| 1 | (***************************************************************************************************************)
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| 2 | (****** This is the FeynRules mod-file for the Standard model ******)
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| 3 | (****** extended with a fermionic SU(2) triplet which give mass ******)
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| 4 | (****** to one neutrino via a type III seesaw mechanism ******)
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| 5 | (****** ******)
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| 6 | (****** Authors: C. Biggio, F. Bonnet ******)
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| 7 | (****** ******)
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| 8 | (****** Choose whether Feynman gauge is desired. ******)
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| 9 | (****** If set to False, unitary gauge is assumed. ****)
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| 10 | (****** Feynman gauge is especially useful for CalcHEP/CompHEP where the calculation is 10-100 times faster. ***)
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| 11 | (****** Feynman gauge is not supported in MadGraph and Sherpa. ****)
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| 12 | (***************************************************************************************************************)
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| 13 |
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| 14 | M$ModelName = "typeIIIseesaw1";
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| 15 |
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| 16 |
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| 17 | M$Information = {Authors -> {"C.Biggio", "F. Bonnet"},
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| 18 | Version -> "1.0",
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| 19 | Date -> "16. 03. 2011",
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| 20 | Institutions -> {"IFAE/UAB", "INFN Padova"},
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| 21 | Emails -> {"biggio@ifae.es", "bonnet@pd.infn.it"},
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| 22 | URLs -> "http://feynrules.phys.ucl.ac.be/view/Main/TypeIIIseesaw"};
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| 23 |
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| 24 | FeynmanGauge = False;
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| 25 |
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| 26 |
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| 27 | (******* Index definitions ********)
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| 28 |
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| 29 | IndexRange[ Index[Generation] ] = Range[3]
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| 30 |
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| 31 | IndexRange[ Index[LeptonGeneration] ] = Range[4]
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| 32 |
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| 33 | IndexRange[ Index[Colour] ] = NoUnfold[Range[3]]
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| 34 |
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| 35 | IndexRange[ Index[Gluon] ] = NoUnfold[Range[8]]
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| 36 |
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| 37 | IndexRange[ Index[SU2W] ] = Range[3]
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| 38 |
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| 39 |
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| 40 | IndexStyle[Colour, i]
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| 41 |
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| 42 | IndexStyle[Generation, f]
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| 43 |
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| 44 | IndexStyle[LeptonGeneration, fl]
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| 45 |
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| 46 | IndexStyle[Gluon ,a]
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| 47 |
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| 48 | IndexStyle[SU2W ,k]
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| 49 |
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| 50 |
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| 51 | (******* Gauge parameters (for FeynArts) ********)
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| 52 |
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| 53 | GaugeXi[ V[1] ] = GaugeXi[A];
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| 54 | GaugeXi[ V[2] ] = GaugeXi[Z];
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| 55 | GaugeXi[ V[3] ] = GaugeXi[W];
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| 56 | GaugeXi[ V[4] ] = GaugeXi[G];
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| 57 | GaugeXi[ S[1] ] = 1;
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| 58 | GaugeXi[ S[2] ] = GaugeXi[Z];
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| 59 | GaugeXi[ S[3] ] = GaugeXi[W];
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| 60 | GaugeXi[ U[1] ] = GaugeXi[A];
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| 61 | GaugeXi[ U[2] ] = GaugeXi[Z];
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| 62 | GaugeXi[ U[31] ] = GaugeXi[W];
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| 63 | GaugeXi[ U[32] ] = GaugeXi[W];
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| 64 | GaugeXi[ U[4] ] = GaugeXi[G];
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| 65 |
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| 66 |
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| 67 | (**************** Parameters *************)
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| 68 |
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| 69 | M$Parameters = {
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| 70 |
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| 71 | (* External parameters *)
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| 72 |
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| 73 | \[Alpha]EWM1== {
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| 74 | ParameterType -> External,
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| 75 | BlockName -> SMINPUTS,
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| 76 | ParameterName -> aEWM1,
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| 77 | InteractionOrder -> {QED, -2},
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| 78 | Value -> 127.9,
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| 79 | Description -> "Inverse of the electroweak coupling constant"},
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| 80 |
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| 81 | Gf == {
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| 82 | ParameterType -> External,
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| 83 | BlockName -> SMINPUTS,
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| 84 | TeX -> Subscript[G, f],
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| 85 | InteractionOrder -> {QED, 2},
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| 86 | Value -> 1.16639 * 10^(-5),
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| 87 | Description -> "Fermi constant"},
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| 88 |
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| 89 | \[Alpha]S == {
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| 90 | ParameterType -> External,
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| 91 | BlockName -> SMINPUTS,
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| 92 | TeX -> Subscript[\[Alpha], s],
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| 93 | ParameterName -> aS,
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| 94 | InteractionOrder -> {QCD, 2},
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| 95 | Value -> 0.118,
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| 96 | Description -> "Strong coupling constant at the Z pole."},
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| 97 |
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| 98 | ymc == {
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| 99 | ParameterType -> External,
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| 100 | BlockName -> YUKAWA,
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| 101 | Value -> 1.42,
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| 102 | OrderBlock -> {4},
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| 103 | Description -> "Charm Yukawa mass"},
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| 104 |
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| 105 | ymb == {
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| 106 | ParameterType -> External,
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| 107 | BlockName -> YUKAWA,
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| 108 | Value -> 4.7,
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| 109 | OrderBlock -> {5},
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| 110 | Description -> "Bottom Yukawa mass"},
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| 111 |
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| 112 | ymt == {
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| 113 | ParameterType -> External,
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| 114 | BlockName -> YUKAWA,
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| 115 | Value -> 174.3,
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| 116 | OrderBlock -> {6},
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| 117 | Description -> "Top Yukawa mass"},
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| 118 |
