| 1 | (***************************************************************************************************************)
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| 2 | (****** This is the FeynRules mod-file for the minimal Zp models ******)
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| 3 | (****** ******)
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| 4 | (****** Author: L. Basso ******)
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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 | M$ModelName = "minimal_Zp";
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| 13 |
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| 14 |
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| 15 | M$Information = {Authors -> "L. Basso",
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| 16 | Version -> "2.0",
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| 17 | Date -> "09-06-2011",
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| 18 | Institutions -> {"University of Southampton", "RAL-PPD, Didcot, UK", "Albert-Ludwigs-UniversitÀt Freiburg"},
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| 19 | Emails -> {"lorenzo.basso@physik.uni-freiburg.de"},
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| 20 | References -> {"L.~Basso, G.M.~Pruna and S.~Moretti, \"A Renormalisation Group Equation Study of the Scalar Sector of the Minimal B-L Extension of the Standard Model,\", Phys.,Rev. D 82, 055018 (2010) [arXiv:1004.3039 [hep-ph]]", "L.~Basso, G.M.~Pruna and S.~Moretti, \"A Theoretical constraints on the couplings of non-exotic minimal Z' bosons,\", JHEP 1108 122 (2011) [arXiv:1106.4762 [hep-ph]]"},
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| 21 | URLs -> "http://feynrules.phys.ucl.ac.be/..."};
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| 22 |
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| 23 | FeynmanGauge = True;
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| 24 |
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| 25 |
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| 26 | (******* Index definitions ********)
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| 27 |
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| 28 | IndexRange[ Index[Generation] ] = Range[3]
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| 29 |
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| 30 | IndexRange[ Index[Colour] ] = NoUnfold[Range[3]]
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| 31 |
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| 32 | IndexRange[ Index[Gluon] ] = NoUnfold[Range[8]]
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| 33 |
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| 34 | IndexRange[ Index[SU2W] ] = Unfold[Range[3]]
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| 35 |
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| 36 |
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| 37 | IndexStyle[Colour, i]
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| 38 |
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| 39 | IndexStyle[Generation, f]
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| 40 |
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| 41 | IndexStyle[Gluon ,a]
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| 42 |
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| 43 | IndexStyle[SU2W ,k]
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| 44 |
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| 45 |
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| 46 |
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| 47 | (******* Gauge parameters (for FeynArts) ********)
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| 48 |
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| 49 | GaugeXi[ V[1] ] = GaugeXi[A];
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| 50 | GaugeXi[ V[2] ] = GaugeXi[Z];
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| 51 | GaugeXi[ V[3] ] = GaugeXi[W];
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| 52 | GaugeXi[ V[4] ] = GaugeXi[G];
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| 53 | GaugeXi[ V[7] ] = GaugeXi[Zp];
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| 54 | GaugeXi[ S[1] ] = 1;
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| 55 | GaugeXi[ S[2] ] = GaugeXi[Z];
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| 56 | GaugeXi[ S[3] ] = GaugeXi[W];
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| 57 | GaugeXi[ S[4] ] = 1;
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| 58 | GaugeXi[ S[5] ] = GaugeXi[Zp];
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| 59 | GaugeXi[ U[1] ] = GaugeXi[A];
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| 60 | GaugeXi[ U[2] ] = GaugeXi[Z];
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| 61 | GaugeXi[ U[31] ] = GaugeXi[W];
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| 62 | GaugeXi[ U[32] ] = GaugeXi[W];
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| 63 | GaugeXi[ U[4] ] = GaugeXi[G];
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| 64 | GaugeXi[ U[7] ] = GaugeXi[Zp];
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| 65 |
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| 66 |
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| 67 | (***** Setting for interaction order (as e.g. used by MadGraph 5) ******)
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| 68 |
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| 69 | M$InteractionOrderHierarchy = {
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| 70 | {QCD, 1},
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| 71 | {QED, 2}
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| 72 | };
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| 73 |
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| 74 |
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| 75 | (**************** Parameters *************)
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| 76 |
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| 77 | M$Parameters = {
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| 78 |
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| 79 | (* External parameters *)
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| 80 |
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| 81 |
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| 82 | \[Alpha]EWM1== {
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| 83 | ParameterType -> External,
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| 84 | BlockName -> BLINPUTS,
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| 85 | ParameterName -> aEWM1,
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| 86 | InteractionOrder -> {QED, -2},
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| 87 | Value -> 127.9,
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| 88 | Description -> "Inverse of the electroweak coupling constant at Z-pole"},
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| 89 |
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| 90 | Gf == {
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| 91 | ParameterType -> External,
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| 92 | BlockName -> BLINPUTS,
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| 93 | InteractionOrder -> {QED, 2},
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| 94 | Value -> 1.16637 * 10^(-5),
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| 95 | Description -> "Fermi constant"},
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| 96 |
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| 97 | \[Alpha]S == {
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| 98 | ParameterType -> External,
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| 99 | BlockName -> BLINPUTS,
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| 100 | TeX -> Subscript[\[Alpha], s],
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| 101 | ParameterName -> aS,
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| 102 | InteractionOrder -> {QCD, 2},
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| 103 | Value -> 0.1184,
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| 104 | Description -> "Strong coupling constant at the Z pole."},
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| 105 |
