == {
|
|---|
| 483 | ClassName -> ghWi,
|
|---|
| 484 | Unphysical -> True,
|
|---|
| 485 | Definitions -> {ghWi[1] -> (ghWp + ghWm)/Sqrt[2],
|
|---|
| 486 | ghWi[2] -> (ghWm - ghWp)/Sqrt[2]/I,
|
|---|
| 487 | ghWi[3] -> cw ghZ + sw ghA},
|
|---|
| 488 | SelfConjugate -> False,
|
|---|
| 489 | Ghost -> Wi,
|
|---|
| 490 | Indices -> {Index[SU2W]},
|
|---|
| 491 | FlavorIndex -> SU2W},
|
|---|
| 492 |
|
|---|
| 493 | U[6] == {
|
|---|
| 494 | ClassName -> ghB,
|
|---|
| 495 | SelfConjugate -> False,
|
|---|
| 496 | Definitions -> {ghB -> -sw ghZ + cw ghA},
|
|---|
| 497 | Indices -> {},
|
|---|
| 498 | Ghost -> B,
|
|---|
| 499 | Unphysical -> True},
|
|---|
| 500 |
|
|---|
| 501 | (************ Gauge Bosons ***************)
|
|---|
| 502 | (* Gauge bosons: Q = 0 *)
|
|---|
| 503 | V[1] == {
|
|---|
| 504 | ClassName -> A,
|
|---|
| 505 | SelfConjugate -> True,
|
|---|
| 506 | Indices -> {},
|
|---|
| 507 | Mass -> 0,
|
|---|
| 508 | Width -> 0,
|
|---|
| 509 | PropagatorLabel -> "a",
|
|---|
| 510 | PropagatorType -> W,
|
|---|
| 511 | PropagatorArrow -> None,
|
|---|
| 512 | PDG -> 22,
|
|---|
| 513 | FullName -> "Photon" },
|
|---|
| 514 |
|
|---|
| 515 | V[2] == {
|
|---|
| 516 | ClassName -> Z,
|
|---|
| 517 | SelfConjugate -> True,
|
|---|
| 518 | Indices -> {},
|
|---|
| 519 | Mass -> {MZ, 91.188},
|
|---|
| 520 | Width -> {WZ, 2.44140351},
|
|---|
| 521 | PropagatorLabel -> "Z",
|
|---|
| 522 | PropagatorType -> Sine,
|
|---|
| 523 | PropagatorArrow -> None,
|
|---|
| 524 | PDG -> 23,
|
|---|
| 525 | FullName -> "Z" },
|
|---|
| 526 |
|
|---|
| 527 | (* Gauge bosons: Q = -1 *)
|
|---|
| 528 | V[3] == {
|
|---|
| 529 | ClassName -> W,
|
|---|
| 530 | SelfConjugate -> False,
|
|---|
| 531 | Indices -> {},
|
|---|
| 532 | Mass -> {MW, Internal},
|
|---|
| 533 | Width -> {WW, 2.04759951},
|
|---|
| 534 | QuantumNumbers -> {Q -> 1},
|
|---|
| 535 | PropagatorLabel -> "W",
|
|---|
| 536 | PropagatorType -> Sine,
|
|---|
| 537 | PropagatorArrow -> Forward,
|
|---|
| 538 | ParticleName ->"W+",
|
|---|
| 539 | AntiParticleName ->"W-",
|
|---|
| 540 | PDG -> 24,
|
|---|
| 541 | FullName -> "W" },
|
|---|
| 542 |
|
|---|
| 543 | V[4] == {
|
|---|
| 544 | ClassName -> G,
|
|---|
| 545 | SelfConjugate -> True,
|
|---|
| 546 | Indices -> {Index[Gluon]},
|
|---|
| 547 | Mass -> 0,
|
|---|
| 548 | Width -> 0,
|
|---|