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| 119 | mv1 == {
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| 120 | ParameterType -> External,
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| 121 | BlockName -> NEWMASSES,
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| 122 | Value -> 0,
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| 123 | OrderBlock -> {1},
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| 124 | Description -> "nu1 mass"},
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| 125 |
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| 126 | mv2 == {
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| 127 | ParameterType -> External,
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| 128 | BlockName -> NEWMASSES,
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| 129 | Value -> 0,
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| 130 | OrderBlock -> {2},
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| 131 | Description -> "nu2 mass"},
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| 132 |
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| 133 | mv3 == {
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| 134 | ParameterType -> External,
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| 135 | BlockName -> NEWMASSES,
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| 136 | Value -> 0,
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| 137 | OrderBlock -> {3},
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| 138 | Description -> "nu3 mass"},
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| 139 |
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| 140 | yme == {
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| 141 | ParameterType -> External,
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| 142 | BlockName -> YUKAWA,
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| 143 | Value -> 0,
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| 144 | OrderBlock -> {13},
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| 145 | Description -> "Electron Yukawa mass"},
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| 146 |
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| 147 | ymm == {
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| 148 | ParameterType -> External,
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| 149 | BlockName -> YUKAWA,
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| 150 | Value -> 0,
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| 151 | OrderBlock -> {14},
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| 152 | Description -> "Muon Yukawa mass"},
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| 153 |
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| 154 | ymtau == {
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| 155 | ParameterType -> External,
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| 156 | BlockName -> YUKAWA,
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| 157 | Value -> 1.777,
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| 158 | OrderBlock -> {15},
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| 159 | Description -> "Tau Yukawa mass"},
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| 160 |
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| 161 | cabi == {
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| 162 | TeX -> Subscript[\[Theta], c],
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| 163 | ParameterType -> External,
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| 164 | BlockName -> CKMBLOCK,
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| 165 | Value -> 0.227736,
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| 166 | OrderBlock -> {1},
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| 167 | Description -> "Cabibbo angle"},
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| 168 |
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| 169 | mtr == {
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| 170 | ParameterType -> External,
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| 171 | BlockName -> NEWMASSES,
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| 172 | Value -> 100.8,
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| 173 | OrderBlock -> {4},
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| 174 | Description -> "Neutral triplet Majorana mass"},
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| 175 |
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| 176 | mtrm == {
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| 177 | ParameterType -> External,
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| 178 | BlockName -> NEWMASSES,
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| 179 | Value -> 101,
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| 180 | OrderBlock -> {5},
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| 181 | Description -> "Charged triplet Majorana mass"},
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| 182 |
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| 183 | Ve == {
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| 184 | ParameterType -> External,
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| 185 | BlockName -> MIXING,
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| 186 | Value -> 0,
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| 187 | OrderBlock -> {1},
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| 188 | Description -> "Electron mixing"},
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| 189 |
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| 190 | Vm == {
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| 191 | ParameterType -> External,
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| 192 | BlockName -> MIXING,
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| 193 | Value -> 0.063,
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| 194 | OrderBlock -> {2},
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| 195 | Description -> "Muon mixing"},
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| 196 |
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| 197 | Vtt == {
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| 198 | ParameterType -> External,
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| 199 | BlockName -> MIXING,
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| 200 | Value -> 0,
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| 201 | OrderBlock -> {3},
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| 202 | Description -> "Tau mixing"},
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| 203 |
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| 204 | theta13 == {
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| 205 | TeX -> Subscript[\[Theta], 13],
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| 206 | ParameterType -> External,
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| 207 | BlockName -> CKMBLOCK,
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| 208 | Value -> 0.1,
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| 209 | OrderBlock -> {2},
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| 210 | Description -> "PMNS theta13"},
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| 211 |
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| 212 | theta12 == {
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| 213 | TeX -> Subscript[\[Theta], 12],
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| 214 | ParameterType -> External,
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| 215 | BlockName -> CKMBLOCK,
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| 216 | Value -> 0.60,
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| 217 | OrderBlock -> {3},
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| 218 | Description -> "PMNS solar angle"},
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| 219 |
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| 220 | theta23 == {
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| 221 | TeX -> Subscript[\[Theta], 23],
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| 222 | ParameterType -> External,
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| 223 | BlockName -> CKMBLOCK,
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| 224 | Value -> 0.75,
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| 225 | OrderBlock -> {4},
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| 226 | Description -> "PMNS athmospheric angle"},
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| 227 |
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| 228 |
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| 229 |
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| 230 | (* Internal Parameters *)
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| 231 |
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| 232 | \[Alpha]EW == {
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| 233 | ParameterType -> Internal,
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| 234 | Value -> 1/\[Alpha]EWM1,
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| 235 | TeX -> Subscript[\[Alpha], EW],
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| 236 | ParameterName -> aEW,
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| 237 | InteractionOrder -> {QED, 2},
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| 238 | Description -> "Electroweak coupling contant"},
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| 239 |
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| 240 |
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| 241 | MW == {
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| 242 | ParameterType -> Internal,
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| 243 | Value -> Sqrt[MZ^2/2+Sqrt[MZ^4/4-Pi/Sqrt[2]*\[Alpha]EW/Gf*MZ^2]],