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| 106 | MW == {
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| 107 | ParameterType -> External,
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| 108 | BlockName -> BLINPUTS,
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| 109 | Value -> 80.292,
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| 110 | Description -> "W mass"},
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| 111 |
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| 112 | MZp == {
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| 113 | ParameterType -> External,
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| 114 | BlockName -> BLINPUTS,
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| 115 | Value -> 1500.00,
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| 116 | Description -> "Zp mass"},
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| 117 |
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| 118 | g1p == {
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| 119 | ParameterType -> External,
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| 120 | BlockName -> BLINPUTS,
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| 121 | InteractionOrder -> {QED, 1},
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| 122 | Value -> 0.2,
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| 123 | Description -> "Zp coupling"},
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| 124 |
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| 125 | gt == {
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| 126 | ParameterType -> External,
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| 127 | BlockName -> BLINPUTS,
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| 128 | InteractionOrder -> {QED, 1},
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| 129 | Value -> -0.1,
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| 130 | Description -> "Z-Zp mixing coupling"},
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| 131 |
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| 132 | ymdo == {
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| 133 | ParameterType -> External,
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| 134 | BlockName -> YUKAWA,
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| 135 | Value -> 5.04*10^(-3),
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| 136 | OrderBlock -> {1},
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| 137 | Description -> "Down Yukawa mass"},
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| 138 |
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| 139 |
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| 140 | ymup == {
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| 141 | ParameterType -> External,
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| 142 | BlockName -> YUKAWA,
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| 143 | Value -> 2.55*10^(-3),
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| 144 | OrderBlock -> {2},
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| 145 | Description -> "Up Yukawa mass"},
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| 146 |
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| 147 | yms == {
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| 148 | ParameterType -> External,
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| 149 | BlockName -> YUKAWA,
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| 150 | Value -> 0.101,
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| 151 | OrderBlock -> {3},
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| 152 | Description -> "Strange Yukawa mass"},
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| 153 |
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| 154 | ymc == {
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| 155 | ParameterType -> External,
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| 156 | BlockName -> YUKAWA,
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| 157 | Value -> 1.27,
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| 158 | OrderBlock -> {4},
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| 159 | Description -> "Charm Yukawa mass"},
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| 160 |
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| 161 | ymb == {
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| 162 | ParameterType -> External,
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| 163 | BlockName -> YUKAWA,
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| 164 | Value -> 4.7,
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| 165 | OrderBlock -> {5},
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| 166 | Description -> "Bottom Yukawa mass"},
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| 167 |
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| 168 | ymt == {
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| 169 | ParameterType -> External,
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| 170 | BlockName -> YUKAWA,
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| 171 | Value -> 172.0,
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| 172 | OrderBlock -> {6},
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| 173 | Description -> "Top Yukawa mass"},
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| 174 |
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| 175 | yme == {
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| 176 | ParameterType -> External,
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| 177 | BlockName -> YUKAWA,
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| 178 | Value -> 0.000511,
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| 179 | OrderBlock -> {11},
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| 180 | Description -> "Electron Yukawa mass"},
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| 181 |
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| 182 | ymmu == {
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| 183 | ParameterType -> External,
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| 184 | BlockName -> YUKAWA,
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| 185 | Value -> 0.1057,
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| 186 | OrderBlock -> {13},
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| 187 | Description -> "Muon Yukawa mass"},
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| 188 |
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| 189 | ymtau == {
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| 190 | ParameterType -> External,
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| 191 | BlockName -> YUKAWA,
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| 192 | Value -> 1.777,
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| 193 | OrderBlock -> {15},
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| 194 | Description -> "Tau Yukawa mass"},
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| 195 |
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| 196 | MH1 == {
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| 197 | ParameterType -> External,
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| 198 | BlockName -> BLINPUTS,
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| 199 | Value -> 120.00,
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| 200 | Description -> "H1 mass"},
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| 201 |
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| 202 | MH2 == {
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| 203 | ParameterType -> External,
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| 204 | BlockName -> BLINPUTS,
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| 205 | Value -> 450.00,
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| 206 | Description -> "H2 mass"},
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| 207 |
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| 208 |
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| 209 | Sa == {
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| 210 | ParameterType -> External,
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| 211 | BlockName -> BLINPUTS,
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| 212 | Value -> 0.1,