| 549 | PropagatorLabel -> G,
|
|---|
| 550 | PropagatorType -> C,
|
|---|
| 551 | PropagatorArrow -> None,
|
|---|
| 552 | PDG -> 21,
|
|---|
| 553 | FullName -> "G" },
|
|---|
| 554 |
|
|---|
| 555 | V[5] == {
|
|---|
| 556 | ClassName -> Wi,
|
|---|
| 557 | Unphysical -> True,
|
|---|
| 558 | Definitions -> {Wi[mu_, 1] -> (W[mu] + Wbar[mu])/Sqrt[2],
|
|---|
| 559 | Wi[mu_, 2] -> (Wbar[mu] - W[mu])/Sqrt[2]/I,
|
|---|
| 560 | Wi[mu_, 3] -> cw Z[mu] + sw A[mu]},
|
|---|
| 561 | SelfConjugate -> True,
|
|---|
| 562 | Indices -> {Index[SU2W]},
|
|---|
| 563 | FlavorIndex -> SU2W,
|
|---|
| 564 | Mass -> 0,
|
|---|
| 565 | PDG -> {1,2,3}},
|
|---|
| 566 |
|
|---|
| 567 | V[6] == {
|
|---|
| 568 | ClassName -> B,
|
|---|
| 569 | SelfConjugate -> True,
|
|---|
| 570 | Definitions -> {B[mu_] -> -sw Z[mu] + cw A[mu]},
|
|---|
| 571 | Indices -> {},
|
|---|
| 572 | Mass -> 0,
|
|---|
| 573 | Unphysical -> True},
|
|---|
| 574 |
|
|---|
| 575 |
|
|---|
| 576 | (************ Scalar Fields **********)
|
|---|
| 577 | (* physical Higgs: Q = 0 *)
|
|---|
| 578 | S[1] == {
|
|---|
| 579 | ClassName -> H,
|
|---|
| 580 | SelfConjugate -> True,
|
|---|
| 581 | Mass -> {MH, 120},
|
|---|
| 582 | Width -> {WH, 0.00575308848},
|
|---|
| 583 | PropagatorLabel -> "H",
|
|---|
| 584 | PropagatorType -> D,
|
|---|
| 585 | PropagatorArrow -> None,
|
|---|
| 586 | PDG -> 25,
|
|---|
| 587 | TeXParticleName -> "\\phi",
|
|---|
| 588 | TeXClassName -> "\\phi",
|
|---|
| 589 | FullName -> "H" },
|
|---|
| 590 |
|
|---|
| 591 | S[2] == {
|
|---|
| 592 | ClassName -> phi,
|
|---|
| 593 | SelfConjugate -> True,
|
|---|
| 594 | Mass -> {MZ, 91.188},
|
|---|
| 595 | Width -> Wphi,
|
|---|
| 596 | PropagatorLabel -> "Phi",
|
|---|
| 597 | PropagatorType -> D,
|
|---|
| 598 | PropagatorArrow -> None,
|
|---|
| 599 | ParticleName ->"phi0",
|
|---|
| 600 | PDG -> 250,
|
|---|
| 601 | FullName -> "Phi",
|
|---|
| 602 | Goldstone -> Z },
|
|---|
| 603 |
|
|---|
| 604 | S[3] == {
|
|---|
| 605 | ClassName -> phi2,
|
|---|
| 606 | SelfConjugate -> False,
|
|---|
| 607 | Mass -> {MW, Internal},
|
|---|
| 608 | Width -> Wphi2,
|
|---|
| 609 | PropagatorLabel -> "Phi2",
|
|---|
| 610 | PropagatorType -> D,
|
|---|
| 611 | PropagatorArrow -> None,
|
|---|
| 612 | ParticleName ->"phi+",
|
|---|
| 613 | AntiParticleName ->"phi-",
|
|---|
| 614 | PDG -> 251,
|
|---|