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| 244 | TeX -> Subscript[M, W],
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| 245 | Description -> "W mass"},
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| 246 |
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| 247 | sw2 == {
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| 248 | ParameterType -> Internal,
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| 249 | Value -> 1-(MW/MZ)^2,
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| 250 | Description -> "Squared Sin of the Weinberg angle"},
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| 251 |
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| 252 | ee == {
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| 253 | TeX -> e,
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| 254 | ParameterType -> Internal,
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| 255 | Value -> Sqrt[4 Pi \[Alpha]EW],
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| 256 | InteractionOrder -> {QED, 1},
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| 257 | Description -> "Electric coupling constant"},
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| 258 |
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| 259 | cw == {
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| 260 | TeX -> Subscript[c, w],
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| 261 | ParameterType -> Internal,
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| 262 | Value -> Sqrt[1 - sw2],
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| 263 | Description -> "Cos of the Weinberg angle"},
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| 264 |
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| 265 | sw == {
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| 266 | TeX -> Subscript[s, w],
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| 267 | ParameterType -> Internal,
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| 268 | Value -> Sqrt[sw2],
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| 269 | Description -> "Sin of the Weinberg angle"},
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| 270 |
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| 271 | gw == {
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| 272 | TeX -> Subscript[g, w],
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| 273 | ParameterType -> Internal,
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| 274 | Value -> ee / sw,
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| 275 | InteractionOrder -> {QED, 1},
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| 276 | Description -> "Weak coupling constant"},
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| 277 |
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| 278 | g1 == {
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| 279 | TeX -> Subscript[g, 1],
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| 280 | ParameterType -> Internal,
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| 281 | Value -> ee / cw,
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| 282 | InteractionOrder -> {QED, 1},
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| 283 | Description -> "U(1)Y coupling constant"},
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| 284 |
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| 285 | gs == {
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| 286 | TeX -> Subscript[g, s],
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| 287 | ParameterType -> Internal,
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| 288 | Value -> Sqrt[4 Pi \[Alpha]S],
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| 289 | InteractionOrder -> {QCD, 1},
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| 290 | ParameterName -> G,
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| 291 | Description -> "Strong coupling constant"},
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| 292 |
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| 293 | v == {
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| 294 | ParameterType -> Internal,
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| 295 | Value -> 2*MW*sw/ee,
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| 296 | InteractionOrder -> {QED, -1},
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| 297 | Description -> "Higgs VEV"},
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| 298 |
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| 299 | \[Lambda] == {
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| 300 | ParameterType -> Internal,
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| 301 | Value -> MH^2/(2*v^2),
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| 302 | InteractionOrder -> {QED, 2},
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| 303 | ParameterName -> lam,
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| 304 | Description -> "Higgs quartic coupling"},
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| 305 |
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| 306 | muH == {
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| 307 | ParameterType -> Internal,
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| 308 | Value -> Sqrt[v^2 \[Lambda]],
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| 309 | TeX -> \[Mu],
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| 310 | Description -> "Coefficient of the quadratic piece of the Higgs potential"},
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| 311 |
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| 312 | yl == {
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| 313 | TeX -> Superscript[y, l],
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| 314 | Indices -> {Index[LeptonGeneration]},
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| 315 | AllowSummation -> True,
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| 316 | ParameterType -> Internal,
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| 317 | Value -> {yl[1] -> Sqrt[2] yme / v, yl[2] -> Sqrt[2] ymm / v, yl[3] -> Sqrt[2] ymtau / v, yl[4] -> 0},
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| 318 | ParameterName -> {yl[1] -> ye, yl[2] -> ym, yl[3] -> ytau, yl[4] -> useless},
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| 319 | InteractionOrder -> {QED, 1},
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| 320 | ComplexParameter -> False,
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| 321 | Description -> "Standard Model lepton Yukawa coupling"},
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| 322 |
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| 323 | yu == {
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| 324 | TeX -> Superscript[y, u],
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| 325 | Indices -> {Index[Generation]},
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| 326 | AllowSummation -> True,
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| 327 | ParameterType -> Internal,
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| 328 | Value -> {yu[1] -> 0, yu[2] -> Sqrt[2] ymc / v, yu[3] -> Sqrt[2] ymt / v},
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| 329 | ParameterName -> {yu[1] -> yu, yu[2] -> yc, yu[3] -> yt},
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| 330 | InteractionOrder -> {QED, 1},
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| 331 | ComplexParameter -> False,
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| 332 | Description -> "U-quark Yukawa coupling"},
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| 333 |
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| 334 | yd == {
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| 335 | TeX -> Superscript[y, d],
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| 336 | Indices -> {Index[Generation]},
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| 337 | AllowSummation -> True,
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| 338 | ParameterType -> Internal,
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| 339 | Value -> {yd[1] -> 0, yd[2] -> 0, yd[3] -> Sqrt[2] ymb / v},
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| 340 | ParameterName -> {yd[1] -> yd, yd[2] -> ys, yd[3] -> yb},
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| 341 | InteractionOrder -> {QED, 1},
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| 342 | ComplexParameter -> False,
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| 343 | Description -> "D-quark Yukawa coupling"},
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| 344 |
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| 345 | (* N. B. : only Cabibbo mixing! *)
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| 346 | CKM == {
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| 347 | Indices -> {Index[Generation], Index[Generation]},
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| 348 | TensorClass -> CKM,
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| 349 | Unitary -> True,
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| 350 | Value -> {CKM[1,1] -> Cos[cabi],
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| 351 | CKM[1,2] -> Sin[cabi],
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| 352 | CKM[1,3] -> 0,
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| 353 | CKM[2,1] -> -Sin[cabi],
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| 354 | CKM[2,2] -> Cos[cabi],
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| 355 | CKM[2,3] -> 0,
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| 356 | CKM[3,1] -> 0,
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| 357 | CKM[3,2] -> 0,
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| 358 | CKM[3,3] -> 1},
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| 359 | Description -> "CKM-Matrix"},