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| 213 | Description -> "Sine of Higgses mixing angle"},
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| 214 |
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| 215 | sw2 == {
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| 216 | ParameterType -> External,
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| 217 | BlockName -> BLINPUTS,
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| 218 | Value -> 0.232,
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| 219 | Description -> "Squared Sin of the Weinberg angle"},
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| 220 |
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| 221 |
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| 222 |
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| 223 | (* Internal Parameters *)
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| 224 |
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| 225 | \[Alpha]EW == {
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| 226 | ParameterType -> Internal,
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| 227 | Value -> 1/\[Alpha]EWM1,
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| 228 | TeX -> Subscript[\[Alpha], EW],
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| 229 | ParameterName -> aEW,
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| 230 | InteractionOrder -> {QED, 2},
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| 231 | Description -> "Electroweak coupling contant"},
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| 232 |
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| 233 |
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| 234 | ee == {
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| 235 | TeX -> e,
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| 236 | ParameterType -> Internal,
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| 237 | Value -> Sqrt[4 Pi \[Alpha]EW],
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| 238 | InteractionOrder -> {QED, 1},
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| 239 | Description -> "Electric coupling constant"},
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| 240 |
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| 241 | cw == {
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| 242 | TeX -> Subscript[c, w],
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| 243 | ParameterType -> Internal,
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| 244 | Value -> Sqrt[1 - sw2],
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| 245 | Description -> "Cos of the Weinberg angle"},
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| 246 |
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| 247 | sw == {
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| 248 | TeX -> Subscript[s, w],
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| 249 | ParameterType -> Internal,
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| 250 | Value -> Sqrt[sw2],
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| 251 | Description -> "Sin of the Weinberg angle"},
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| 252 |
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| 253 | gw == {
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| 254 | TeX -> Subscript[g, w],
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| 255 | ParameterType -> Internal,
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| 256 | Value -> ee / sw,
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| 257 | Definitions -> {gw -> ee / sw},
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| 258 | InteractionOrder -> {QED, 1},
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| 259 | Description -> "Weak coupling constant"},
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| 260 |
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| 261 | g1 == {
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| 262 | TeX -> Subscript[g, 1],
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| 263 | ParameterType -> Internal,
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| 264 | Value -> ee / cw,
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| 265 | Definitions -> {g1 -> ee / cw},
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| 266 | InteractionOrder -> {QED, 1},
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| 267 | Description -> "U(1)Y coupling constant"},
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| 268 |
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| 269 | gs == {
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| 270 | TeX -> Subscript[g, s],
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| 271 | ParameterType -> Internal,
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| 272 | Value -> Sqrt[4 Pi \[Alpha]S],
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| 273 | InteractionOrder -> {QCD, 1},
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| 274 | ParameterName -> G,
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| 275 | Description -> "Strong coupling constant"},
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| 276 |
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| 277 | v == {
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| 278 | ParameterType -> Internal,
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| 279 | BlockName -> VEV,
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| 280 | Value -> 2*MW*sw/ee,
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| 281 | InteractionOrder -> {QED, -1},
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| 282 | Description -> "H1 VEV"},
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| 283 |
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| 284 |
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| 285 | x == {
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| 286 | ParameterType -> Internal,
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| 287 | BlockName -> VEV,
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| 288 | Value -> MZp/(2*g1p)*Sqrt[1-gt^2*v^2/(4*MZp^2-v^2*(gw^2+g1^2))],
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| 289 | InteractionOrder -> {QED, -1},
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| 290 | Description -> "H2 VEV"},
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| 291 |
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| 292 |
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| 293 | Ca == {
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| 294 | ParameterType -> Internal,
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| 295 | Value -> Sqrt[1-Sa^2],
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| 296 | ParameterName -> Ca,
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| 297 | Description -> "Cosine of Higgses mixing angle"},
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| 298 |
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| 299 |
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| 300 | yl == {
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| 301 | TeX -> Superscript[y, l],
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| 302 | Indices -> {Index[Generation]},
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| 303 | AllowSummation -> True,
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| 304 | ParameterType -> Internal,
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| 305 | Value -> {yl[1] -> Sqrt[2] yme / v, yl[2] -> Sqrt[2] ymmu / v, yl[3] -> Sqrt[2] ymtau / v},
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| 306 | ParameterName -> {yl[1] -> ye, yl[2] -> ym, yl[3] -> ytau},
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| 307 | InteractionOrder -> {QED, 1},
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| 308 | ComplexParameter -> False,
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| 309 | Description -> "Lepton Yukawa coupling"},
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| 310 |
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| 311 | yu == {
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| 312 | Indices -> {Index[Generation]},
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| 313 | AllowSummation -> True,
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| 314 | AllowSummation -> True,