| 615 | FullName -> "Phi2",
|
|---|
| 616 | TeXClassName -> "\\phi^+",
|
|---|
| 617 | TeXParticleName -> "\\phi^+",
|
|---|
| 618 | TeXAntiParticleName -> "\\phi^-",
|
|---|
| 619 | Goldstone -> W,
|
|---|
| 620 | QuantumNumbers -> {Q -> 1}}
|
|---|
| 621 | }
|
|---|
| 622 |
|
|---|
| 623 |
|
|---|
| 624 |
|
|---|
| 625 |
|
|---|
| 626 | (*****************************************************************************************)
|
|---|
| 627 |
|
|---|
| 628 | (* SM Lagrangian *)
|
|---|
| 629 |
|
|---|
| 630 | (******************** Gauge F^2 Lagrangian terms*************************)
|
|---|
| 631 | (*Sign convention from Lagrangian in between Eq. (A.9) and Eq. (A.10) of Peskin & Schroeder.*)
|
|---|
| 632 | LGauge = -1/4 (del[Wi[nu, i1], mu] - del[Wi[mu, i1], nu] + gw Eps[i1, i2, i3] Wi[mu, i2] Wi[nu, i3])*
|
|---|
| 633 | (del[Wi[nu, i1], mu] - del[Wi[mu, i1], nu] + gw Eps[i1, i4, i5] Wi[mu, i4] Wi[nu, i5]) -
|
|---|
| 634 |
|
|---|
| 635 | 1/4 (del[B[nu], mu] - del[B[mu], nu])^2 -
|
|---|
| 636 |
|
|---|
| 637 | 1/4 (del[G[nu, a1], mu] - del[G[mu, a1], nu] + gs f[a1, a2, a3] G[mu, a2] G[nu, a3])*
|
|---|
| 638 | (del[G[nu, a1], mu] - del[G[mu, a1], nu] + gs f[a1, a4, a5] G[mu, a4] G[nu, a5]);
|
|---|
| 639 |
|
|---|
| 640 |
|
|---|
| 641 | (********************* Fermion Lagrangian terms*************************)
|
|---|
| 642 | (*Sign convention from Lagrangian in between Eq. (A.9) and Eq. (A.10) of Peskin & Schroeder.*)
|
|---|
| 643 | LFermions = Module[{Lkin, LQCD, LEWleft, LEWright},
|
|---|
| 644 |
|
|---|
| 645 | Lkin = I uqbar.Ga[mu].del[uq, mu] +
|
|---|
| 646 | I dqbar.Ga[mu].del[dq, mu] +
|
|---|
| 647 | I lbar.Ga[mu].del[l, mu] +
|
|---|
| 648 | I vlbar.Ga[mu].del[vl, mu];
|
|---|
| 649 |
|
|---|
| 650 | LQCD = gs (uqbar.Ga[mu].T[a].uq +
|
|---|
| 651 | dqbar.Ga[mu].T[a].dq)G[mu, a];
|
|---|
| 652 |
|
|---|
| 653 | LBright =
|
|---|
| 654 | -2ee/cw B[mu]/2 lbar.Ga[mu].ProjP.l + (*Y_lR=-2*)
|
|---|
| 655 | 4ee/3/cw B[mu]/2 uqbar.Ga[mu].ProjP.uq - (*Y_uR=4/3*)
|
|---|
| 656 | 2ee/3/cw B[mu]/2 dqbar.Ga[mu].ProjP.dq; (*Y_dR=-2/3*)
|
|---|
| 657 |
|
|---|
| 658 | LBleft =
|
|---|
| 659 | -ee/cw B[mu]/2 vlbar.Ga[mu].ProjM.vl - (*Y_LL=-1*)
|
|---|
| 660 | ee/cw B[mu]/2 lbar.Ga[mu].ProjM.l + (*Y_LL=-1*)
|
|---|
| 661 | ee/3/cw B[mu]/2 uqbar.Ga[mu].ProjM.uq + (*Y_QL=1/3*)
|
|---|
| 662 | ee/3/cw B[mu]/2 dqbar.Ga[mu].ProjM.dq ; (*Y_QL=1/3*)