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| 360 |
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| 361 | (* N. B. : no phases! *)
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| 362 | PMNS == {
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| 363 | Indices -> {Index[Generation], Index[Generation]},
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| 364 | TensorClass -> CKM,
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| 365 | Unitary -> True,
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| 366 | Value -> {PMNS[1,1] -> Cos[theta13] Cos[theta12],
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| 367 | PMNS[1,2] -> Cos[theta13] Sin[theta12],
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| 368 | PMNS[1,3] -> Sin[theta13],
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| 369 | PMNS[2,1] -> -Cos[theta23]*Sin[theta12] - Sin[theta23]*Sin[theta13]*Cos[theta12],
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| 370 | PMNS[2,2] -> Cos[theta23]*Cos[theta12] - Sin[theta23]*Sin[theta13]*Sin[theta12],
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| 371 | PMNS[2,3] -> Sin[theta23]*Cos[theta13],
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| 372 | PMNS[3,1] -> Sin[theta23]*Sin[theta12] - Cos[theta23]*Sin[theta13]*Cos[theta12],
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| 373 | PMNS[3,2] -> -Sin[theta23]*Cos[theta12] - Cos[theta23]*Sin[theta13]*Sin[theta12],
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| 374 | PMNS[3,3] -> Cos[theta23]*Cos[theta13]},
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| 375 | Description -> "PMNS-Matrix"},
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| 376 |
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| 377 |
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| 378 | (***********************************************)
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| 379 | (********** COUPLINGS **********)
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| 380 | (***********************************************)
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| 381 |
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| 382 | gCCL == {
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| 383 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
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| 384 | TensorClass -> CKM,
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| 385 | ComplexParameter -> False,
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| 386 | Value -> {gCCL[1,1] -> Cos[theta12] Cos[theta13] + 1/2 (Ve^2 Cos[theta12] Cos[theta13] +
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| 387 | Ve Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
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| 388 | Ve Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
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| 389 | gCCL[1,2] -> Cos[theta13] Sin[theta12] + 1/2 (Ve^2 Cos[theta13] Sin[theta12] +
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| 390 | Ve Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
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| 391 | Ve Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
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| 392 | gCCL[1,3] -> Sin[theta13] + 1/2 (Ve Vtt Cos[theta13] Cos[theta23] + Ve^2 Sin[theta13] + Ve Vm Cos[theta13] Sin[theta23]),
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| 393 | gCCL[1,4] -> - Ve,
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| 394 | gCCL[2,1] -> -Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23] +
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| 395 | 1/2 (Ve Vm Cos[theta12] Cos[theta13] + Vm Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
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| 396 | Sin[theta12] Sin[theta23]) + Vm^2 (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
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| 397 | gCCL[2,2] -> Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23] +
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| 398 | 1/2 (Ve Vm Cos[theta13] Sin[theta12] + Vm Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
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| 399 | Vm^2 (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 400 | gCCL[2,3] -> Cos[theta13] Sin[theta23] + 1/2 (Vm Vtt Cos[theta13] Cos[theta23] + Ve Vm Sin[theta13] + Vm^2 Cos[theta13] Sin[theta23]),
|
|---|
| 401 | gCCL[2,4] -> - Vm,
|
|---|
| 402 | gCCL[3,1] -> -Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23] + 1/2 (Ve Vtt Cos[theta12] Cos[theta13] +
|
|---|
| 403 | Vtt^2 (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 404 | Vm Vtt (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 405 | gCCL[3,2] -> -Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23] + 1/2 (Ve Vtt Cos[theta13] Sin[theta12] +
|
|---|
| 406 | Vtt^2 (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 407 | Vm Vtt (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 408 | gCCL[3,3] -> Cos[theta13] Cos[theta23] + 1/2 (Vtt^2 Cos[theta13] Cos[theta23] + Ve Vtt Sin[theta13] + Vm Vtt Cos[theta13] Sin[theta23]),
|
|---|
| 409 | gCCL[3,4] -> - Vtt,
|
|---|
| 410 | gCCL[4,1] -> 0,
|
|---|
| 411 | gCCL[4,2] -> 0,
|
|---|
| 412 | gCCL[4,3] -> 0,
|
|---|
| 413 | gCCL[4,4] -> Sqrt[2] (1 + 1/2 (-Ve^2 - Vm^2 - Vtt^2))},
|
|---|
| 414 | Description -> "gCCL-Matrix"},
|
|---|
| 415 |
|
|---|
| 416 |
|
|---|
| 417 |
|
|---|
| 418 |
|
|---|
| 419 | gCCR == {
|
|---|
| 420 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 421 | TensorClass -> CKM,
|
|---|
| 422 | ComplexParameter -> False,
|
|---|
| 423 | Value -> {gCCR[1,1] -> 0,
|
|---|
| 424 | gCCR[1,2] -> 0,
|
|---|
| 425 | gCCR[1,3] -> 0,
|
|---|
| 426 | gCCR[1,4] -> -Sqrt[2]*yme/mtr*Ve,
|
|---|
| 427 | gCCR[2,1] -> 0,
|
|---|
| 428 | gCCR[2,2] -> 0,
|
|---|
| 429 | gCCR[2,3] -> 0,
|
|---|
| 430 | gCCR[2,4] -> -Sqrt[2]*ymm/mtr*Vm,
|
|---|
| 431 | gCCR[3,1] -> 0,
|
|---|
| 432 | gCCR[3,2] -> 0,
|
|---|
| 433 | gCCR[3,3] -> 0,
|
|---|
| 434 | gCCR[3,4] -> -Sqrt[2]*ymtau/mtr*Vtt,
|
|---|
| 435 | gCCR[4,1] -> -( Ve Cos[theta12] Cos[theta13] + Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 436 | Sin[theta12] Sin[theta23]) + Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 437 | gCCR[4,2] -> - (Ve Cos[theta13] Sin[theta12] + Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 438 | Cos[theta12] Sin[theta23]) + Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 439 | gCCR[4,3] -> - (Vtt Cos[theta13] Cos[theta23] + Ve Sin[theta13] + Vm Cos[theta13] Sin[theta23]),
|
|---|
| 440 | gCCR[4,4] -> 1 + 1/2 (-Ve^2 - Vm^2 - Vtt^2)},
|
|---|
| 441 | Description -> "gCCR-Matrix"},
|
|---|
| 442 |
|
|---|
| 443 |
|
|---|
| 444 |
|
|---|
| 445 |
|
|---|
| 446 |
|
|---|
| 447 | gNCL == {
|
|---|
| 448 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 449 | TensorClass -> CKM,
|
|---|
| 450 | Hermitian -> True,
|
|---|
| 451 | Value -> {gNCL[1,1] -> 1/2-cw^2-Ve^2,
|
|---|
| 452 | gNCL[1,2] -> Ve*Vm,
|
|---|
| 453 | gNCL[1,3] -> Ve*Vtt,
|
|---|
| 454 | gNCL[1,4] -> Ve/Sqrt[2],
|
|---|
| 455 | gNCL[2,1] -> Ve*Vm,
|
|---|
| 456 | gNCL[2,2] -> 1/2-cw^2-Vm^2,
|
|---|
| 457 | gNCL[2,3] -> Vm*Vtt,
|
|---|
| 458 | gNCL[2,4] -> Vm/Sqrt[2],
|
|---|
| 459 | gNCL[3,1] -> Ve*Vtt,
|
|---|
| 460 | gNCL[3,2] -> Vm*Vtt,
|
|---|
| 461 | gNCL[3,3] -> 1/2-cw^2-Vtt^2,
|
|---|
| 462 | gNCL[3,4] -> Vtt/Sqrt[2],
|
|---|
| 463 | gNCL[4,1] -> Ve/Sqrt[2],
|
|---|
| 464 | gNCL[4,2] -> Vm/Sqrt[2],
|
|---|
| 465 | gNCL[4,3] -> Vtt/Sqrt[2],
|
|---|
| 466 | gNCL[4,4] -> Ve^2+Vm^2+Vtt^2-cw^2},
|
|---|
| 467 | Description -> "gNCL-Matrix"},
|
|---|
| 468 |
|
|---|
| 469 |
|
|---|
| 470 |
|
|---|
| 471 | gNCR == {
|
|---|
| 472 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 473 | TensorClass -> CKM,
|
|---|
| 474 | Hermitian -> True,
|
|---|
| 475 | Value -> {gNCR[1,1] -> 1-cw^2,
|
|---|
| 476 | gNCR[1,2] -> 0,
|
|---|
| 477 | gNCR[1,3] -> 0,
|
|---|
| 478 | gNCR[1,4] -> Sqrt[2]*yme/mtr*Ve,
|
|---|
| 479 | gNCR[2,1] -> 0,
|
|---|
| 480 | gNCR[2,2] -> 1-cw^2,
|
|---|
| 481 | gNCR[2,3] -> 0,
|
|---|
| 482 | gNCR[2,4] -> Sqrt[2]*ymm/mtr*Vm,
|
|---|
| 483 | gNCR[3,1] -> 0,
|
|---|
| 484 | gNCR[3,2] -> 0,
|
|---|
| 485 | gNCR[3,3] -> 1-cw^2,
|
|---|
| 486 | gNCR[3,4] -> Sqrt[2]*ymtau/mtr*Vtt,
|
|---|
| 487 | gNCR[4,1] -> Sqrt[2]*yme/mtr*Ve,
|
|---|
| 488 | gNCR[4,2] -> Sqrt[2]*ymm/mtr*Vm,
|
|---|
| 489 | gNCR[4,3] -> Sqrt[2]*ymtau/mtr*Vtt,
|
|---|
| 490 | gNCR[4,4] -> -cw^2},
|
|---|
| 491 | Description -> "gNCR-Matrix"},
|
|---|
| 492 |
|
|---|
| 493 |
|
|---|
| 494 |
|
|---|
| 495 |
|
|---|
| 496 |
|
|---|
| 497 |
|
|---|
| 498 | gNCnu == {
|
|---|
| 499 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 500 | TensorClass -> CKM,
|
|---|
| 501 | Hermitian -> True,
|
|---|
| 502 | Value -> {gNCnu[1,1] -> 1 - Cos[theta12] Cos[theta13] (Ve^2 Cos[theta12] Cos[theta13] +
|
|---|
| 503 | Ve Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 504 | Ve Vm (-Cos[theta23] Sin[theta12] -
|
|---|
| 505 | Cos[theta12] Sin[theta13] Sin[theta23])) - (-Cos[theta23] Sin[theta12] -
|
|---|
| 506 | Cos[theta12] Sin[theta13] Sin[theta23]) (Ve Vm Cos[theta12] Cos[theta13] +
|
|---|
| 507 | Vm Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 508 | Sin[theta12] Sin[theta23]) + Vm^2 (-Cos[theta23] Sin[theta12] -
|
|---|
| 509 | Cos[theta12] Sin[theta13] Sin[theta23])) - (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 510 | Sin[theta12] Sin[theta23]) (Ve Vtt Cos[theta12] Cos[theta13] +
|
|---|
| 511 | Vtt^2 (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 512 | Vm Vtt (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 513 | gNCnu[1,2] -> -Cos[theta13] Sin[theta12] (Ve^2 Cos[theta12] Cos[theta13] +
|
|---|
| 514 | Ve Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 515 | Ve Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])) - (Cos[theta12] Cos[theta23] -
|
|---|