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| 315 | ParameterType -> Internal,
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| 316 | Value -> {yu[1] -> Sqrt[2] ymup / v, yu[2] -> Sqrt[2] ymc / v, yu[3] -> Sqrt[2] ymt / v},
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| 317 | ParameterName -> {yu[1] -> yup, yu[2] -> yc, yu[3] -> yt},
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| 318 | InteractionOrder -> {QED, 1},
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| 319 | ComplexParameter -> False,
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| 320 | Description -> "U-quark Yukawa coupling"},
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| 321 |
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| 322 | yd == {
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| 323 | TeX -> Superscript[y, d],
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| 324 | Indices -> {Index[Generation]},
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| 325 | AllowSummation -> True,
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| 326 | ParameterType -> Internal,
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| 327 | Value -> {yd[1] -> Sqrt[2] ymdo / v, yd[2] -> Sqrt[2] yms / v, yd[3] -> Sqrt[2] ymb / v},
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| 328 | ParameterName -> {yd[1] -> ydo, yd[2] -> ys, yd[3] -> yb},
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| 329 | InteractionOrder -> {QED, 1},
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| 330 | ComplexParameter -> False,
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| 331 | Description -> "D-quark Yukawa coupling"},
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| 332 |
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| 333 | ynd == {
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| 334 | Indices -> {Index[Generation]},
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| 335 | AllowSummation -> True,
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| 336 | ParameterType -> Internal,
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| 337 | Value -> {ynd[1] -> Sqrt[2*MnL1*MnH1]/v,
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| 338 | ynd[2] -> Sqrt[2*MnL2*MnH2]/v,
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| 339 | ynd[3] -> Sqrt[2*MnL3*MnH3]/v},
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| 340 | ParameterName -> {ynd[1] -> ynd1,
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| 341 | ynd[2] -> ynd2,
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| 342 | ynd[3] -> ynd3},
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| 343 | InteractionOrder -> {QED, 1},
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| 344 | ComplexParameter -> False,
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| 345 | Description -> "Dirac neutrino Yukawa coupling"},
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| 346 |
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| 347 | ynm == {
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| 348 | Indices -> {Index[Generation]},
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| 349 | AllowSummation -> True,
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| 350 | ParameterType -> Internal,
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| 351 | Value -> {ynm[1] -> (MnH1-MnL1)/Sqrt[2]/x,
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| 352 | ynm[2] -> (MnH2-MnL2)/Sqrt[2]/x,
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| 353 | ynm[3] -> (MnH3-MnL3)/Sqrt[2]/x},
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| 354 | ParameterName -> {ynm[1] -> ynm1, ynm[2] -> ynm2, ynm[3] -> ynm3},
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| 355 | InteractionOrder -> {QED, 1},
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| 356 | ComplexParameter -> False,
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| 357 | Description -> "Majorana neutrino Yukawa coupling"},
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| 358 |
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| 359 | Mdd == {
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| 360 | Indices -> {Index[Generation]},
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| 361 | AllowSummation -> True,
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| 362 | ParameterType -> Internal,
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| 363 | Value -> {Mdd[1] -> ynd1*v/Sqrt[2],
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| 364 | Mdd[2] -> ynd2*v/Sqrt[2],
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| 365 | Mdd[3] -> ynd3*v/Sqrt[2]},
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| 366 | ParameterName -> {Mdd[1] -> Mdd1, Mdd[2] -> Mdd2, Mdd[3] -> Mdd3},
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| 367 | ComplexParameter -> False,
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| 368 | Description -> "Neutrino Dirac Mass"},
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| 369 |
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| 370 | s12 == {
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| 371 | TeX -> Subscript[S\[Theta], 12],
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| 372 | ParameterType -> External,
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| 373 | BlockName -> CKMBLOCK,
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| 374 | Value -> 0.221,
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| 375 | Description -> "Sin(theta_12), PDG-94"},
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| 376 |
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| 377 | s23 == {
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| 378 | TeX -> Subscript[S\[Theta], 23],
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| 379 | ParameterType -> External,
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| 380 | BlockName -> CKMBLOCK,
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| 381 | Value -> 0.040,
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| 382 | Description -> "Sin(theta_23), PDG-94"},
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| 383 |
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| 384 | s13 == {
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| 385 | TeX -> Subscript[S\[Theta], 13],
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| 386 | ParameterType -> External,
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| 387 | BlockName -> CKMBLOCK,
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| 388 | Value -> 0.0035,
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| 389 | Description -> "Sin(theta_13), PDG-94"},
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| 390 |
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| 391 | c12 == {
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| 392 | TeX -> Subscript[C\[Theta], 12],
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| 393 | ParameterType -> Internal,
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| 394 | BlockName -> CKMBLOCK,
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| 395 | Value -> Sqrt[1-s12^2],
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| 396 | Description -> "Cos(theta_12)"},
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| 397 |
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| 398 | c23 == {
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| 399 | TeX -> Subscript[C\[Theta], 23],
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| 400 | ParameterType -> Internal,
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| 401 | BlockName -> CKMBLOCK,
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| 402 | Value -> Sqrt[1-s23^2],
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| 403 | Description -> "Cos(theta_23)"},
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| 404 |
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| 405 | c13 == {
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| 406 | TeX -> Subscript[C\[Theta], 13],
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| 407 | ParameterType -> Internal,
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| 408 | BlockName -> CKMBLOCK,
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| 409 | Value -> Sqrt[1-s13^2],
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| 410 | Description -> "Cos(theta_13)"},