|
|---|
| 663 |
|
|---|
| 664 | LWleft = ee/sw/2(
|
|---|
| 665 | vlbar.Ga[mu].ProjM.vl Wi[mu, 3] - (*sigma3 = ( 1 0 )*)
|
|---|
| 666 | lbar.Ga[mu].ProjM.l Wi[mu, 3] + (* ( 0 -1 )*)
|
|---|
| 667 |
|
|---|
| 668 | Sqrt[2] vlbar.Ga[mu].ProjM.l W[mu] +
|
|---|
| 669 | Sqrt[2] lbar.Ga[mu].ProjM.vl Wbar[mu]+
|
|---|
| 670 |
|
|---|
| 671 | uqbar.Ga[mu].ProjM.uq Wi[mu, 3] - (*sigma3 = ( 1 0 )*)
|
|---|
| 672 | dqbar.Ga[mu].ProjM.dq Wi[mu, 3] + (* ( 0 -1 )*)
|
|---|
| 673 |
|
|---|
| 674 | Sqrt[2] uqbar.Ga[mu].ProjM.CKM.dq W[mu] +
|
|---|
| 675 | Sqrt[2] dqbar.Ga[mu].ProjM.HC[CKM].uq Wbar[mu]
|
|---|
| 676 | );
|
|---|
| 677 |
|
|---|
| 678 | Lkin + LQCD + LBright + LBleft + LWleft];
|
|---|
| 679 |
|
|---|
| 680 | (******************** Higgs Lagrangian terms****************************)
|
|---|
| 681 | Phi := If[FeynmanGauge, {-I phi2, (v + H + I phi)/Sqrt[2]}, {0, (v + H)/Sqrt[2]}];
|
|---|
| 682 | Phibar := If[FeynmanGauge, {I phi2bar, (v + H - I phi)/Sqrt[2]} ,{0, (v + H)/Sqrt[2]}];
|
|---|
| 683 |
|
|---|
| 684 |
|
|---|
| 685 |
|
|---|
| 686 | LHiggs := Block[{PMVec, WVec, Dc, Dcbar, Vphi},
|
|---|
| 687 |
|
|---|
| 688 | PMVec = Table[PauliSigma[i], {i, 3}];
|
|---|
| 689 | Wvec[mu_] := {Wi[mu, 1], Wi[mu, 2], Wi[mu, 3]};
|
|---|
| 690 |
|
|---|
| 691 | (*Y_phi=1*)
|
|---|
| 692 | Dc[f_, mu_] := I del[f, mu] + ee/cw B[mu]/2 f + ee/sw/2 (Wvec[mu].PMVec).f;
|
|---|
| 693 | Dcbar[f_, mu_] := -I del[f, mu] + ee/cw B[mu]/2 f + ee/sw/2 f.(Wvec[mu].PMVec);
|
|---|
| 694 |
|
|---|
| 695 | Vphi[Phi_, Phibar_] := -muH^2 Phibar.Phi + \[Lambda] (Phibar.Phi)^2;
|
|---|
| 696 |
|
|---|
| 697 | (Dcbar[Phibar, mu]).Dc[Phi, mu] - Vphi[Phi, Phibar]];
|
|---|
| 698 |
|
|---|
| 699 |
|
|---|
| 700 | (*************** Yukawa Lagrangian***********************)
|
|---|
| 701 | LYuk := If[FeynmanGauge,
|
|---|
| 702 |
|
|---|
| 703 | Module[{s,r,n,m,i}, -
|
|---|
| 704 | yd[m] CKM[n,m] uqbar[s,n,i].ProjP[s,r].dq[r,m,i] (-I phi2) -
|
|---|
| 705 | yd[n] dqbar[s,n,i].ProjP[s,r].dq[r,n,i] (v+H +I phi)/Sqrt[2] -
|
|---|
| 706 |
|
|---|
| 707 | yu[n] uqbar[s,n,i].ProjP[s,r].uq[r,n,i] (v+H -I phi)/Sqrt[2] + (*This sign from eps matrix*)
|
|---|
| 708 | yu[m] Conjugate[CKM[m,n]] dqbar[s,n,i].ProjP[s,r].uq[r,m,i] ( I phi2bar) -
|
|---|
| 709 |
|
|---|
| 710 | yl[n] vlbar[s,n].ProjP[s,r].l[r,n] (-I phi2) -
|
|---|