| 516 | Sin[theta12] Sin[theta13] Sin[theta23]) (Ve Vm Cos[theta12] Cos[theta13] +
|
|---|
| 517 | Vm Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 518 | Vm^2 (-Cos[theta23] Sin[theta12] -
|
|---|
| 519 | Cos[theta12] Sin[theta13] Sin[theta23])) - (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 520 | Cos[theta12] Sin[theta23]) (Ve Vtt Cos[theta12] Cos[theta13] +
|
|---|
| 521 | Vtt^2 (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 522 | Vm Vtt (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 523 | gNCnu[1,3] -> -Sin[theta13] (Ve^2 Cos[theta12] Cos[theta13] + Ve Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 524 | Sin[theta12] Sin[theta23]) + Ve Vm (-Cos[theta23] Sin[theta12] -
|
|---|
| 525 | Cos[theta12] Sin[theta13] Sin[theta23])) - Cos[theta13] Sin[theta23] (Ve Vm Cos[theta12] Cos[theta13] +
|
|---|
| 526 | Vm Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 527 | Vm^2 (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])) -
|
|---|
| 528 | Cos[theta13] Cos[theta23] (Ve Vtt Cos[theta12] Cos[theta13] +
|
|---|
| 529 | Vtt^2 (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 530 | Vm Vtt (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 531 | gNCnu[1,4] -> Ve Cos[theta12] Cos[theta13] + Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 532 | Sin[theta12] Sin[theta23]) + Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23]),
|
|---|
| 533 | gNCnu[2,1] -> -Cos[theta12] Cos[theta13] (Ve^2 Cos[theta13] Sin[theta12] +
|
|---|
| 534 | Ve Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 535 | Ve Vm (Cos[theta12] Cos[theta23] -
|
|---|
| 536 | Sin[theta12] Sin[theta13] Sin[theta23])) - (-Cos[theta23] Sin[theta12] -
|
|---|
| 537 | Cos[theta12] Sin[theta13] Sin[theta23]) (Ve Vm Cos[theta13] Sin[theta12] +
|
|---|
| 538 | Vm Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 539 | Vm^2 (Cos[theta12] Cos[theta23] -
|
|---|
| 540 | Sin[theta12] Sin[theta13] Sin[theta23])) - (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 541 | Sin[theta12] Sin[theta23]) (Ve Vtt Cos[theta13] Sin[theta12] +
|
|---|
| 542 | Vtt^2 (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 543 | Vm Vtt (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 544 | gNCnu[2,2] -> 1 - Cos[theta13] Sin[theta12] (Ve^2 Cos[theta13] Sin[theta12] +
|
|---|
| 545 | Ve Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 546 | Ve Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])) - (Cos[theta12] Cos[theta23] -
|
|---|
| 547 | Sin[theta12] Sin[theta13] Sin[theta23]) (Ve Vm Cos[theta13] Sin[theta12] +
|
|---|
| 548 | Vm Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 549 | Vm^2 (Cos[theta12] Cos[theta23] -
|
|---|
| 550 | Sin[theta12] Sin[theta13] Sin[theta23])) - (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 551 | Cos[theta12] Sin[theta23]) (Ve Vtt Cos[theta13] Sin[theta12] +
|
|---|
| 552 | Vtt^2 (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 553 | Vm Vtt (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 554 | gNCnu[2,3] -> -Sin[theta13] (Ve^2 Cos[theta13] Sin[theta12] +
|
|---|
| 555 | Ve Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 556 | Ve Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])) -
|
|---|
| 557 | Cos[theta13] Sin[theta23] (Ve Vm Cos[theta13] Sin[theta12] +
|
|---|
| 558 | Vm Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 559 | Vm^2 (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])) -
|
|---|
| 560 | Cos[theta13] Cos[theta23] (Ve Vtt Cos[theta13] Sin[theta12] +
|
|---|
| 561 | Vtt^2 (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 562 | Vm Vtt (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 563 | gNCnu[2,4] -> Ve Cos[theta13] Sin[theta12] + Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 564 | Cos[theta12] Sin[theta23]) + Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]),
|
|---|
| 565 | gNCnu[3,1] -> -Cos[theta12] Cos[theta13] (Ve Vtt Cos[theta13] Cos[theta23] + Ve^2 Sin[theta13] +
|
|---|
| 566 | Ve Vm Cos[theta13] Sin[theta23]) - (Vtt^2 Cos[theta13] Cos[theta23] + Ve Vtt Sin[theta13] +
|
|---|
| 567 | Vm Vtt Cos[theta13] Sin[theta23]) (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 568 | Sin[theta12] Sin[theta23]) - (Vm Vtt Cos[theta13] Cos[theta23] + Ve Vm Sin[theta13] +
|
|---|
| 569 | Vm^2 Cos[theta13] Sin[theta23]) (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23]),
|
|---|
| 570 | gNCnu[3,2] -> -Cos[theta13] Sin[theta12] (Ve Vtt Cos[theta13] Cos[theta23] + Ve^2 Sin[theta13] +
|
|---|
| 571 | Ve Vm Cos[theta13] Sin[theta23]) - (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 572 | Cos[theta12] Sin[theta23]) (Vtt^2 Cos[theta13] Cos[theta23] + Ve Vtt Sin[theta13] +
|
|---|
| 573 | Vm Vtt Cos[theta13] Sin[theta23]) - (Vm Vtt Cos[theta13] Cos[theta23] + Ve Vm Sin[theta13] +
|
|---|
| 574 | Vm^2 Cos[theta13] Sin[theta23]) (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]),
|
|---|
| 575 | gNCnu[3,3] -> 1 - Sin[theta13] (Ve Vtt Cos[theta13] Cos[theta23] +
|
|---|
| 576 | Ve^2 Sin[theta13] + Ve Vm Cos[theta13] Sin[theta23]) -
|
|---|
| 577 | Cos[theta13] Sin[theta23] (Vm Vtt Cos[theta13] Cos[theta23] + Ve Vm Sin[theta13] +
|
|---|
| 578 | Vm^2 Cos[theta13] Sin[theta23]) -
|
|---|
| 579 | Cos[theta13] Cos[theta23] (Vtt^2 Cos[theta13] Cos[theta23] + Ve Vtt Sin[theta13] +
|
|---|
| 580 | Vm Vtt Cos[theta13] Sin[theta23]),
|
|---|
| 581 | gNCnu[3,4] -> Vtt Cos[theta13] Cos[theta23] + Ve Sin[theta13] + Vm Cos[theta13] Sin[theta23],
|
|---|
| 582 | gNCnu[4,1] -> Ve Cos[theta12] Cos[theta13] + Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 583 | Sin[theta12] Sin[theta23]) + Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23]),
|
|---|
| 584 | gNCnu[4,2] -> Ve Cos[theta13] Sin[theta12] + Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 585 | Cos[theta12] Sin[theta23]) + Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]),
|
|---|
| 586 | gNCnu[4,3] -> Vtt Cos[theta13] Cos[theta23] + Ve Sin[theta13] + Vm Cos[theta13] Sin[theta23],
|
|---|
| 587 | gNCnu[4,4] -> Ve^2 + Vm^2 + Vtt^2},
|
|---|
| 588 | Description -> "gNCnu-Matrix"},
|
|---|
| 589 |
|
|---|
| 590 |
|
|---|
| 591 |
|
|---|
| 592 |
|
|---|
| 593 | gHlR == {
|
|---|
| 594 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 595 | TensorClass -> CKM,
|
|---|
| 596 | ComplexParameter -> False,
|
|---|
| 597 | Value -> {gHlR[1,1] -> yme/v*(1-3*Ve^2),
|
|---|
| 598 | gHlR[2,1] -> -3*yme/v*Ve*Vm,
|
|---|
| 599 | gHlR[3,1] -> -3*yme/v*Ve*Vtt,
|
|---|
| 600 | gHlR[4,1] -> Sqrt[2]*yme/v*Ve,
|
|---|
| 601 | gHlR[1,2] -> -3*ymm/v*Ve*Vm,
|
|---|
| 602 | gHlR[2,2] -> ymm/v*(1-3*Vm^2),
|
|---|
| 603 | gHlR[3,2] -> -3*ymm/v*Vm*Vtt,
|
|---|
| 604 | gHlR[4,2] -> Sqrt[2]*ymm/v*Vm,
|
|---|
| 605 | gHlR[1,3] -> -3*ymtau/v*Ve*Vtt,
|
|---|
| 606 | gHlR[2,3] -> -3*ymtau/v*Vm*Vtt,
|
|---|
| 607 | gHlR[3,3] -> ymtau/v*(1-3*Vtt^2),
|
|---|
| 608 | gHlR[4,3] -> Sqrt[2]*ymtau/v*Vtt,
|
|---|
| 609 | gHlR[1,4] -> Sqrt[2]*mtr/v*Ve*(1-Ve^2-Vm^2-Vtt^2)+Sqrt[2]*yme^2/v/mtr*Ve,
|
|---|
| 610 | gHlR[2,4] -> Sqrt[2]*mtr/v*Vm*(1-Ve^2-Vm^2-Vtt^2)+Sqrt[2]*ymm^2/v/mtr*Vm,
|
|---|
| 611 | gHlR[3,4] -> Sqrt[2]*mtr/v*Vtt*(1-Ve^2-Vm^2-Vtt^2)+Sqrt[2]*ymtau^2/v/mtr*Vtt,
|
|---|
| 612 | gHlR[4,4] -> 2*mtr/v*(Ve^2+Vm^2+Vtt^2)},
|
|---|
| 613 | InteractionOrder -> {QED, 1},
|
|---|
| 614 | Description -> "gHlR-Matrix"},
|
|---|
| 615 |
|
|---|
| 616 |
|
|---|
| 617 |
|
|---|
| 618 |
|
|---|
| 619 | getalR == {
|
|---|
| 620 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 621 | TensorClass -> CKM,
|
|---|
| 622 | ComplexParameter -> False,
|
|---|
| 623 | Value -> {getalR[1,1] -> yme/v*(1+Ve^2),
|
|---|
| 624 | getalR[2,1] -> yme/v*Ve*Vm,
|
|---|
| 625 | getalR[3,1] -> yme/v*Ve*Vtt,
|
|---|
| 626 | getalR[4,1] -> Sqrt[2]*yme/v*Ve,
|
|---|
| 627 | getalR[1,2] -> ymm/v*Ve*Vm,
|
|---|
| 628 | getalR[2,2] -> ymm/v*(1+Vm^2),
|
|---|
| 629 | getalR[3,2] -> ymm/v*Vm*Vtt,
|
|---|
| 630 | getalR[4,2] -> Sqrt[2]*ymm/v*Vm,
|
|---|
| 631 | getalR[1,3] -> ymtau/v*Ve*Vtt,
|
|---|
| 632 | getalR[2,3] -> ymtau/v*Vm*Vtt,
|
|---|
| 633 | getalR[3,3] -> ymtau/v*(1+Vtt^2),
|
|---|
| 634 | getalR[4,3] -> Sqrt[2]*ymtau/v*Vtt,
|
|---|
| 635 | getalR[1,4] -> -Sqrt[2]*mtr/v*Ve*(1-Ve^2-Vm^2-Vtt^2)+Sqrt[2]*yme^2/v/mtr*Ve,
|
|---|
| 636 | getalR[2,4] -> -Sqrt[2]*mtr/v*Vm*(1-Ve^2-Vm^2-Vtt^2)+Sqrt[2]*ymm^2/v/mtr*Vm,
|
|---|
| 637 | getalR[3,4] -> -Sqrt[2]*mtr/v*Vtt*(1-Ve^2-Vm^2-Vtt^2)+Sqrt[2]*ymtau^2/v/mtr*Vtt,
|
|---|
| 638 | getalR[4,4] -> -2*mtr/v*(Ve^2+Vm^2+Vtt^2)},
|
|---|
| 639 | InteractionOrder -> {QED, 1},
|
|---|
| 640 | Description -> "getalR-Matrix"},
|
|---|
| 641 |
|
|---|
| 642 |
|
|---|
| 643 |
|
|---|
| 644 |
|
|---|
| 645 | gHnuR == {
|
|---|
| 646 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 647 | TensorClass -> CKM,
|
|---|
| 648 | ComplexParameter -> False,
|
|---|
| 649 | Value -> {gHnuR[1,1] -> Sqrt[2]/v*mv1,
|
|---|
| 650 | gHnuR[2,1] -> 0,
|
|---|
| 651 | gHnuR[3,1] -> 0,
|
|---|
| 652 | gHnuR[4,1] -> Sqrt[2]/v*mv1*(Ve Cos[theta12] Cos[theta13] + Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 653 | Sin[theta12] Sin[theta23]) + Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 654 | gHnuR[1,2] -> 0,
|
|---|
| 655 | gHnuR[2,2] -> Sqrt[2]/v*mv2,
|
|---|
| 656 | gHnuR[3,2] -> 0,
|
|---|
| 657 | gHnuR[4,2] -> Sqrt[2]/v*mv2*(Ve Cos[theta13] Sin[theta12] + Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 658 | Cos[theta12] Sin[theta23]) + Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 659 | gHnuR[1,3] -> 0,
|
|---|
| 660 | gHnuR[2,3] -> 0,
|
|---|
| 661 | gHnuR[3,3] -> Sqrt[2]/v*mv3,
|
|---|
| 662 | gHnuR[4,3] -> Sqrt[2]/v*mv3*(Vtt Cos[theta13] Cos[theta23] + Ve Sin[theta13] + Vm Cos[theta13] Sin[theta23]),
|
|---|
| 663 | gHnuR[1,4] -> Sqrt[2]*mtr/v*(-(-1 + Ve^2 + Vm^2 + Vtt^2) (Sin[theta12] (-Vm Cos[theta23] + Vtt Sin[theta23]) +
|
|---|
| 664 | Cos[theta12] (Ve Cos[theta13] - Sin[theta13] (Vtt Cos[theta23] + Vm Sin[theta23])))),
|
|---|
| 665 | gHnuR[2,4] -> Sqrt[2]*mtr/v*(-(-1 + Ve^2 + Vm^2 + Vtt^2) (Cos[theta12] (Vm Cos[theta23] - Vtt Sin[theta23]) +
|