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| 411 |
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| 412 | CKM == {
|
|---|
| 413 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 414 | TensorClass -> CKM,
|
|---|
| 415 | Unitary -> True,
|
|---|
| 416 | Value -> {CKM[1,1] -> c12*c13,
|
|---|
| 417 | CKM[1,2] -> s12*c13,
|
|---|
| 418 | CKM[1,3] -> s13,
|
|---|
| 419 | CKM[2,1] -> -s12*c23-c12*s23*s13,
|
|---|
| 420 | CKM[2,2] -> c12*c23-s12*s23*s13,
|
|---|
| 421 | CKM[2,3] -> s23*c13,
|
|---|
| 422 | CKM[3,1] -> s12*s23-c12*c23*s13,
|
|---|
| 423 | CKM[3,2] -> -c12*s23-s12*c23*s13,
|
|---|
| 424 | CKM[3,3] -> c23*c13},
|
|---|
| 425 | Description -> "CKM-Matrix"},
|
|---|
| 426 |
|
|---|
| 427 | San == {
|
|---|
| 428 | Indices -> {Index[Generation]},
|
|---|
| 429 | AllowSummation -> True,
|
|---|
| 430 | ParameterType -> Internal,
|
|---|
| 431 | Value -> {San[1] -> Sin[ArcSin[-2*Mdd1/Sqrt[4*Mdd1^2+(MnH1-MnL1)^2]]/2],
|
|---|
| 432 | San[2] -> Sin[ArcSin[-2*Mdd2/Sqrt[4*Mdd2^2+(MnH2-MnL2)^2]]/2],
|
|---|
| 433 | San[3] -> Sin[ArcSin[-2*Mdd3/Sqrt[4*Mdd3^2+(MnH3-MnL3)^2]]/2]},
|
|---|
| 434 | ParameterName -> {San[1] -> San1, San[2] -> San2, San[3] -> San3},
|
|---|
| 435 | ComplexParameter -> False,
|
|---|
| 436 | Description -> "Sin-array of neutrino mass-eigenstates"},
|
|---|
| 437 |
|
|---|
| 438 | Can == {
|
|---|
| 439 | Indices -> {Index[Generation]},
|
|---|
| 440 | AllowSummation -> True,
|
|---|
| 441 | ParameterType -> Internal,
|
|---|
| 442 | Value -> {Can[1] -> Sqrt[1-San1^2],
|
|---|
| 443 | Can[2] -> Sqrt[1-San2^2],
|
|---|
| 444 | Can[3] -> Sqrt[1-San3^2]},
|
|---|
| 445 | Definitions -> {Can[1]*San1-> Sa2n1/2,
|
|---|
| 446 | Can[2]*San2-> Sa2n2/2,
|
|---|
| 447 | Can[3]*San3-> Sa2n3/2,
|
|---|
| 448 | Can[1]^2 -San1^2-> Ca2n1,
|
|---|
| 449 | Can[2]^2 -San2^2-> Ca2n2,
|
|---|
| 450 | Can[3]^2 -San3^2-> Ca2n3},
|
|---|
| 451 | ParameterName -> {Can[1] -> Can1, Can[2] -> Can2, Can[3] -> Can3},
|
|---|
| 452 | ComplexParameter -> False,
|
|---|
| 453 | Description -> "Cos-array of neutrino mass-eigenstates"},
|
|---|
| 454 |
|
|---|
| 455 |
|
|---|
| 456 |
|
|---|
| 457 | \[Lambda]1 == {
|
|---|
| 458 | ParameterType -> Internal,
|
|---|
| 459 | Value -> MH1^2 /(2*v^2)*Ca^2 + MH2^2 /(2*v^2)*Sa^2,
|
|---|
| 460 | ParameterName -> lam1,
|
|---|
| 461 | InteractionOrder -> {QED, 2},
|
|---|
| 462 | Description -> "Lambda 1"},
|
|---|
| 463 |
|
|---|
| 464 | \[Lambda]2 == {
|
|---|
| 465 | ParameterType -> Internal,
|
|---|
| 466 | Value -> MH1^2 /(2*x^2)*Sa^2 + MH2^2 /(2*x^2)*Ca^2,
|
|---|
| 467 | ParameterName -> lam2,
|
|---|
| 468 | InteractionOrder -> {QED, 2},
|
|---|
| 469 | Description -> "Lambda 2"},
|
|---|
| 470 |
|
|---|
| 471 | \[Lambda]3 == {
|
|---|
| 472 | ParameterType -> Internal,
|
|---|
| 473 | Value -> (MH2^2 - MH1^2)/(x*v)*Sa*Ca,
|
|---|
| 474 | ParameterName -> lam3,
|
|---|
| 475 | InteractionOrder -> {QED, 2},
|
|---|
| 476 | Description -> "Lambda 3, mixing parameter"},
|
|---|
| 477 |
|
|---|
| 478 | mu2H1 == {
|
|---|
| 479 | ParameterType -> Internal,
|
|---|
| 480 | Value -> - \[Lambda]1 * v^2 - \[Lambda]3 /2 * x^2,
|
|---|
| 481 | TeX -> m^2,
|
|---|
| 482 | Description -> "Coefficient of the quadratic piece of the H1 potential"},
|
|---|
| 483 |
|
|---|
| 484 | mu2H2 == {
|
|---|
| 485 | ParameterType -> Internal,
|
|---|
| 486 | Value -> - \[Lambda]3 /2 * v^2 - \[Lambda]2 * x^2,
|
|---|
| 487 | TeX -> \[Mu]^2,
|
|---|
| 488 | Description -> "Coefficient of the quadratic piece of the H2 potential"},
|
|---|
| 489 |
|
|---|
| 490 |
|
|---|
| 491 | Sp2num == {
|
|---|
| 492 | ParameterType -> Internal,
|
|---|
| 493 | Value -> 2*gt*Sqrt[(ee/sw)^2+(ee/cw)^2]},
|
|---|
| 494 |
|
|---|
| 495 | Cp2num == {
|
|---|
| 496 | ParameterType -> Internal,
|
|---|
| 497 | Value -> gt^2+16*(x/v)^2*g1p^2-(ee/sw)^2-(ee/cw)^2},
|
|---|
| 498 |
|
|---|
| 499 | Sp == {
|
|---|
| 500 | AllowSummation -> True,
|
|---|
| 501 | ParameterType -> Internal,
|
|---|
| 502 | Value -> Sin[ArcSin[Sp2num/Sqrt[Sp2num^2+Cp2num^2]]/2],
|
|---|
| 503 | ComplexParameter -> False,
|
|---|
| 504 | Description -> "Sin-array of neutrino mass-eigenstates"},
|
|---|
| 505 |
|
|---|
| 506 | Cp == {
|
|---|
| 507 | AllowSummation -> True,
|
|---|
| 508 | ParameterType -> Internal,
|
|---|
| 509 | Value -> Sqrt[1-Sp^2],
|
|---|
| 510 | ComplexParameter -> False,
|
|---|
| 511 | Description -> "Cos-array of neutrino mass-eigenstates"},
|
|---|
| 512 |
|
|---|
| 513 |
|
|---|
| 514 | Cn == {
|
|---|
| 515 | ParameterType -> Internal,
|
|---|
| 516 | ComplexParameter -> False,
|
|---|
| 517 | Value -> (ee/sw)^2+(ee/cw)^2+gt^2+16*(x/v)^2*g1p^2},
|
|---|
| 518 |
|
|---|
| 519 | Dn == {
|
|---|
| 520 | ParameterType -> Internal,
|
|---|
| 521 | ComplexParameter -> False,
|
|---|
| 522 | Value -> 64*((ee/sw)^2+(ee/cw)^2)*g1p^2*v^2*x^2},
|
|---|
| 523 |
|
|---|
| 524 |
|
|---|
| 525 | MZ == {
|
|---|
| 526 | ParameterType -> Internal,
|
|---|
| 527 | Value -> Sqrt[(Cn*v^2-Sqrt[-Dn+v^4*Cn^2])/8],
|
|---|
| 528 | Description -> "Z mass"},
|
|---|
| 529 |
|
|---|
| 530 | S2gNum == {
|
|---|
| 531 | ParameterType -> Internal,
|
|---|
| 532 | ComplexParameter -> False,
|
|---|
| 533 | Value -> 8*x/v*gt*g1p},
|
|---|
| 534 |
|
|---|
| 535 | C2gNum == {
|
|---|
| 536 | ParameterType -> Internal,
|
|---|
| 537 | ComplexParameter -> False,
|
|---|
| 538 | Value -> (ee/sw)^2+(ee/cw)^2+gt^2-16*(x/v)^2*g1p^2},
|
|---|
| 539 |
|
|---|
| 540 |
|
|---|
| 541 | sg == {
|
|---|
| 542 | ParameterType -> Internal,
|
|---|
| 543 | ComplexParameter -> False,
|
|---|
| 544 | Value -> Sin[ArcSin[-S2gNum/Sqrt[S2gNum^2+C2gNum^2]]/2],
|
|---|
| 545 | Description -> "cosine of Z-Zp goldostone mixing angle"},
|
|---|
| 546 |
|
|---|
| 547 | cg == {
|
|---|
| 548 | ParameterType -> Internal,
|
|---|
| 549 | ComplexParameter -> False,
|
|---|
| 550 | Value -> Sqrt[1-sg^2],
|
|---|
| 551 | Description -> "sine of Z-Zp goldstone mixing angle"}
|
|---|
| 552 | (* Value -> Cos[ArcCos[-C2gNum/Sqrt[S2gNum^2+C2gNum^2]]/2], *)
|
|---|
| 553 | }
|
|---|
| 554 |
|
|---|
| 555 | (************** Gauge Groups ******************)
|
|---|
| 556 |
|
|---|
| 557 | M$GaugeGroups = {
|
|---|
| 558 |
|
|---|
| 559 | U1BL == {
|
|---|
| 560 | Abelian -> True,
|
|---|
| 561 | GaugeBoson -> Bp,
|
|---|
| 562 | Charge -> BL,
|
|---|
| 563 | CouplingConstant -> g1p},
|
|---|
| 564 |
|
|---|
| 565 | U1Y == {
|
|---|
| 566 | Abelian -> True,
|
|---|
| 567 | GaugeBoson -> B,
|
|---|
| 568 | Charge -> Y,
|
|---|
| 569 | CouplingConstant -> g1},
|
|---|
| 570 |
|
|---|
| 571 | SU2L == {
|
|---|
| 572 | Abelian -> False,
|
|---|
| 573 | GaugeBoson -> Wi,
|
|---|
| 574 | StructureConstant -> Eps,
|
|---|
| 575 | CouplingConstant -> gw},
|
|---|
| 576 |
|
|---|
| 577 | SU3C == {
|
|---|
| 578 | Abelian -> False,
|
|---|
| 579 | GaugeBoson -> G,
|
|---|
| 580 | StructureConstant -> f,
|
|---|
| 581 | SymmetricTensor -> dSUN,
|
|---|
| 582 | Representations -> {T, Colour},
|
|---|
| 583 | CouplingConstant -> gs}
|
|---|
| 584 | }
|
|---|
| 585 |
|
|---|
| 586 | (********* Particle Classes **********)
|
|---|
| 587 |
|
|---|
| 588 | M$ClassesDescription = {
|
|---|
| 589 |
|
|---|
| 590 | (********** Fermions ************)
|
|---|
| 591 |
|
|---|
| 592 | (* Mass-Eigenstate light neutrino: Q = 0, BL= -1 *)
|
|---|
| 593 |
|
|---|
| 594 | F[11] == {
|
|---|
| 595 | ClassName -> nL,
|
|---|
| 596 | ClassMembers -> {nL1, nL2, nL3},
|
|---|
| 597 | FlavorIndex -> Generation,
|
|---|
| 598 | SelfConjugate -> True,
|
|---|
| 599 | Indices -> {Index[Generation]},
|
|---|
| 600 | Mass -> {MnL, {MnL1, 10^(-9)}, {MnL2, 10^(-9)}, {MnL3, 10^(-9)}},
|
|---|
| 601 | Width -> 0,
|
|---|
| 602 | PropagatorLabel -> {"nL", "nul1", "nul2", "nul3"},
|
|---|
| 603 | PropagatorType -> Straight,
|
|---|
| 604 | ParticleName -> {"n1", "n2", "n3"},
|
|---|
| 605 | PropagatorArrow -> Forward,
|
|---|
| 606 | PDG -> {12, 14, 16},
|
|---|
| 607 | FullName -> {"Light neutrino 1", "Light neutrino 2", "Light neutrino 3"} },
|
|---|
| 608 |
|
|---|
| 609 | (* Mass-Eigenstate heavy neutrino: Q = 0, BL= -1 *)
|
|---|
| 610 |
|
|---|
| 611 | F[12] == {
|
|---|
| 612 | ClassName -> nH,
|
|---|
| 613 | ClassMembers -> {nH1, nH2, nH3},
|
|---|
| 614 | FlavorIndex -> Generation,
|
|---|
| 615 | SelfConjugate -> True,
|
|---|
| 616 | Indices -> {Index[Generation]},
|
|---|
| 617 | Mass -> {MnH, {MnH1, 200.00}, {MnH2, 200.00}, {MnH3, 200.00}},
|
|---|
| 618 | Width -> 10^(-13),
|
|---|
| 619 | PropagatorLabel -> {"nH", "nuh1", "nuh2", "nuh3"},