| 711 | yl[n] lbar[s,n].ProjP[s,r].l[r,n] (v+H +I phi)/Sqrt[2]
|
|---|
| 712 | ],
|
|---|
| 713 |
|
|---|
| 714 | Module[{s,r,n,m,i}, -
|
|---|
| 715 | yd[n] dqbar[s,n,i].ProjP[s,r].dq[r,n,i] (v+H)/Sqrt[2] -
|
|---|
| 716 | yu[n] uqbar[s,n,i].ProjP[s,r].uq[r,n,i] (v+H)/Sqrt[2] -
|
|---|
| 717 | yl[n] lbar[s,n].ProjP[s,r].l[r,n] (v+H)/Sqrt[2]
|
|---|
| 718 | ]
|
|---|
| 719 | ];
|
|---|
| 720 |
|
|---|
| 721 | LYukawa := LYuk + HC[LYuk];
|
|---|
| 722 |
|
|---|
| 723 |
|
|---|
| 724 |
|
|---|
| 725 | (**************Ghost terms**************************)
|
|---|
| 726 | (* Now we need the ghost terms which are of the form: *)
|
|---|
| 727 | (* - g * antighost * d_BRST G *)
|
|---|
| 728 | (* where d_BRST G is BRST transform of the gauge fixing function. *)
|
|---|
| 729 |
|
|---|
| 730 | LGhost := If[FeynmanGauge,
|
|---|
| 731 | Block[{dBRSTG,LGhostG,dBRSTWi,LGhostWi,dBRSTB,LGhostB},
|
|---|
| 732 |
|
|---|
| 733 | (***********First the pure gauge piece.**********************)
|
|---|
| 734 | dBRSTG[mu_,a_] := 1/gs Module[{a2, a3}, del[ghG[a], mu] + gs f[a,a2,a3] G[mu,a2] ghG[a3]];
|
|---|
| 735 | LGhostG := - gs ghGbar[a].del[dBRSTG[mu,a],mu];
|
|---|
| 736 |
|
|---|
| 737 | dBRSTWi[mu_,i_] := sw/ee Module[{i2, i3}, del[ghWi[i], mu] + ee/sw Eps[i,i2,i3] Wi[mu,i2] ghWi[i3] ];
|
|---|
| 738 | LGhostWi := - ee/sw ghWibar[a].del[dBRSTWi[mu,a],mu];
|
|---|
| 739 |
|
|---|
| 740 | dBRSTB[mu_] := cw/ee del[ghB, mu];
|
|---|
| 741 | LGhostB := - ee/cw ghBbar.del[dBRSTB[mu],mu];
|
|---|
| 742 |
|
|---|
| 743 | (***********Next the piece from the scalar field.************)
|
|---|
| 744 | LGhostphi := - ee/(2*sw*cw) MW ( - I phi2 ( (cw^2-sw^2)ghWpbar.ghZ + 2sw*cw ghWpbar.ghA ) +
|
|---|
| 745 | I phi2bar ( (cw^2-sw^2)ghWmbar.ghZ + 2sw*cw ghWmbar.ghA ) ) -
|
|---|
| 746 | ee/(2*sw) MW ( ( (v+H) + I phi) ghWpbar.ghWp + ( (v+H) - I phi) ghWmbar.ghWm ) -
|
|---|
| 747 | I ee/(2*sw) MZ ( - phi2bar ghZbar.ghWp + phi2 ghZbar.ghWm ) -
|
|---|
| 748 | ee/(2*sw*cw) MZ (v+H) ghZbar.ghZ ;
|
|---|
| 749 |
|
|---|
| 750 |
|
|---|
| 751 | (***********Now add the pieces together.********************)
|
|---|
| 752 | LGhostG + LGhostWi + LGhostB + LGhostphi]
|
|---|
| 753 |
|
|---|
| 754 | , 0];
|
|---|
| 755 |
|
|---|
| 756 | (*********Total SM Lagrangian*******)
|
|---|
| 757 | L4Gen := LGauge + LHiggs + LFermions + LYukawa + LGhost;
|
|---|