|---|
| 666 | Sin[theta12] (Ve Cos[theta13] - Sin[theta13] (Vtt Cos[theta23] + Vm Sin[theta23])))),
|
|---|
| 667 | gHnuR[3,4] -> Sqrt[2]*mtr/v*(-(-1 + Ve^2 + Vm^2 + Vtt^2) (Ve Sin[theta13] + Cos[theta13] (Vtt Cos[theta23] + Vm Sin[theta23]))),
|
|---|
| 668 | gHnuR[4,4] -> Sqrt[2]*mtr/v*(Ve^2+Vm^2+Vtt^2)},
|
|---|
| 669 | InteractionOrder -> {QED, 1},
|
|---|
| 670 | Description -> "gHnuR-Matrix"},
|
|---|
| 671 |
|
|---|
| 672 |
|
|---|
| 673 |
|
|---|
| 674 |
|
|---|
| 675 |
|
|---|
| 676 | getanuR == {
|
|---|
| 677 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 678 | TensorClass -> CKM,
|
|---|
| 679 | ComplexParameter -> False,
|
|---|
| 680 | Value -> {getanuR[1,1] -> -Sqrt[2]/v*mv1,
|
|---|
| 681 | getanuR[2,1] -> 0,
|
|---|
| 682 | getanuR[3,1] -> 0,
|
|---|
| 683 | getanuR[4,1] -> -(Sqrt[2]/v*mv1*(Ve Cos[theta12] Cos[theta13] + Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 684 | Sin[theta12] Sin[theta23]) + Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23]))),
|
|---|
| 685 | getanuR[1,2] -> 0,
|
|---|
| 686 | getanuR[2,2] -> -Sqrt[2]/v*mv2,
|
|---|
| 687 | getanuR[3,2] -> 0,
|
|---|
| 688 | getanuR[4,2] -> -(Sqrt[2]/v*mv2*(Ve Cos[theta13] Sin[theta12] + Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 689 | Cos[theta12] Sin[theta23]) + Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]))),
|
|---|
| 690 | getanuR[1,3] -> 0,
|
|---|
| 691 | getanuR[2,3] -> 0,
|
|---|
| 692 | getanuR[3,3] -> -Sqrt[2]/v*mv3,
|
|---|
| 693 | getanuR[4,3] -> -(Sqrt[2]/v*mv3*(Vtt Cos[theta13] Cos[theta23] + Ve Sin[theta13] + Vm Cos[theta13] Sin[theta23])),
|
|---|
| 694 | getanuR[1,4] -> -(Sqrt[2]*mtr/v*(-(-1 + Ve^2 + Vm^2 + Vtt^2) (Sin[theta12] (-Vm Cos[theta23] + Vtt Sin[theta23]) +
|
|---|
| 695 | Cos[theta12] (Ve Cos[theta13] - Sin[theta13] (Vtt Cos[theta23] + Vm Sin[theta23]))))),
|
|---|
| 696 | getanuR[2,4] -> -(Sqrt[2]*mtr/v*(-(-1 + Ve^2 + Vm^2 + Vtt^2) (Cos[theta12] (Vm Cos[theta23] - Vtt Sin[theta23]) +
|
|---|
| 697 | Sin[theta12] (Ve Cos[theta13] - Sin[theta13] (Vtt Cos[theta23] + Vm Sin[theta23]))))),
|
|---|
| 698 | getanuR[3,4] -> -(Sqrt[2]*mtr/v*(-(-1 + Ve^2 + Vm^2 + Vtt^2) (Ve Sin[theta13] + Cos[theta13] (Vtt Cos[theta23] + Vm Sin[theta23])))),
|
|---|
| 699 | getanuR[4,4] -> -(Sqrt[2]*mtr/v*(Ve^2+Vm^2+Vtt^2))},
|
|---|
| 700 | InteractionOrder -> {QED, 1},
|
|---|
| 701 | Description -> "getanuR-Matrix"},
|
|---|
| 702 |
|
|---|
| 703 |
|
|---|
| 704 |
|
|---|
| 705 | gPhiL == {
|
|---|
| 706 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 707 | TensorClass -> CKM,
|
|---|
| 708 | ComplexParameter -> False,
|
|---|
| 709 | Value -> {gPhiL[1,1] -> Sqrt[2]/v*yme*((1 - Ve^2/2) Cos[theta12] Cos[theta13] -
|
|---|
| 710 | 1/2 Ve Vtt (Sin[theta12] Sin[theta23] - Cos[theta12] Cos[theta23] Sin[theta13]) -
|
|---|
| 711 | 1/2 Ve Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 712 | gPhiL[1,2] -> Sqrt[2]/v*yme*((1 - Ve^2/2) Cos[theta13] Sin[theta12] -
|
|---|
| 713 | 1/2 Ve Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) -
|
|---|
| 714 | 1/2 Ve Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 715 | gPhiL[1,3] -> Sqrt[2]/v*yme*( (1 - Ve^2/2) Sin[theta13] -
|
|---|
| 716 | 1/2 Ve Vtt Cos[theta13] Cos[theta23] - 1/2 Ve Vm Cos[theta13] Sin[theta23] ),
|
|---|
| 717 | gPhiL[1,4] -> Sqrt[2]/v*yme Ve,
|
|---|
| 718 | gPhiL[2,1] -> Sqrt[2]/v*ymm*( (1 - Vm^2/2) (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23]) -
|
|---|
| 719 | 1/2 Ve Vm Cos[theta12] Cos[theta13] -
|
|---|
| 720 | 1/2 Vm Vtt (Sin[theta12] Sin[theta23] - Cos[theta12] Cos[theta23] Sin[theta13])),
|
|---|
| 721 | gPhiL[2,2] -> Sqrt[2]/v*ymm*( (1 - Vm^2/2) (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]) -
|
|---|
| 722 | 1/2 Ve Vm Cos[theta13] Sin[theta12] -
|
|---|
| 723 | 1/2 Vm Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23])),
|
|---|
| 724 | gPhiL[2,3] -> Sqrt[2]/v*ymm*( (1 - Vm^2/2) Cos[theta13] Sin[theta23] -
|
|---|
| 725 | 1/2 Vm Vtt Cos[theta13] Cos[theta23] - 1/2 Ve Vm Sin[theta13]),
|
|---|
| 726 | gPhiL[2,4] -> Sqrt[2]/v* ymm Vm,
|
|---|
| 727 | gPhiL[3,1] -> Sqrt[2]/v*ymtau*( (1 - Vtt^2/2) (Sin[theta12] Sin[theta23] - Cos[theta12] Cos[theta23] Sin[theta13]) -
|
|---|
| 728 | 1/2 Ve Vtt Cos[theta12] Cos[theta13] -
|
|---|
| 729 | 1/2 Vm Vtt (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 730 | gPhiL[3,2] -> Sqrt[2]/v*ymtau*( (1 - Vtt^2/2) (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) -
|
|---|
| 731 | 1/2 Ve Vtt Cos[theta13] Sin[theta12] -
|
|---|
| 732 | 1/2 Vm Vtt (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 733 | gPhiL[3,3] -> Sqrt[2]/v*ymtau*( (1 - Vtt^2/2) Cos[theta13] Cos[theta23] -
|
|---|
| 734 | 1/2 Ve Vtt Sin[theta13] - 1/2 Vm Vtt Cos[theta13] Sin[theta23]),
|
|---|
| 735 | gPhiL[3,4] -> Sqrt[2]/v* ymtau Vtt,
|
|---|
| 736 | gPhiL[4,1] -> 2/(mtr*v)*(Ve Cos[theta12] Cos[theta13] yme^2 +
|
|---|
| 737 | ymtau^2 Vtt (Sin[theta12] Sin[theta23]-Cos[theta12] Cos[theta23] Sin[theta13]) +
|
|---|
| 738 | ymm^2 Vm (-Cos[theta23] Sin[theta12]-Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 739 | gPhiL[4,2] -> 2/(mtr*v)*(Ve Cos[theta13] Sin[theta12] yme^2 +
|
|---|
| 740 | ymtau^2 Vtt (-Cos[theta23] Sin[theta12] Sin[theta13]-Cos[theta12] Sin[theta23]) +
|
|---|
| 741 | ymm^2 Vm (Cos[theta12] Cos[theta23]-Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 742 | gPhiL[4,3] -> 2/(mtr*v)*(Ve Sin[theta13] yme^2 + ymtau^2 Vtt Cos[theta13] Cos[theta23] + ymm^2 Vm Cos[theta13] Sin[theta23]),
|
|---|
| 743 | gPhiL[4,4] -> 0 },
|
|---|
| 744 | Description -> "gPhiL-Matrix"},
|
|---|
| 745 |
|
|---|
| 746 |
|
|---|
| 747 |
|
|---|
| 748 | gPhiR == {
|
|---|
| 749 | Indices -> {Index[LeptonGeneration], Index[LeptonGeneration]},
|
|---|
| 750 | TensorClass -> CKM,
|
|---|
| 751 | ComplexParameter -> False,
|
|---|
| 752 | Value -> {gPhiR[1,1] -> -Sqrt[2]/v*(mv1 Cos[theta12] Cos[theta13]),
|
|---|
| 753 | gPhiR[1,2] -> -Sqrt[2]/v*(mv2 Cos[theta13] Sin[theta12]),
|
|---|
| 754 | gPhiR[1,3] -> -Sqrt[2]/v*(mv3 Sin[theta13]),
|
|---|
| 755 | gPhiR[1,4] -> (mtr/v*Sqrt[2])*(-1/2 Ve (3 Ve^2 + 3 Vm^2 + 3 Vtt^2 - 2)) -
|
|---|
| 756 | 2/v*Sqrt[2]( mv3 Sin[theta13] (Vtt Cos[theta13] Cos[theta23] + Ve Sin[theta13] + Vm Cos[theta13] Sin[theta23]) +
|
|---|
| 757 | mv1 Cos[theta12] Cos[theta13] (Ve Cos[theta12] Cos[theta13] + Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] +
|
|---|
| 758 | Sin[theta12] Sin[theta23]) + Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])) +
|
|---|
| 759 | mv2 Cos[theta13] Sin[theta12] (Ve Cos[theta13] Sin[theta12] + Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] -
|
|---|
| 760 | Cos[theta12] Sin[theta23]) + Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]))),
|
|---|
| 761 | gPhiR[2,1] -> -Sqrt[2]/v*(mv1 (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 762 | gPhiR[2,2] -> -Sqrt[2]/v*(mv2 (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23])),
|
|---|
| 763 | gPhiR[2,3] -> -Sqrt[2]/v*(mv3 Cos[theta13] Sin[theta23]),
|
|---|
| 764 | gPhiR[2,4] -> (mtr/v*Sqrt[2])*(-1/2 Vm (3 Ve^2 + 3 Vm^2 + 3 Vtt^2 - 2)) -
|
|---|
| 765 | 2/v*Sqrt[2] (
|
|---|
| 766 | mv3 Cos[theta13] Sin[theta23] (Vtt Cos[theta13] Cos[theta23] + Ve Sin[theta13] + Vm Cos[theta13] Sin[theta23]) +
|
|---|
| 767 | mv1 (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23]) (Ve Cos[theta12] Cos[theta13] +
|
|---|
| 768 | Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 769 | Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])) +
|
|---|
| 770 | mv2 (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]) (Ve Cos[theta13] Sin[theta12] +
|
|---|
| 771 | Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 772 | Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]))),
|
|---|
| 773 | gPhiR[3,1] -> -Sqrt[2]/v*(mv1 (Sin[theta12] Sin[theta23] - Cos[theta12] Cos[theta23] Sin[theta13])),
|
|---|
| 774 | gPhiR[3,2] -> -Sqrt[2]/v*(mv2 (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23])),
|
|---|
| 775 | gPhiR[3,3] -> -Sqrt[2]/v*(mv3 Cos[theta13] Cos[theta23]),
|
|---|
| 776 | gPhiR[3,4] -> (mtr/v*Sqrt[2])*(-1/2 Vtt (3 Ve^2 + 3 Vm^2 + 3 Vtt^2 - 2)) -
|
|---|
| 777 | 2/v*Sqrt[2] (
|
|---|
| 778 | mv3 Cos[theta13] Cos[theta23] (Vtt Cos[theta13] Cos[theta23] + Ve Sin[theta13] + Vm Cos[theta13] Sin[theta23]) +
|
|---|
| 779 | mv1 (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) (Ve Cos[theta12] Cos[theta13] +
|
|---|
| 780 | Vtt (-Cos[theta12] Cos[theta23] Sin[theta13] + Sin[theta12] Sin[theta23]) +
|
|---|
| 781 | Vm (-Cos[theta23] Sin[theta12] - Cos[theta12] Sin[theta13] Sin[theta23])) +
|
|---|
| 782 | mv2 (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) (Ve Cos[theta13] Sin[theta12] +
|
|---|
| 783 | Vtt (-Cos[theta23] Sin[theta12] Sin[theta13] - Cos[theta12] Sin[theta23]) +
|
|---|
| 784 | Vm (Cos[theta12] Cos[theta23] - Sin[theta12] Sin[theta13] Sin[theta23]))),
|
|---|
| 785 | gPhiR[4,1] -> mtr/v*( (Ve^2 + Vm^2 + Vtt^2 - 2) (Sin[theta12] (Vtt Sin[theta23] - Vm Cos[theta23]) +
|
|---|
| 786 | Cos[theta12] (Ve Cos[theta13] - Sin[theta13] (Vtt Cos[theta23] + Vm Sin[theta23])))),
|
|---|
| 787 | gPhiR[4,2] -> mtr/v*( (Ve^2 + Vm^2 + Vtt^2 - 2) (Cos[theta12] (Vm Cos[theta23] - Vtt Sin[theta23]) +
|
|---|
| 788 | Sin[theta12] (Ve Cos[theta13] - Sin[theta13] (Vtt Cos[theta23] + Vm Sin[theta23])))),
|
|---|
| 789 | gPhiR[4,3] -> mtr/v*( (Ve^2 + Vm^2 + Vtt^2 - 2) (Ve Sin[theta13] + Cos[theta13] (Vtt Cos[theta23] + Vm Sin[theta23]))),
|
|---|
| 790 | gPhiR[4,4] -> 0 },
|
|---|
| 791 | Description -> "gPhiR-Matrix"}
|
|---|
| 792 |
|
|---|
| 793 |
|
|---|
| 794 |
|
|---|
| 795 |
|
|---|
| 796 | }
|
|---|
| 797 |
|
|---|
| 798 |
|
|---|
| 799 | (************** Gauge Groups ******************)
|
|---|
| 800 |
|
|---|
| 801 | M$GaugeGroups = {
|
|---|
| 802 |
|
|---|
| 803 | U1Y == {
|
|---|
| 804 | Abelian -> True,
|
|---|
| 805 | GaugeBoson -> B,
|
|---|
| 806 | Charge -> Y,
|
|---|
| 807 | CouplingConstant -> g1},
|
|---|
| 808 |
|
|---|
| 809 | SU2L == {
|
|---|
| 810 | Abelian -> False,
|
|---|
| 811 | GaugeBoson -> Wi,
|
|---|