|
|---|
| 620 | PropagatorType -> Straight,
|
|---|
| 621 | ParticleName -> {"~n1", "~n2", "~n3"},
|
|---|
| 622 | PropagatorArrow -> Forward,
|
|---|
| 623 | PDG -> {9100012, 9100014, 9100016},
|
|---|
| 624 | FullName -> {"Heavy neutrino 1", "Heavy neutrino 2", "Heavy neutrino 3"} },
|
|---|
| 625 |
|
|---|
| 626 | (* Left-handed neutrino: unphysical *)
|
|---|
| 627 | F[13] == {
|
|---|
| 628 | ClassName -> nF,
|
|---|
| 629 | ClassMembers -> {nF1,nF2,nF3},
|
|---|
| 630 | FlavorIndex -> Generation,
|
|---|
| 631 | SelfConjugate -> True,
|
|---|
| 632 | Indices -> {Index[Generation]},
|
|---|
| 633 | Unphysical -> True,
|
|---|
| 634 | Definitions -> {nF[s_,i_] -> Can[i] nL[s,i]-San[i] nH[s,i]},
|
|---|
| 635 | FullName -> {"Majorana LH component of Dirac neutrino 1",
|
|---|
| 636 | "Majorana LH component of Dirac neutrino 2", "Majorana LH component of Dirac neutrino 3"} },
|
|---|
| 637 |
|
|---|
| 638 | (* Right-handed neutrino: unphysical *)
|
|---|
| 639 | F[14] == {
|
|---|
| 640 | ClassName -> nR,
|
|---|
| 641 | ClassMembers -> {nR1,nR2,nR3},
|
|---|
| 642 | FlavorIndex -> Generation,
|
|---|
| 643 | SelfConjugate -> True,
|
|---|
| 644 | Indices -> {Index[Generation]},
|
|---|
| 645 | Unphysical -> True,
|
|---|
| 646 | Definitions -> {nR[s_,i_] -> San[i] nL[s,i]+Can[i] nH[s,i]},
|
|---|
| 647 | FullName -> {"Majorana LH component of Dirac neutrino 1", "Majorana LH component of Dirac neutrino 2", "Majorana LH component of Dirac neutrino 3"} },
|
|---|
| 648 |
|
|---|
| 649 |
|
|---|
| 650 | (* Flavour-eigenstate neutrino: unphysical *)
|
|---|
| 651 | F[15] == {
|
|---|
| 652 | ClassName -> vl,
|
|---|
| 653 | ClassMembers -> {vle,vlm,vlt},
|
|---|
| 654 | FlavorIndex -> Generation,
|
|---|
| 655 | SelfConjugate -> False,
|
|---|
| 656 | Indices -> {Index[Generation]},
|
|---|
| 657 | QuantumNumbers -> {Q -> 0, LeptonNumber -> 1, BarionLepton -> -1},
|
|---|
| 658 | Unphysical -> True,
|
|---|
| 659 | Definitions -> {vl[s_,i_] -> left[nF[s,i]]+right[nR[s,i]]},
|
|---|
| 660 | ParticleName -> {"nue", "num", "nut"},
|
|---|
| 661 | AntiParticleName -> {"nue-bar", "num-bar", "nut-bar"},
|
|---|
| 662 | FullName -> {"Electron-neutrino", "Mu-neutrino", "Tau-neutrino"} },
|
|---|
| 663 |
|
|---|
| 664 |
|
|---|
| 665 | (* Leptons (electron): I_3 = -1/2, Q = -1, BL= -1 *)
|
|---|
| 666 | F[2] == {
|
|---|
| 667 | ClassName -> l,
|
|---|
| 668 | ClassMembers -> {e, m, tt},
|
|---|
| 669 | FlavorIndex -> Generation,
|
|---|
| 670 | SelfConjugate -> False,
|
|---|
| 671 | Indices -> {Index[Generation]},
|
|---|
| 672 | Mass -> {Ml, {ME, 0.000511}, {MM, 0.1057}, {MTA, 1.777}},
|
|---|
| 673 | Width -> 0,
|
|---|
| 674 | QuantumNumbers -> {Q -> -1, LeptonNumber -> 1, BarionLepton -> -1},
|
|---|
| 675 | PropagatorLabel -> {"l", "e", "m", "tt"},
|
|---|
| 676 | PropagatorType -> Straight,
|
|---|
| 677 | ParticleName -> {"e", "m", "l"},
|
|---|
| 678 | AntiParticleName -> {"E", "M", "L"},
|
|---|
| 679 | PropagatorArrow -> Forward,
|
|---|
| 680 | PDG -> {11, 13, 15},
|
|---|
| 681 | FullName -> {"Electron", "Muon", "Tau"} },
|
|---|
| 682 |
|
|---|
| 683 | (* Quarks (u): I_3 = +1/2, Q = +2/3, BL=1/3 *)
|
|---|
| 684 | F[3] == {
|
|---|
| 685 | ClassMembers -> {u, c, t},
|
|---|
| 686 | ClassName -> uq,
|
|---|
| 687 | FlavorIndex -> Generation,
|
|---|
| 688 | SelfConjugate -> False,
|
|---|
| 689 | Indices -> {Index[Generation], Index[Colour]},
|
|---|
| 690 | Mass -> {Mu, {MU, 2.55*10^(-3)}, {MC, 1.27}, {MT, 172.0}},
|
|---|
| 691 | Width -> {0, 0, {WT, 1.50833649}},
|
|---|
| 692 | QuantumNumbers -> {Q -> 2/3, BarionLepton -> 1/3},
|
|---|
| 693 | PropagatorLabel -> {"uq", "u", "c", "t"},
|
|---|
| 694 | ParticleName -> {"u", "c", "t"},
|
|---|
| 695 | AntiParticleName -> {"U", "C", "T"},
|
|---|
| 696 | PropagatorType -> Straight,
|
|---|
| 697 | PropagatorArrow -> Forward,
|
|---|
| 698 | PDG -> {2, 4, 6},
|
|---|
| 699 | FullName -> {"u-quark", "c-quark", "t-quark"}},
|
|---|
| 700 |
|
|---|
| 701 | (* Quarks (d): I_3 = -1/2, Q = -1/3, BL=1/3 *)
|
|---|
| 702 | F[4] == {
|
|---|
| 703 | ClassMembers -> {d, s, b},
|
|---|
| 704 | ClassName -> dq,
|
|---|
| 705 | FlavorIndex -> Generation,
|
|---|
| 706 | SelfConjugate -> False,
|
|---|
| 707 | Indices -> {Index[Generation], Index[Colour]},
|
|---|
| 708 | Mass -> {Md, {MD, 5.04*10^(-3)}, {MS, 0.101}, {MB, 4.7}},
|
|---|
| 709 | Width -> 0,
|
|---|
| 710 | QuantumNumbers -> {Q -> -1/3, BarionLepton -> 1/3},
|
|---|
| 711 | ParticleName -> {"d", "s", "b"},
|
|---|
| 712 | AntiParticleName -> {"D", "S", "B"},
|
|---|
| 713 | PropagatorLabel -> {"dq", "d", "s", "b"},
|
|---|
| 714 | PropagatorType -> Straight,
|
|---|
| 715 | PropagatorArrow -> Forward,
|
|---|
| 716 | PDG -> {1,3,5},
|
|---|
| 717 | FullName -> {"d-quark", "s-quark", "b-quark"} },
|
|---|
| 718 |
|
|---|
| 719 |
|
|---|
| 720 | (********** Ghosts **********)
|
|---|
| 721 | U[1] == {
|
|---|
| 722 | ClassName -> ghA,
|
|---|
| 723 | SelfConjugate -> False,
|
|---|
| 724 | Indices -> {},
|
|---|
| 725 | Ghost -> A,
|
|---|
| 726 | Mass -> 0,
|
|---|
| 727 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 728 | PropagatorLabel -> uA,
|
|---|
| 729 | PropagatorType -> GhostDash,
|
|---|
| 730 | PropagatorArrow -> Forward},
|
|---|
| 731 |
|
|---|
| 732 | U[2] == {
|
|---|
| 733 | ClassName -> ghZ,
|
|---|
| 734 | SelfConjugate -> False,
|
|---|
| 735 | Indices -> {},
|
|---|
| 736 | Mass -> {MZ, Internal},
|
|---|
| 737 | Ghost -> Z,
|
|---|
| 738 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 739 | PropagatorLabel -> uZ,
|
|---|
| 740 | PropagatorType -> GhostDash,
|
|---|
| 741 | PropagatorArrow -> Forward},
|
|---|
| 742 |
|
|---|
| 743 | U[31] == {
|
|---|
| 744 | ClassName -> ghWp,
|
|---|
| 745 | SelfConjugate -> False,
|
|---|
| 746 | Indices -> {},
|
|---|
| 747 | Mass -> {MW, Internal},
|
|---|
| 748 | Ghost -> W,
|
|---|
| 749 | QuantumNumbers -> {Q-> 1, GhostNumber -> 1},
|
|---|
| 750 | PropagatorLabel -> uWp,
|
|---|
| 751 | PropagatorType -> GhostDash,
|
|---|
| 752 | PropagatorArrow -> Forward},
|
|---|
| 753 |
|
|---|
| 754 | U[32] == {
|
|---|
| 755 | ClassName -> ghWm,
|
|---|
| 756 | SelfConjugate -> False,
|
|---|
| 757 | Indices -> {},
|
|---|
| 758 | Mass -> {MW, Internal},
|
|---|
| 759 | Ghost -> Wbar,
|
|---|
| 760 | QuantumNumbers -> {Q-> -1, GhostNumber -> 1},
|
|---|
| 761 | PropagatorLabel -> uWm,
|
|---|
| 762 | PropagatorType -> GhostDash,
|
|---|
| 763 | PropagatorArrow -> Forward},
|
|---|
| 764 |
|
|---|
| 765 | U[4] == {
|
|---|
| 766 | ClassName -> ghG,
|
|---|
| 767 | SelfConjugate -> False,
|
|---|
| 768 | Indices -> {Index[Gluon]},
|
|---|
| 769 | Ghost -> G,
|
|---|
| 770 | Mass -> 0,
|
|---|
| 771 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 772 | PropagatorLabel -> uG,
|
|---|
| 773 | PropagatorType -> GhostDash,
|
|---|
| 774 | PropagatorArrow -> Forward},
|
|---|
| 775 |
|
|---|
| 776 | U[5] == {
|
|---|
| 777 | ClassName -> ghWi,
|
|---|
| 778 | Unphysical -> True,
|
|---|
| 779 | Definitions -> {ghWi[1] -> (ghWp + ghWm)/Sqrt[2],
|
|---|
| 780 | ghWi[2] -> (ghWm - ghWp)/Sqrt[2]/I,
|
|---|
| 781 | ghWi[3] -> cw*Cp ghZ + sw ghA - cw*Sp ghZp},
|
|---|
| 782 | SelfConjugate -> False,
|
|---|
| 783 | Indices -> {Index[SU2W]},
|
|---|
| 784 | FlavorIndex -> SU2W,
|
|---|
| 785 | Ghost -> Wi},
|
|---|
| 786 |
|
|---|
| 787 | U[6] == {
|
|---|
| 788 | ClassName -> ghB,
|
|---|
| 789 | SelfConjugate -> False,
|
|---|
| 790 | Definitions -> {ghB -> -sw*Cp ghZ + cw ghA + sw*Sp ghZp},
|
|---|
| 791 | Indices -> {},
|
|---|
| 792 | Unphysical -> True,
|
|---|
| 793 | Ghost -> B},
|
|---|
| 794 |
|
|---|
| 795 | U[7] == {
|
|---|
| 796 | ClassName -> ghZp,
|
|---|
| 797 | SelfConjugate -> False,
|
|---|
| 798 | Indices -> {},
|
|---|
| 799 | Mass -> {MZp, Internal},
|
|---|
| 800 | Ghost -> Zp,
|
|---|
| 801 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 802 | PropagatorLabel -> uZp,
|
|---|
| 803 | PropagatorType -> GhostDash,
|
|---|
| 804 | PropagatorArrow -> Forward},
|
|---|
| 805 |
|
|---|
| 806 | U[8] == {
|
|---|
| 807 | ClassName -> ghBp,
|
|---|
| 808 | SelfConjugate -> False,
|
|---|
| 809 | Definitions -> {ghBp -> Sp ghZ + Cp ghZp},
|
|---|
| 810 | Indices -> {},
|
|---|
| 811 | Unphysical -> True,
|
|---|
| 812 | Ghost -> Bp},
|
|---|
| 813 |
|
|---|
| 814 | (************ Gauge Bosons ***************)
|
|---|
| 815 | (* Gauge bosons: Q = 0 *)
|
|---|
| 816 | V[1] == {
|
|---|
| 817 | ClassName -> A,
|
|---|