| 812 | StructureConstant -> Eps,
|
|---|
| 813 | CouplingConstant -> gw},
|
|---|
| 814 |
|
|---|
| 815 | SU3C == {
|
|---|
| 816 | Abelian -> False,
|
|---|
| 817 | GaugeBoson -> G,
|
|---|
| 818 | StructureConstant -> f,
|
|---|
| 819 | SymmetricTensor -> dSUN,
|
|---|
| 820 | Representations -> {T, Colour},
|
|---|
| 821 | CouplingConstant -> gs}
|
|---|
| 822 | }
|
|---|
| 823 |
|
|---|
| 824 | (********* Particle Classes **********)
|
|---|
| 825 |
|
|---|
| 826 | M$ClassesDescription = {
|
|---|
| 827 |
|
|---|
| 828 | (********** Fermions ************)
|
|---|
| 829 | (* Leptons (neutrino): I_3 = +1/2, Q = 0 *)
|
|---|
| 830 | F[1] == {
|
|---|
| 831 | ClassName -> vl,
|
|---|
| 832 | ClassMembers -> {v1,v2,v3,tr0},
|
|---|
| 833 | FlavorIndex -> LeptonGeneration,
|
|---|
| 834 | SelfConjugate -> True,
|
|---|
| 835 | Indices -> {Index[LeptonGeneration]},
|
|---|
| 836 | Mass -> {Mv, {Mv1, 0}, {Mv2, 0}, {Mv3, 0}, {Mtr0, 100.8}},
|
|---|
| 837 | Width -> {0, 0, 0, {Wtr0, 0.1}},
|
|---|
| 838 | PropagatorLabel -> {"v", "v1", "v2", "v3","tr0"} ,
|
|---|
| 839 | PropagatorType -> S,
|
|---|
| 840 | PropagatorArrow -> Forward,
|
|---|
| 841 | PDG -> {8000012,8000014,8000016,8000018},
|
|---|
| 842 | FullName -> {"nu1", "nu2", "nu3", "Sigma0"} },
|
|---|
| 843 |
|
|---|
| 844 | (* Leptons (electron): I_3 = -1/2, Q = -1 *)
|
|---|
| 845 | F[2] == {
|
|---|
| 846 | ClassName -> l,
|
|---|
| 847 | ClassMembers -> {e, m, tt,trm},
|
|---|
| 848 | FlavorIndex -> LeptonGeneration,
|
|---|
| 849 | SelfConjugate -> False,
|
|---|
| 850 | Indices -> {Index[LeptonGeneration]},
|
|---|
| 851 | Mass -> {Ml, {Me, 5.11 * 10^(-4)}, {MM, 0.10566}, {MTA, 1.777}, {Mtrch, 101}},
|
|---|
| 852 | Width -> {0, 0, {Wtau, 0.1}, {Wtrch, 0.1}},
|
|---|
| 853 | QuantumNumbers -> {Q -> -1},
|
|---|
| 854 | PropagatorLabel -> {"l", "e", "m", "tt", "tr-"},
|
|---|
| 855 | PropagatorType -> Straight,
|
|---|
| 856 | ParticleName -> {"e-", "m-", "tt-", "tr-"},
|
|---|
| 857 | AntiParticleName -> {"e+", "m+", "tt+", "tr+"},
|
|---|
| 858 | PropagatorArrow -> Forward,
|
|---|
| 859 | PDG -> {11, 13, 15,8000020},
|
|---|
| 860 | FullName -> {"Electron", "Muon", "Tau", "Sigma-"} },
|
|---|
| 861 |
|
|---|
| 862 | (* Quarks (u): I_3 = +1/2, Q = +2/3 *)
|
|---|
| 863 | F[3] == {
|
|---|
| 864 | ClassMembers -> {u, c, t},
|
|---|
| 865 | ClassName -> uq,
|
|---|
| 866 | FlavorIndex -> Generation,
|
|---|
| 867 | SelfConjugate -> False,
|
|---|
| 868 | Indices -> {Index[Generation], Index[Colour]},
|
|---|
| 869 | Mass -> {Mu, {MU, 2.55*10^(-3)}, {MC, 1.42}, {MT, 174.3}},
|
|---|
| 870 | Width -> {0, {WC, 0.1}, {WT, 1.50833649}},
|
|---|
| 871 | QuantumNumbers -> {Q -> 2/3},
|
|---|
| 872 | PropagatorLabel -> {"uq", "u", "c", "t"},
|
|---|
| 873 | PropagatorType -> Straight,
|
|---|
| 874 | PropagatorArrow -> Forward,
|
|---|
| 875 | PDG -> {2, 4, 6},
|
|---|
| 876 | FullName -> {"u-quark", "c-quark", "t-quark"}},
|
|---|
| 877 |
|
|---|
| 878 | (* Quarks (d): I_3 = -1/2, Q = -1/3 *)
|
|---|
| 879 | F[4] == {
|
|---|
| 880 | ClassMembers -> {d, s, b},
|
|---|
| 881 | ClassName -> dq,
|
|---|
| 882 | FlavorIndex -> Generation,
|
|---|
| 883 | SelfConjugate -> False,
|
|---|
| 884 | Indices -> {Index[Generation], Index[Colour]},
|
|---|
| 885 | Mass -> {Md, {MD, 5.04*10^(-3)}, {MS, 0.104}, {MB, 4.7}},
|
|---|
| 886 | Width -> {0, 0, {WB, 0.1}},
|
|---|
| 887 | QuantumNumbers -> {Q -> -1/3},
|
|---|
| 888 | PropagatorLabel -> {"dq", "d", "s", "b"},
|
|---|
| 889 | PropagatorType -> Straight,
|
|---|
| 890 | PropagatorArrow -> Forward,
|
|---|
| 891 | PDG -> {1,3,5},
|
|---|
| 892 | FullName -> {"d-quark", "s-quark", "b-quark"} },
|
|---|
| 893 |
|
|---|
| 894 | (********** Ghosts **********)
|
|---|
| 895 | U[1] == {
|
|---|
| 896 | ClassName -> ghA,
|
|---|
| 897 | SelfConjugate -> False,
|
|---|
| 898 | Indices -> {},
|
|---|
| 899 | Ghost -> A,
|
|---|
| 900 | Mass -> 0,
|
|---|
| 901 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 902 | PropagatorLabel -> uA,
|
|---|
| 903 | PropagatorType -> GhostDash,
|
|---|
| 904 | PropagatorArrow -> Forward},
|
|---|
| 905 |
|
|---|
| 906 | U[2] == {
|
|---|
| 907 | ClassName -> ghZ,
|
|---|
| 908 | SelfConjugate -> False,
|
|---|
| 909 | Indices -> {},
|
|---|
| 910 | Mass -> {MZ, 91.188},
|
|---|
| 911 | Ghost -> Z,
|
|---|
| 912 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 913 | PropagatorLabel -> uZ,
|
|---|
| 914 | PropagatorType -> GhostDash,
|
|---|
| 915 | PropagatorArrow -> Forward},
|
|---|
| 916 |
|
|---|
| 917 | U[31] == {
|
|---|
| 918 | ClassName -> ghWp,
|
|---|
| 919 | SelfConjugate -> False,
|
|---|
| 920 | Indices -> {},
|
|---|
| 921 | Mass -> {MW, Internal},
|
|---|
| 922 | Ghost -> W,
|
|---|
| 923 | QuantumNumbers -> {Q-> 1, GhostNumber -> 1},
|
|---|
| 924 | PropagatorLabel -> uWp,
|
|---|
| 925 | PropagatorType -> GhostDash,
|
|---|
| 926 | PropagatorArrow -> Forward},
|
|---|
| 927 |
|
|---|
| 928 | U[32] == {
|
|---|
| 929 | ClassName -> ghWm,
|
|---|
| 930 | SelfConjugate -> False,
|
|---|
| 931 | Indices -> {},
|
|---|
| 932 | Mass -> {MW, Internal},
|
|---|
| 933 | Ghost -> Wbar,
|
|---|
| 934 | QuantumNumbers -> {Q-> -1, GhostNumber -> 1},
|
|---|
| 935 | PropagatorLabel -> uWm,
|
|---|
| 936 | PropagatorType -> GhostDash,
|
|---|
| 937 | PropagatorArrow -> Forward},
|
|---|
| 938 |
|
|---|
| 939 | U[4] == {
|
|---|
| 940 | ClassName -> ghG,
|
|---|
| 941 | SelfConjugate -> False,
|
|---|
| 942 | Indices -> {Index[Gluon]},
|
|---|
| 943 | Ghost -> G,
|
|---|
| 944 | Mass -> 0,
|
|---|
| 945 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 946 | PropagatorLabel -> uG,
|
|---|
| 947 | PropagatorType -> GhostDash,
|
|---|
| 948 | PropagatorArrow -> Forward},
|
|---|
| 949 |
|
|---|
| 950 | U[5] == {
|
|---|
| 951 | ClassName -> ghWi,
|
|---|
| 952 | Unphysical -> True,
|
|---|
| 953 | Definitions -> {ghWi[1] -> (ghWp + ghWm)/Sqrt[2],
|
|---|
| 954 | ghWi[2] -> (ghWm - ghWp)/Sqrt[2]/I,
|
|---|
| 955 | ghWi[3] -> cw ghZ + sw ghA},
|
|---|
| 956 | SelfConjugate -> False,
|
|---|
| 957 | Ghost -> Wi,
|
|---|
| 958 | Indices -> {Index[SU2W]},
|
|---|
| 959 | FlavorIndex -> SU2W},
|
|---|
| 960 |
|
|---|
| 961 | U[6] == {
|
|---|
| 962 | ClassName -> ghB,
|
|---|
| 963 | SelfConjugate -> False,
|
|---|
| 964 | Definitions -> {ghB -> -sw ghZ + cw ghA},
|
|---|
| 965 | Indices -> {},
|
|---|
| 966 | Ghost -> B,
|
|---|
| 967 | Unphysical -> True},
|
|---|
| 968 |
|
|---|
| 969 | (************ Gauge Bosons ***************)
|
|---|
| 970 | (* Gauge bosons: Q = 0 *)
|
|---|
| 971 | V[1] == {
|
|---|
| 972 | ClassName -> A,
|
|---|
| 973 | SelfConjugate -> True,
|
|---|
| 974 | Indices -> {},
|
|---|
| 975 | Mass -> 0,
|
|---|
| 976 | Width -> 0,
|
|---|
| 977 | PropagatorLabel -> "a",
|
|---|
| 978 | PropagatorType -> W,
|
|---|
| 979 | PropagatorArrow -> None,
|
|---|
| 980 | PDG -> 22,
|
|---|
| 981 | FullName -> "Photon" },
|
|---|
| 982 |
|
|---|
| 983 | V[2] == {
|
|---|
| 984 | ClassName -> Z,
|
|---|
| 985 | SelfConjugate -> True,
|
|---|
| 986 | Indices -> {},
|
|---|
| 987 | Mass -> {MZ, 91.188},
|
|---|
| 988 | Width -> {WZ, 2.44140351},
|
|---|
| 989 | PropagatorLabel -> "Z",
|
|---|
| 990 | PropagatorType -> Sine,
|
|---|
| 991 | PropagatorArrow -> None,
|
|---|
| 992 | PDG -> 23,
|
|---|
| 993 | FullName -> "Z" },
|
|---|
| 994 |
|
|---|
| 995 | (* Gauge bosons: Q = -1 *)
|
|---|
| 996 | V[3] == {
|
|---|
| 997 | ClassName -> W,
|
|---|
| 998 | SelfConjugate -> False,
|
|---|
| 999 | Indices -> {},
|
|---|
| 1000 | Mass -> {MW, Internal},
|
|---|
| 1001 | Width -> {WW, 2.04759951},
|
|---|
| 1002 | QuantumNumbers -> {Q -> 1},
|
|---|
| 1003 | PropagatorLabel -> "W",
|
|---|
| 1004 | PropagatorType -> Sine,
|
|---|
| 1005 | PropagatorArrow -> Forward,
|
|---|
| 1006 | ParticleName ->"W+",
|
|---|
| 1007 | AntiParticleName ->"W-",
|
|---|
| 1008 | PDG -> 24,
|
|---|
| 1009 | FullName -> "W" },
|
|---|
| 1010 |
|
|---|
| 1011 | V[4] == {
|
|---|
| 1012 | ClassName -> G,
|
|---|
| 1013 | SelfConjugate -> True,
|
|---|
| 1014 | Indices -> {Index[Gluon]},
|
|---|
| 1015 | Mass -> 0,
|
|---|
| 1016 | Width -> 0,
|
|---|
| 1017 | PropagatorLabel -> G,
|
|---|
| 1018 | PropagatorType -> C,
|
|---|
| 1019 | PropagatorArrow -> None,
|
|---|
| 1020 | PDG -> 21,
|
|---|
| 1021 | FullName -> "G" },
|
|---|
| 1022 |
|
|---|
| 1023 | V[5] == {
|
|---|
| 1024 | ClassName -> Wi,
|
|---|
| 1025 | Unphysical -> True,
|
|---|
| 1026 | Definitions -> {Wi[mu_, 1] -> (W[mu] + Wbar[mu])/Sqrt[2],
|
|---|
| 1027 | Wi[mu_, 2] -> (Wbar[mu] - W[mu])/Sqrt[2]/I,
|
|---|
| 1028 | Wi[mu_, 3] -> cw Z[mu] + sw A[mu]},
|
|---|
| 1029 | SelfConjugate -> True,
|
|---|
| 1030 | Indices -> {Index[SU2W]},
|
|---|
| 1031 | FlavorIndex -> SU2W,
|
|---|
| 1032 | Mass -> 0,
|
|---|
| 1033 | PDG -> {1,2,3}},
|
|---|
| 1034 |
|
|---|
| 1035 | V[6] == {
|
|---|
| 1036 | ClassName -> B,
|
|---|
| 1037 | SelfConjugate -> True,
|
|---|
| 1038 | Definitions -> {B[mu_] -> -sw Z[mu] + cw A[mu]},
|
|---|
| 1039 | Indices -> {},
|
|---|
| 1040 | Mass -> 0,
|
|---|
| 1041 | Unphysical -> True},
|
|---|
| 1042 |
|
|---|
| 1043 |
|
|---|
| 1044 | (************ Scalar Fields **********)
|
|---|
| 1045 | (* physical Higgs: Q = 0 *)
|
|---|
| 1046 | S[1] == {
|
|---|
| 1047 | ClassName -> H,
|
|---|
| 1048 | SelfConjugate -> True,
|
|---|
| 1049 | Mass -> {MH, 120},
|
|---|
| 1050 | Width -> {WH, 0.00575308848},
|
|---|
| 1051 | PropagatorLabel -> "H",
|
|---|
| 1052 | PropagatorType -> D,
|
|---|
| 1053 | PropagatorArrow -> None,
|
|---|
| 1054 | PDG -> 25,
|
|---|
| 1055 | TeXParticleName -> "\\phi",
|
|---|
| 1056 | TeXClassName -> "\\phi",
|
|---|
| 1057 | FullName -> "H" },
|
|---|
| 1058 |
|
|---|
| 1059 | S[2] == {
|
|---|
| 1060 | ClassName -> phi,
|
|---|
| 1061 | SelfConjugate -> True,
|
|---|
| 1062 | Mass -> {MZ, 91.188},
|
|---|
| 1063 | Width -> Wphi,
|
|---|
| 1064 | PropagatorLabel -> "Phi",
|
|---|
| 1065 | PropagatorType -> D,
|
|---|
| 1066 | PropagatorArrow -> None,
|
|---|
| 1067 | ParticleName ->"phi0",
|
|---|