| 818 | SelfConjugate -> True,
|
|---|
| 819 | Indices -> {},
|
|---|
| 820 | Mass -> 0,
|
|---|
| 821 | Width -> 0,
|
|---|
| 822 | PropagatorLabel -> "a",
|
|---|
| 823 | PropagatorType -> W,
|
|---|
| 824 | PropagatorArrow -> None,
|
|---|
| 825 | PDG -> 22,
|
|---|
| 826 | FullName -> "Photon" },
|
|---|
| 827 |
|
|---|
| 828 | V[2] == {
|
|---|
| 829 | ClassName -> Z,
|
|---|
| 830 | SelfConjugate -> True,
|
|---|
| 831 | Indices -> {},
|
|---|
| 832 | Mass -> {MZ, Internal},
|
|---|
| 833 | Width -> {WZ, 2.4952},
|
|---|
| 834 | PropagatorLabel -> "Z",
|
|---|
| 835 | PropagatorType -> Sine,
|
|---|
| 836 | PropagatorArrow -> None,
|
|---|
| 837 | PDG -> 23,
|
|---|
| 838 | FullName -> "Z" },
|
|---|
| 839 |
|
|---|
| 840 | (* Gauge bosons: Q = -1 *)
|
|---|
| 841 | V[3] == {
|
|---|
| 842 | ClassName -> W,
|
|---|
| 843 | SelfConjugate -> False,
|
|---|
| 844 | Indices -> {},
|
|---|
| 845 | Mass -> {MW, Internal},
|
|---|
| 846 | Width -> {WW, 2.085},
|
|---|
| 847 | QuantumNumbers -> {Q -> 1},
|
|---|
| 848 | PropagatorLabel -> "W",
|
|---|
| 849 | PropagatorType -> Sine,
|
|---|
| 850 | PropagatorArrow -> Forward,
|
|---|
| 851 | ParticleName ->"W+",
|
|---|
| 852 | AntiParticleName ->"W-",
|
|---|
| 853 | PDG -> 24,
|
|---|
| 854 | FullName -> "W" },
|
|---|
| 855 |
|
|---|
| 856 | V[4] == {
|
|---|
| 857 | ClassName -> G,
|
|---|
| 858 | SelfConjugate -> True,
|
|---|
| 859 | Indices -> {Index[Gluon]},
|
|---|
| 860 | Mass -> 0,
|
|---|
| 861 | Width -> 0,
|
|---|
| 862 | PropagatorLabel -> G,
|
|---|
| 863 | PropagatorType -> C,
|
|---|
| 864 | PropagatorArrow -> None,
|
|---|
| 865 | PDG -> 21,
|
|---|
| 866 | FullName -> "G" },
|
|---|
| 867 |
|
|---|
| 868 | V[5] == {
|
|---|
| 869 | ClassName -> Wi,
|
|---|
| 870 | Unphysical -> True,
|
|---|
| 871 | Definitions -> {Wi[mu_, 1] -> (W[mu] + Wbar[mu])/Sqrt[2],
|
|---|
| 872 | Wi[mu_, 2] -> (Wbar[mu] - W[mu])/Sqrt[2]/I,
|
|---|
| 873 | Wi[mu_, 3] -> sw A[mu] + cw*Cp Z[mu] - cw*Sp Zp[mu]},
|
|---|
| 874 | SelfConjugate -> True,
|
|---|
| 875 | Indices -> {Index[SU2W]},
|
|---|
| 876 | FlavorIndex -> SU2W,
|
|---|
| 877 | Mass -> 0,
|
|---|
| 878 | PDG -> {1,2,3}},
|
|---|
| 879 |
|
|---|
| 880 | V[6] == {
|
|---|
| 881 | ClassName -> B,
|
|---|
| 882 | SelfConjugate -> True,
|
|---|
| 883 | Definitions -> {B[mu_] -> cw A[mu] - sw*Cp Z[mu] + sw*Sp Zp[mu]},
|
|---|
| 884 | Indices -> {},
|
|---|
| 885 | Mass -> 0,
|
|---|
| 886 | Unphysical -> True},
|
|---|
| 887 |
|
|---|
| 888 | V[7] == {
|
|---|
| 889 | ClassName -> Zp,
|
|---|
| 890 | SelfConjugate -> True,
|
|---|
| 891 | Indices -> {},
|
|---|
| 892 | Mass -> {MZp, Internal},
|
|---|
| 893 | Width -> {WZp, 80.00},
|
|---|
| 894 | PropagatorLabel -> "Zp",
|
|---|
| 895 | PropagatorType -> Sine,
|
|---|
| 896 | PropagatorArrow -> None,
|
|---|
| 897 | PDG -> 9900032,
|
|---|
| 898 | FullName -> "Zp" },
|
|---|
| 899 |
|
|---|
| 900 | V[8] == {
|
|---|
| 901 | ClassName -> Bp,
|
|---|
| 902 | SelfConjugate -> True,
|
|---|
| 903 | Definitions -> {Bp[mu_] -> Sp Z[mu] + Cp Zp[mu]},
|
|---|
| 904 | Indices -> {},
|
|---|
| 905 | Unphysical -> True},
|
|---|
| 906 |
|
|---|
| 907 |
|
|---|
| 908 | (************ Scalar Fields **********)
|
|---|
| 909 | (* physical Higgs: Q = 0 *)
|
|---|
| 910 | S[1] == {
|
|---|
| 911 | ClassName -> H1,
|
|---|
| 912 | SelfConjugate -> True,
|
|---|
| 913 | Mass -> {MH1, Internal},
|
|---|
| 914 | Width -> {WH1, 1.5},
|
|---|
| 915 | PropagatorLabel -> "H1",
|
|---|
| 916 | PropagatorType -> D,
|
|---|
| 917 | PropagatorArrow -> None,
|
|---|
| 918 | PDG -> 9900025,
|
|---|
| 919 | FullName -> "H1" },
|
|---|
| 920 |
|
|---|
| 921 | S[2] == {
|
|---|
| 922 | ClassName -> phiZ,
|
|---|
| 923 | SelfConjugate -> True,
|
|---|
| 924 | Mass -> {MZ, Internal},
|
|---|
| 925 | Width -> Wphi,
|
|---|
| 926 | PropagatorLabel -> "PhiZ",
|
|---|
| 927 | PropagatorType -> D,
|
|---|
| 928 | PropagatorArrow -> None,
|
|---|
| 929 | ParticleName ->"phiZ",
|
|---|
| 930 | PDG -> 9900250,
|
|---|
| 931 | FullName -> "PhiZ",
|
|---|
| 932 | Goldstone -> Z },
|
|---|
| 933 |
|
|---|
| 934 | S[3] == {
|
|---|
| 935 | ClassName -> phi2,
|
|---|
| 936 | SelfConjugate -> False,
|
|---|
| 937 | Mass -> {MW, Internal},
|
|---|
| 938 | Width -> Wphi2,
|
|---|
| 939 | PropagatorLabel -> "Phi2",
|
|---|
| 940 | PropagatorType -> D,
|
|---|
| 941 | PropagatorArrow -> None,
|
|---|
| 942 | ParticleName ->"phi+",
|
|---|
| 943 | AntiParticleName ->"phi-",
|
|---|
| 944 | PDG -> 9900251,
|
|---|
| 945 | FullName -> "Phi2",
|
|---|
| 946 | Goldstone -> W,
|
|---|
| 947 | QuantumNumbers -> {Q -> 1}},
|
|---|
| 948 |
|
|---|
| 949 | S[4] == {
|
|---|
| 950 | ClassName -> H2,
|
|---|
| 951 | SelfConjugate -> True,
|
|---|
| 952 | Mass -> {MH2, Internal},
|
|---|
| 953 | Width -> {WH2, 10},
|
|---|
| 954 | PropagatorLabel -> "H2",
|
|---|
| 955 | PropagatorType -> D,
|
|---|
| 956 | PropagatorArrow -> None,
|
|---|
| 957 | PDG -> 9900026,
|
|---|
| 958 | FullName -> "H2" },
|
|---|
| 959 |
|
|---|
| 960 | S[5] == {
|
|---|
| 961 | ClassName -> phiZp,
|
|---|
| 962 | SelfConjugate -> True,
|
|---|
| 963 | Mass -> {MZp, Internal},
|
|---|
| 964 | Width -> WphiZp,
|
|---|
| 965 | PropagatorLabel -> "PhiZp",
|
|---|
| 966 | PropagatorType -> D,
|
|---|
| 967 | PropagatorArrow -> None,
|
|---|
| 968 | ParticleName ->"phiZp",
|
|---|
| 969 | PDG -> 9900252,
|
|---|
| 970 | FullName -> "PhiZp",
|
|---|
| 971 | Goldstone -> Zp },
|
|---|
| 972 |
|
|---|
| 973 | S[6] == {
|
|---|
| 974 | ClassName -> phi,
|
|---|
| 975 | Unphysical -> True,
|
|---|
| 976 | Definitions -> {phi -> cg phiZ - sg phiZp},
|
|---|
| 977 | SelfConjugate -> True},
|
|---|
| 978 |
|
|---|
| 979 | S[7] == {
|
|---|
| 980 | ClassName -> phip,
|
|---|
| 981 | Unphysical -> True,
|
|---|
| 982 | Definitions -> {phip -> sg phiZ + cg phiZp},
|
|---|
| 983 | SelfConjugate -> True},
|
|---|
| 984 |
|
|---|
| 985 | S[8] == {
|
|---|
| 986 | ClassName -> phic,
|
|---|
| 987 | Unphysical -> True,
|
|---|
| 988 | Definitions -> {phic[1] -> (phi2 + phi2bar)/Sqrt[2],
|
|---|
| 989 | phic[2] -> (phi2bar - phi2)/Sqrt[2]/I},
|
|---|
| 990 | SelfConjugate -> False}
|
|---|
| 991 |
|
|---|
| 992 | }
|
|---|
| 993 |
|
|---|
| 994 |
|
|---|
| 995 | (*****************************************************************************************)
|
|---|
| 996 |
|
|---|
| 997 | (* mZp Lagrangian *)
|
|---|
| 998 |
|
|---|
| 999 | (******************** Gauge F^2 Lagrangian terms*************************)
|
|---|
| 1000 | (*Sign convention from Lagrangian in between Eq. (A.9) and Eq. (A.10) of Peskin & Schroeder.*)
|
|---|
| 1001 | LGauge = -1/4 (del[Wi[nu, i1], mu] - del[Wi[mu, i1], nu] + gw Eps[i1, i2, i3] Wi[mu, i2] Wi[nu, i3])*
|
|---|
| 1002 | (del[Wi[nu, i1], mu] - del[Wi[mu, i1], nu] + gw Eps[i1, i4, i5] Wi[mu, i4] Wi[nu, i5]) -
|
|---|
| 1003 |
|
|---|
| 1004 | 1/4 (del[B[nu], mu] - del[B[mu], nu])^2 - 1/4 (del[Bp[nu], mu] - del[Bp[mu], nu])^2 -
|
|---|
| 1005 |
|
|---|
| 1006 | 1/4 (del[G[nu, a1], mu] - del[G[mu, a1], nu] + gs f[a1, a2, a3] G[mu, a2] G[nu, a3])*
|
|---|
| 1007 | (del[G[nu, a1], mu] - del[G[mu, a1], nu] + gs f[a1, a4, a5] G[mu, a4] G[nu, a5]);
|
|---|
| 1008 |
|
|---|
| 1009 |
|
|---|
| 1010 | (********************* Fermion Lagrangian terms*************************)
|
|---|
| 1011 | (*Sign convention from Lagrangian in between Eq. (A.9) and Eq. (A.10) of Peskin & Schroeder.*)
|
|---|
| 1012 | LFermions = Module[{Lkin, LQCD, LEWleft, LEWright},
|
|---|
| 1013 |
|
|---|
| 1014 | Lkin = I uqbar.Ga[mu].del[uq, mu] +
|
|---|
| 1015 | I dqbar.Ga[mu].del[dq, mu] +
|
|---|
| 1016 | I lbar.Ga[mu].del[l, mu] +
|
|---|
| 1017 | I left[anti[vl]].Ga[mu].del[left[vl],mu] +
|
|---|
| 1018 | I right[anti[vl]].Ga[mu].del[right[vl],mu];
|
|---|
| 1019 |
|
|---|
| 1020 | LQCD = gs (uqbar.Ga[mu].T[a].uq +
|
|---|
| 1021 | dqbar.Ga[mu].T[a].dq)G[mu, a];
|
|---|
| 1022 |
|
|---|
| 1023 | LBright =
|
|---|
| 1024 | -2ee/cw B[mu]/2 lbar.Ga[mu].ProjP.l + (*Y_lR=-2*)
|
|---|
| 1025 | 4ee/3/cw B[mu]/2 uqbar.Ga[mu].ProjP.uq - (*Y_uR=4/3*)
|
|---|
| 1026 | 2ee/3/cw B[mu]/2 dqbar.Ga[mu].ProjP.dq; (*Y_dR=-2/3*)
|
|---|
| 1027 |
|
|---|
| 1028 | LBleft =
|
|---|
| 1029 | -ee/cw B[mu]/2 left[anti[vl]].Ga[mu].ProjM.vl - (*Y_LL=-1*)
|
|---|
| 1030 | ee/cw B[mu]/2 lbar.Ga[mu].ProjM.l + (*Y_LL=-1*)
|
|---|
| 1031 | ee/3/cw B[mu]/2 uqbar.Ga[mu].ProjM.uq + (*Y_QL=1/3*)
|
|---|
| 1032 | ee/3/cw B[mu]/2 dqbar.Ga[mu].ProjM.dq ; (*Y_QL=1/3*)
|
|---|
| 1033 |
|
|---|
| 1034 | LWleft = ee/sw/2(