| 1068 | PDG -> 250,
|
|---|
| 1069 | FullName -> "Phi",
|
|---|
| 1070 | Goldstone -> Z },
|
|---|
| 1071 |
|
|---|
| 1072 | S[3] == {
|
|---|
| 1073 | ClassName -> phi2,
|
|---|
| 1074 | SelfConjugate -> False,
|
|---|
| 1075 | Mass -> {MW, Internal},
|
|---|
| 1076 | Width -> Wphi2,
|
|---|
| 1077 | PropagatorLabel -> "Phi2",
|
|---|
| 1078 | PropagatorType -> D,
|
|---|
| 1079 | PropagatorArrow -> None,
|
|---|
| 1080 | ParticleName ->"phi+",
|
|---|
| 1081 | AntiParticleName ->"phi-",
|
|---|
| 1082 | PDG -> 251,
|
|---|
| 1083 | FullName -> "Phi2",
|
|---|
| 1084 | TeXClassName -> "\\phi^+",
|
|---|
| 1085 | TeXParticleName -> "\\phi^+",
|
|---|
| 1086 | TeXAntiParticleName -> "\\phi^-",
|
|---|
| 1087 | Goldstone -> W,
|
|---|
| 1088 | QuantumNumbers -> {Q -> 1}}
|
|---|
| 1089 | }
|
|---|
| 1090 |
|
|---|
| 1091 |
|
|---|
| 1092 |
|
|---|
| 1093 |
|
|---|
| 1094 | (*****************************************************************************************)
|
|---|
| 1095 |
|
|---|
| 1096 | (* SM + type III seesaw Lagrangian *)
|
|---|
| 1097 |
|
|---|
| 1098 | (******************** Gauge F^2 Lagrangian terms*************************)
|
|---|
| 1099 | (*Sign convention from Lagrangian in between Eq. (A.9) and Eq. (A.10) of Peskin & Schroeder.*)
|
|---|
| 1100 | LGauge = -1/4 (del[Wi[nu, i1], mu] - del[Wi[mu, i1], nu] + gw Eps[i1, i2, i3] Wi[mu, i2] Wi[nu, i3])*
|
|---|
| 1101 | (del[Wi[nu, i1], mu] - del[Wi[mu, i1], nu] + gw Eps[i1, i4, i5] Wi[mu, i4] Wi[nu, i5]) -
|
|---|
| 1102 |
|
|---|
| 1103 | 1/4 (del[B[nu], mu] - del[B[mu], nu])^2 -
|
|---|
| 1104 |
|
|---|
| 1105 | 1/4 (del[G[nu, a1], mu] - del[G[mu, a1], nu] + gs f[a1, a2, a3] G[mu, a2] G[nu, a3])*
|
|---|
| 1106 | (del[G[nu, a1], mu] - del[G[mu, a1], nu] + gs f[a1, a4, a5] G[mu, a4] G[nu, a5]);
|
|---|
| 1107 |
|
|---|
| 1108 |
|
|---|
| 1109 | (********************* Fermion Lagrangian terms*************************)
|
|---|
| 1110 | (*Sign convention from Lagrangian in between Eq. (A.9) and Eq. (A.10) of Peskin & Schroeder.*)
|
|---|
| 1111 | LFermions = Module[{Lkin, LQCD, LEWleft, LEWright},
|
|---|
| 1112 |
|
|---|
| 1113 | Lkin = I uqbar.Ga[mu].del[uq, mu] +
|
|---|
| 1114 | I dqbar.Ga[mu].del[dq, mu] +
|
|---|
| 1115 | I lbar.Ga[mu].del[l, mu] +
|
|---|
| 1116 | I/2 vlbar.Ga[mu].del[vl, mu];
|
|---|
| 1117 |
|
|---|
| 1118 | LQCD = gs (uqbar.Ga[mu].T[a].uq +
|
|---|
| 1119 | dqbar.Ga[mu].T[a].dq)G[mu, a];
|
|---|
| 1120 |
|
|---|
| 1121 | LBright =
|
|---|
| 1122 | -2ee/cw B[mu]/2 lbar.Ga[mu].ProjP.gNCR.l +
|
|---|
| 1123 | -2ee*cw B[mu]/2 lbar.Ga[mu].ProjP.l +
|
|---|
| 1124 | 4ee/3/cw B[mu]/2 uqbar.Ga[mu].ProjP.uq - (*Y_uR=4/3*)
|
|---|
| 1125 | 2ee/3/cw B[mu]/2 dqbar.Ga[mu].ProjP.dq; (*Y_dR=-2/3*)
|
|---|
| 1126 |
|
|---|
| 1127 | LBleft =
|
|---|
| 1128 | -ee/cw B[mu]/2 vlbar.Ga[mu].ProjM.gNCnu.vl +
|
|---|
| 1129 | -2ee/cw B[mu]/2 lbar.Ga[mu].ProjM.gNCL.l +
|
|---|
| 1130 | -2ee*cw B[mu]/2 lbar.Ga[mu].ProjM.l +
|
|---|
| 1131 | ee/3/cw B[mu]/2 uqbar.Ga[mu].ProjM.uq + (*Y_QL=1/3*)
|
|---|
| 1132 | ee/3/cw B[mu]/2 dqbar.Ga[mu].ProjM.dq ; (*Y_QL=1/3*)
|
|---|
| 1133 |
|
|---|
| 1134 | LWleft = Module[{s,r,p,n,m,i},
|
|---|
| 1135 | ee/sw/2(
|
|---|
| 1136 |
|
|---|
| 1137 | vlbar[s,n].Ga[mu,s,p].ProjM[p,r].gNCnu[n,m].vl[r,m] Wi[mu, 3] +
|
|---|
| 1138 | + 2 lbar[s,n].Ga[mu,s,p].ProjM[p,r].gNCL[n,m].l[r,m] Wi[mu, 3] +
|
|---|
| 1139 | - 2*sw^2 lbar[s,n].Ga[mu,s,p].ProjM[p,r].l[r,n] Wi[mu, 3] +
|
|---|
| 1140 | + 2 lbar[s,n].Ga[mu,s,p].ProjP[p,r].gNCR[n,m].l[r,m] Wi[mu, 3] +
|
|---|
| 1141 | - 2*sw^2 lbar[s,n].Ga[mu,s,p].ProjP[p,r].l[r,n] Wi[mu, 3] +
|
|---|
| 1142 |
|
|---|
| 1143 | Sqrt[2] vlbar[s,n].Ga[mu,s,p].ProjM[p,r].gCCL[m,n].l[r,m] W[mu] +
|
|---|
| 1144 | Sqrt[2] lbar[s,n].Ga[mu,s,p].ProjM[p,r].gCCL[n,m].vl[r,m] Wbar[mu]+
|
|---|
| 1145 | 2 vlbar[s,n].Ga[mu,s,p].ProjP[p,r].gCCR[m,n].l[r,m] W[mu] +
|
|---|
| 1146 | 2 lbar[s,n].Ga[mu,s,p].ProjP[p,r].gCCR[n,m].vl[r,m] Wbar[mu]+
|
|---|
| 1147 |
|
|---|
| 1148 | uqbar[s,n,i].Ga[mu,s,p].ProjM[p,r].uq[r,n,i] Wi[mu, 3] - (*sigma3 = ( 1 0 )*)
|
|---|
| 1149 | dqbar[s,n,i].Ga[mu,s,p].ProjM[p,r].dq[r,n,i] Wi[mu, 3] + (* ( 0 -1 )*)
|
|---|
| 1150 |
|
|---|
| 1151 | Sqrt[2] uqbar[s,n,i].Ga[mu,s,p].ProjM[p,r].CKM[n,m].dq[r,m,i] W[mu] +
|
|---|
| 1152 | Sqrt[2] dqbar[s,n,i].Ga[mu,s,p].ProjM[p,r].Conjugate[CKM[m,n]].uq[r,m,i] Wbar[mu]
|
|---|
| 1153 | )];
|
|---|
| 1154 |
|
|---|
| 1155 | Lkin + LQCD + LBright + LBleft + LWleft];
|
|---|
| 1156 |
|
|---|
| 1157 | (******************** Higgs Lagrangian terms****************************)
|
|---|
| 1158 | Phi := If[FeynmanGauge, {-I phi2, (v + H + I phi)/Sqrt[2]}, {0, (v + H)/Sqrt[2]}];
|
|---|
| 1159 | Phibar := If[FeynmanGauge, {I phi2bar, (v + H - I phi)/Sqrt[2]} ,{0, (v + H)/Sqrt[2]}];
|
|---|
| 1160 |
|
|---|
| 1161 |
|
|---|
| 1162 |
|
|---|
| 1163 | LHiggs := Block[{PMvec, WVec, Dc, Dcbar, Vphi},
|
|---|
| 1164 |
|
|---|
| 1165 | PMvec = Table[PauliSigma[i], {i, 3}];
|
|---|
| 1166 | Wvec[mu_] := {Wi[mu, 1], Wi[mu, 2], Wi[mu, 3]};
|
|---|
| 1167 |
|
|---|
| 1168 | (*Y_phi=1*)
|
|---|
| 1169 | Dc[f_, mu_] := I del[f, mu] + ee/cw B[mu]/2 f + ee/sw/2 (Wvec[mu].PMvec).f;
|
|---|
| 1170 | Dcbar[f_, mu_] := -I del[f, mu] + ee/cw B[mu]/2 f + ee/sw/2 f.(Wvec[mu].PMvec);
|
|---|
| 1171 |
|
|---|
| 1172 | Vphi[Phi_, Phibar_] := -muH^2 Phibar.Phi + \[Lambda] (Phibar.Phi)^2;
|
|---|
| 1173 |
|
|---|
| 1174 | (Dcbar[Phibar, mu]).Dc[Phi, mu] - Vphi[Phi, Phibar]];
|
|---|
| 1175 |
|
|---|
| 1176 |
|
|---|
| 1177 | (*************** Yukawa Lagrangian***********************)
|
|---|
| 1178 | LYuk := If[FeynmanGauge,
|
|---|
| 1179 |
|
|---|
| 1180 | Module[{s,r,n,m,i}, -
|
|---|
| 1181 | yd[n] CKM[n,m] uqbar[s,n,i].ProjP[s,r].dq[r,m,i] (-I phi2) -
|
|---|
| 1182 | yd[n] dqbar[s,n,i].ProjP[s,r].dq[r,n,i] (v+H +I phi)/Sqrt[2] -
|
|---|
| 1183 |
|
|---|
| 1184 | yu[n] uqbar[s,n,i].ProjP[s,r].uq[r,n,i] (v+H -I phi)/Sqrt[2] + (*This sign from eps matrix*)
|
|---|
| 1185 | yu[n] Conjugate[CKM[m,n]] dqbar[s,n,i].ProjP[s,r].uq[r,m,i] ( I phi2bar) -
|
|---|
| 1186 |
|
|---|
| 1187 | yl[n] lbar[s,n].ProjP[s,r].l[r,n] (v)/Sqrt[2] -
|
|---|
| 1188 | gHlR[n,m] lbar[s,n].ProjP[s,r].l[r,m] (H) -
|
|---|
| 1189 | gHnuR[n,m] vlbar[s,n].ProjP[s,r].vl[r,m] (H)/Sqrt[2] -
|
|---|
| 1190 | getalR[n,m] lbar[s,n].ProjP[s,r].l[r,m] (I phi) -
|
|---|
| 1191 | getanuR[n,m] vlbar[s,n].ProjP[s,r].vl[r,m] (I phi)/Sqrt[2] -
|
|---|
| 1192 | gPhiR[n,m] lbar[s,n].ProjP[s,r].vl[r,m] (I phi2bar) - (* Different convention in phi2 definition compared to paper *)
|
|---|
| 1193 | gPhiL[n,m] lbar[s,n].ProjM[s,r].vl[r,m] (I phi2bar) (* Different convention in phi2 definition compared to paper *)
|
|---|
| 1194 | ],
|
|---|
| 1195 |
|
|---|
| 1196 | Module[{s,r,n,m,i}, -
|
|---|
| 1197 | yd[n] dqbar[s,n,i].ProjP[s,r].dq[r,n,i] (v+H)/Sqrt[2] -
|
|---|
| 1198 | yu[n] uqbar[s,n,i].ProjP[s,r].uq[r,n,i] (v+H)/Sqrt[2] -
|
|---|
| 1199 | yl[n] lbar[s,n].ProjP[s,r].l[r,n] (v)/Sqrt[2] -
|
|---|
| 1200 | gHlR[n,m] lbar[s,n].ProjP[s,r].l[r,m] (H) -
|
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| 1201 | gHnuR[n,m] vlbar[s,n].ProjP[s,r].vl[r,m] (H)/Sqrt[2]
|
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| 1202 | ]
|
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| 1203 | ];
|
|---|
| 1204 |
|
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| 1205 | LYukawa := LYuk + HC[LYuk];
|
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| 1206 |
|
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| 1207 | (****************** Majorana Masses *********************)
|
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| 1208 |
|
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| 1209 | LMasses= - mtr/2 tr0bar.tr0 - mtrm trmbar.trm
|
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| 1210 |
|
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| 1211 |
|
|---|
| 1212 | (**************Ghost terms**************************)
|
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| 1213 | (* Now we need the ghost terms which are of the form: *)
|
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| 1214 | (* - g * antighost * d_BRST G *)
|
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| 1215 | (* where d_BRST G is BRST transform of the gauge fixing function. *)
|
|---|
| 1216 |
|
|---|
| 1217 | LGhost := If[FeynmanGauge,
|
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| 1218 | Block[{dBRSTG,LGhostG,dBRSTWi,LGhostWi,dBRSTB,LGhostB},
|
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| 1219 |
|
|---|
| 1220 | (***********First the pure gauge piece.**********************)
|
|---|
| 1221 | dBRSTG[mu_,a_] := 1/gs Module[{a2, a3}, del[ghG[a], mu] + gs f[a,a2,a3] G[mu,a2] ghG[a3]];
|
|---|
| 1222 | LGhostG := - gs ghGbar[a].del[dBRSTG[mu,a],mu];
|
|---|
| 1223 |
|
|---|
| 1224 | dBRSTWi[mu_,i_] := sw/ee Module[{i2, i3}, del[ghWi[i], mu] + ee/sw Eps[i,i2,i3] Wi[mu,i2] ghWi[i3] ];
|
|---|
| 1225 | LGhostWi := - ee/sw ghWibar[a].del[dBRSTWi[mu,a],mu];
|
|---|
| 1226 |
|
|---|
| 1227 | dBRSTB[mu_] := cw/ee del[ghB, mu];
|
|---|
| 1228 | LGhostB := - ee/cw ghBbar.del[dBRSTB[mu],mu];
|
|---|
| 1229 |
|
|---|
| 1230 | (***********Next the piece from the scalar field.************)
|
|---|
| 1231 | LGhostphi := - ee/(2*sw*cw) MW ( - I phi2 ( (cw^2-sw^2)ghWpbar.ghZ + 2sw*cw ghWpbar.ghA ) +
|
|---|
| 1232 | I phi2bar ( (cw^2-sw^2)ghWmbar.ghZ + 2sw*cw ghWmbar.ghA ) ) -
|
|---|
| 1233 | ee/(2*sw) MW ( ( (v+H) + I phi) ghWpbar.ghWp + ( (v+H) - I phi) ghWmbar.ghWm ) -
|
|---|
| 1234 | I ee/(2*sw) MZ ( - phi2bar ghZbar.ghWp + phi2 ghZbar.ghWm ) -
|
|---|
| 1235 | ee/(2*sw*cw) MZ (v+H) ghZbar.ghZ ;
|
|---|
| 1236 |
|
|---|
| 1237 |
|
|---|
| 1238 | (***********Now add the pieces together.********************)
|
|---|
| 1239 | LGhostG + LGhostWi + LGhostB + LGhostphi]
|
|---|
| 1240 |
|
|---|
| 1241 | , 0];
|
|---|
| 1242 |
|
|---|
| 1243 | (*********Total Lagrangian*******)
|
|---|
| 1244 | LTypeIII := LGauge + LHiggs + LFermions + LYukawa + LGhost + LMasses
|
|---|
| 1245 |
|
|---|
| 1246 |
|
|---|