|
|---|
| 1035 | left[anti[vl]].Ga[mu].ProjM.vl Wi[mu, 3] - (*sigma3 = ( 1 0 )*)
|
|---|
| 1036 | lbar.Ga[mu].ProjM.l Wi[mu, 3] + (* ( 0 -1 )*)
|
|---|
| 1037 |
|
|---|
| 1038 | Sqrt[2] left[anti[vl]].Ga[mu].ProjM.l W[mu] +
|
|---|
| 1039 | Sqrt[2] lbar.Ga[mu].ProjM.vl Wbar[mu]+
|
|---|
| 1040 |
|
|---|
| 1041 | uqbar.Ga[mu].ProjM.uq Wi[mu, 3] - (*sigma3 = ( 1 0 )*)
|
|---|
| 1042 | dqbar.Ga[mu].ProjM.dq Wi[mu, 3] + (* ( 0 -1 )*)
|
|---|
| 1043 |
|
|---|
| 1044 | Sqrt[2] uqbar.Ga[mu].ProjM.CKM.dq W[mu] +
|
|---|
| 1045 | Sqrt[2] dqbar.Ga[mu].ProjM.HC[CKM].uq Wbar[mu]
|
|---|
| 1046 | );
|
|---|
| 1047 |
|
|---|
| 1048 | LBpright =
|
|---|
| 1049 | - g1p Bp[mu] right[anti[vl]].Ga[mu].ProjP.vl + (*Y_vlR=0, BL_vlR=-1*)
|
|---|
| 1050 | (-1*gt -g1p) Bp[mu] lbar.Ga[mu].ProjP.l + (*Y_lR=-1, BL_lR=-1*)
|
|---|
| 1051 | (2/3*gt + g1p/3) Bp[mu] uqbar.Ga[mu].ProjP.uq + (*Y_uR=2/3, BL_uR=1/3*)
|
|---|
| 1052 | (-1/3*gt + g1p/3) Bp[mu] dqbar.Ga[mu].ProjP.dq; (*Y_dR=-1/3, BL_dR=1/3*)
|
|---|
| 1053 |
|
|---|
| 1054 | LBpleft =
|
|---|
| 1055 | - (gt/2 + g1p) Bp[mu] left[anti[vl]].Ga[mu].ProjM.vl - (*Y_lL=-1/2, BL_vlL=-1*)
|
|---|
| 1056 | (gt/2 + g1p) Bp[mu] lbar.Ga[mu].ProjM.l + (*Y_lL=-1/2, BL_lL=-1*)
|
|---|
| 1057 | (gt/3/2 + g1p/3) Bp[mu] uqbar.Ga[mu].ProjM.uq + (*Y_qL=1/6, BL_uL=1/3*)
|
|---|
| 1058 | (gt/3/2 + g1p/3) Bp[mu] dqbar.Ga[mu].ProjM.dq (*Y_qL=1/6, BL_dL=1/3*)
|
|---|
| 1059 | ;
|
|---|
| 1060 |
|
|---|
| 1061 | Lkin + LQCD + LBright + LBleft + LWleft + LBpright + LBpleft ];
|
|---|
| 1062 |
|
|---|
| 1063 | (******************** Higgs Lagrangian terms****************************)
|
|---|
| 1064 | Phi := If[FeynmanGauge, {-I phi2, (v + Ca*H1+Sa*H2 + I phi)/Sqrt[2]}, {0, (v + Ca*H1+Sa*H2)/Sqrt[2]}];
|
|---|
| 1065 | Phibar := If[FeynmanGauge, {I phi2bar, (v + Ca*H1+Sa*H2 - I phi)/Sqrt[2]} ,{0, (v + Ca*H1+Sa*H2)/Sqrt[2]}];
|
|---|
| 1066 |
|
|---|
| 1067 | Chi := If[FeynmanGauge, {(x -Sa*H1+Ca*H2 + I phip)/Sqrt[2]}, {(x -Sa*H1+Ca*H2)/Sqrt[2]}];
|
|---|
| 1068 | Chibar := If[FeynmanGauge, {(x -Sa*H1+Ca*H2 - I phip)/Sqrt[2]}, {(x -Sa*H1+Ca*H2)/Sqrt[2]}];
|
|---|
| 1069 |
|
|---|
| 1070 | LHiggs := Block[{PMVec, WVec, Dc, Dcbar, Vphichi, Dcp, Dcpbar},
|
|---|
| 1071 |
|
|---|
| 1072 | PMVec = Table[PauliSigma[i], {i, 3}];
|
|---|
| 1073 | Wvec[mu_] := {Wi[mu, 1], Wi[mu, 2], Wi[mu, 3]};
|
|---|
| 1074 |
|
|---|
| 1075 | (*Y_phi=1/2*)
|
|---|
| 1076 | Dc[f_, mu_] := I del[f, mu] + ee/cw B[mu]/2 f + gt/2 Bp[mu] f + ee/sw/2 (Wvec[mu].PMVec).f;
|
|---|
| 1077 | Dcbar[f_, mu_] := -I del[f, mu] + ee/cw B[mu]/2 f + gt/2 Bp[mu] f + ee/sw/2 f.(Wvec[mu].PMVec);
|
|---|
| 1078 |
|
|---|
| 1079 | (*BL_phi=2*)
|
|---|
| 1080 | Dcp[f_, mu_] := I del[f, mu] + 2*g1p Bp[mu] f ;
|
|---|
| 1081 | Dcpbar[f_, mu_] := -I del[f, mu] + 2*g1p Bp[mu] f ;
|
|---|
| 1082 |
|
|---|
| 1083 | Vphichi[Phi_, Phibar_, Chi_, Chibar_] := mu2H1 Phibar.Phi + mu2H2 Chibar.Chi +
|
|---|
| 1084 | \[Lambda]1 (Phibar.Phi)^2 + \[Lambda]2 (Chibar.Chi)^2 + \[Lambda]3 (Phibar.Phi)*(Chibar.Chi);
|
|---|
| 1085 |
|
|---|
| 1086 | (Dcbar[Phibar, mu]).Dc[Phi, mu] + (Dcpbar[Chibar, mu]).Dcp[Chi, mu] - Vphichi[Phi, Phibar, Chi, Chibar]
|
|---|
| 1087 |
|
|---|
| 1088 | ];
|
|---|
| 1089 |
|
|---|
| 1090 |
|
|---|
| 1091 |
|
|---|
| 1092 | (*************** Yukawa Lagrangian***********************)
|
|---|
| 1093 | (*NOTE: Neutrino states have been expanded on the LH/RH components and the LH mass terms have been changed signs*)
|
|---|
| 1094 |
|
|---|
| 1095 | LYuk := If[FeynmanGauge,
|
|---|
| 1096 |
|
|---|
| 1097 | Module[{s,r,n,m,i}, -
|
|---|
| 1098 | yd[m] CKM[n,m] uqbar[s,n,i].ProjP[s,r].dq[r,m,i] (-I phi2) -
|
|---|
| 1099 | yd[n] dqbar[s,n,i].ProjP[s,r].dq[r,n,i] (v+Ca*H1+Sa*H2 +I phi)/Sqrt[2] -
|
|---|
| 1100 |
|
|---|
| 1101 | yu[n] uqbar[s,n,i].ProjP[s,r].uq[r,n,i] (v+Ca*H1+Sa*H2 -I phi)/Sqrt[2] + (*This sign from eps matrix*)
|
|---|
| 1102 | yu[m] Conjugate[CKM[m,n]] dqbar[s,n,i].ProjP[s,r].uq[r,m,i] ( I phi2bar)
|
|---|
| 1103 |
|
|---|
| 1104 | - yl[n] Can[n] anti[nL][s,n].ProjP[s,r].l[r,n] (-I phi2)
|
|---|
| 1105 | + yl[n] San[n] anti[nH][s,n].ProjP[s,r].l[r,n] (-I phi2)
|
|---|
| 1106 |
|
|---|
| 1107 | - yl[n] lbar[s,n].ProjP[s,r].l[r,n] (v+Ca*H1+Sa*H2 +I phi)/Sqrt[2] +
|
|---|
| 1108 | ynd[n] San[n] Can[n] anti[nL][s,n].ProjP[s,r].nL[r,n] (v+Ca*H1+Sa*H2 - I phi)/Sqrt[2]+
|
|---|
| 1109 | ynd[n] San[n] Can[n] anti[nH][s,n].ProjP[s,r].nH[r,n] (v+Ca*H1+Sa*H2 - I phi)/Sqrt[2]-
|
|---|
| 1110 |
|
|---|
| 1111 | ynd[n] (Can[n] Can[n] - San[n] San[n]) anti[nL][s,n].ProjP[s,r].nH[r,n] (v+Ca*H1+Sa*H2 - I phi)/Sqrt[2]
|
|---|
| 1112 |
|
|---|
| 1113 | - ynd[n] San[n] lbar[s,n].ProjP[s,r].nL[r,n] (I phi2bar) +
|
|---|
| 1114 | ynd[n] Can[n] lbar[s,n].ProjP[s,r].nH[r,n] (I phi2bar) +
|
|---|
| 1115 |
|
|---|
| 1116 | ynm[n] San[n] San[n] anti[nL][s,n].ProjP[s,r].nL[r,n] (x-Sa*H1+Ca*H2 + I phip)/Sqrt[2]-
|
|---|
| 1117 | ynm[n] Can[n] Can[n] anti[nH][s,n].ProjP[s,r].nH[r,n] (x-Sa*H1+Ca*H2 + I phip)/Sqrt[2]-
|
|---|
| 1118 |
|
|---|
| 1119 | ynm[n] 2 San[n] Can[n] anti[nL][s,n].ProjP[s,r].nH[r,n] (x-Sa*H1+Ca*H2 + I phip)/Sqrt[2]
|
|---|
| 1120 |
|
|---|
| 1121 |
|
|---|
| 1122 | ],
|
|---|
| 1123 |
|
|---|
| 1124 | Module[{s,r,n,m,i}, -
|
|---|
| 1125 | yd[n] dqbar[s,n,i].ProjP[s,r].dq[r,n,i] (v+Ca*H1+Sa*H2)/Sqrt[2] -
|
|---|
| 1126 | yu[n] uqbar[s,n,i].ProjP[s,r].uq[r,n,i] (v+Ca*H1+Sa*H2)/Sqrt[2]
|
|---|
| 1127 |
|
|---|
| 1128 | - yl[n] lbar[s,n].ProjP[s,r].l[r,n] (v+Ca*H1+Sa*H2)/Sqrt[2] +
|
|---|
| 1129 | ynd[n] San[n] Can[n] anti[nL][s,n].ProjP[s,r].nL[r,n] (v+Ca*H1+Sa*H2)/Sqrt[2]+
|
|---|
| 1130 | ynd[n] San[n] Can[n] anti[nH][s,n].ProjP[s,r].nH[r,n] (v+Ca*H1+Sa*H2)/Sqrt[2]-
|
|---|
| 1131 |
|
|---|
| 1132 | ynd[n] (Can[n] Can[n] - San[n] San[n]) anti[nL][s,n].ProjP[s,r].nH[r,n] (v+Ca*H1+Sa*H2)/Sqrt[2]+
|
|---|
| 1133 |
|
|---|
| 1134 |
|
|---|
| 1135 |
|
|---|
| 1136 | ynm[n] San[n] San[n] anti[nL][s,n].ProjP[s,r].nL[r,n] (x-Sa*H1+Ca*H2)/Sqrt[2]-
|
|---|
| 1137 | ynm[n] Can[n] Can[n] anti[nH][s,n].ProjP[s,r].nH[r,n] (x-Sa*H1+Ca*H2)/Sqrt[2]-
|
|---|
| 1138 |
|
|---|
| 1139 | ynm[n] 2 San[n] Can[n] anti[nL][s,n].ProjP[s,r].nH[r,n] (x-Sa*H1+Ca*H2)/Sqrt[2]
|
|---|
| 1140 |
|
|---|
| 1141 | ]
|
|---|
| 1142 | ];
|
|---|
| 1143 |
|
|---|
| 1144 | LYukawa := LYuk + HC[LYuk];
|
|---|
| 1145 |
|
|---|
| 1146 |
|
|---|
| 1147 |
|
|---|
| 1148 | (**************Ghost terms**************************)
|
|---|
| 1149 | (* Now we need the ghost terms which are of the form: *)
|
|---|
| 1150 | (* - g * antighost * d_BRST G *)
|
|---|
| 1151 | (* where d_BRST G is BRST transform of the gauge fixing function. *)
|
|---|
| 1152 |
|
|---|
| 1153 | LGhost := If[FeynmanGauge,
|
|---|
| 1154 | Block[{dBRSTG,LGhostG,dBRSTWi,LGhostWi,dBRSTB,LGhostB, dBRSTBp, LGhostBp},
|
|---|
| 1155 |
|
|---|
| 1156 | (***********First the pure gauge piece.**********************)
|
|---|
| 1157 | dBRSTG[mu_,a_] := 1/gs Module[{a2, a3}, del[ghG[a], mu] + gs f[a,a2,a3] G[mu,a2] ghG[a3]];
|
|---|
| 1158 | LGhostG := - gs ghGbar[a].del[dBRSTG[mu,a],mu];
|
|---|
| 1159 |
|
|---|
| 1160 | dBRSTWi[mu_,i_] := sw/ee Module[{i2, i3}, del[ghWi[i], mu] + ee/sw Eps[i,i2,i3] Wi[mu,i2] ghWi[i3] ];
|
|---|
| 1161 | LGhostWi := - ee/sw ghWibar[a].del[dBRSTWi[mu,a],mu];
|
|---|
| 1162 |
|
|---|
| 1163 | dBRSTB[mu_] := cw/ee del[ghB, mu];
|
|---|
| 1164 | LGhostB := - ee/cw ghBbar.del[dBRSTB[mu],mu];
|
|---|
| 1165 |
|
|---|
| 1166 | dBRSTBp[mu_] := 1/g1p del[ghBp, mu];
|
|---|
| 1167 | LGhostBp := - g1p ghBpbar.del[dBRSTBp[mu],mu];
|
|---|
| 1168 |
|
|---|
| 1169 | (***********Next the piece from the scalar field.************)
|
|---|
| 1170 | LGhostphi :=
|
|---|
| 1171 | (*- ee/(2*sw*cw) MW ( - I phi2 ( (cw^2-sw^2)ghWpbar.ghZ + 2sw*cw ghWpbar.ghA ) +
|
|---|
| 1172 | I phi2bar ( (cw^2-sw^2)ghWmbar.ghZ + 2sw*cw ghWmbar.ghA ) ) -
|
|---|
| 1173 | ee/(2*sw) MW ( ( (v+Ca*H1+Sa*H2) + I phi) ghWpbar.ghWp +
|
|---|
| 1174 | ( (v+Ca*H1+Sa*H2) - I phi) ghWmbar.ghWm ) -
|
|---|
| 1175 | I ee/(2*sw) MZ ( - phi2bar ghZbar.ghWp + phi2 ghZbar.ghWm ) -
|
|---|
| 1176 | ee/(2*sw*cw) MZ (v+Ca*H1+Sa*H2) ghZbar.ghZ *)
|
|---|
| 1177 |
|
|---|
| 1178 | 1/4*gw*v (-gw*(v+Ca*H1+Sa*H2) ghWibar[1].ghWi[1] +g1 phic[2] ghWibar[1].ghB +gw phic[2] ghWibar[1].ghWi[3] -gw phi ghWibar[1].ghWi[2] + gt phic[2] ghWibar[1].ghBp) +
|
|---|
| 1179 | 1/4*gw*v (-gw*(v+Ca*H1+Sa*H2) ghWibar[2].ghWi[2] -g1 phic[1] ghWibar[2].ghB -gw phic[1] ghWibar[2].ghWi[3] +gw phi ghWibar[2].ghWi[1] -gt phic[1] ghWibar[2].ghBp) +
|
|---|
| 1180 | 1/4*gw*v (g1*(v+Ca*H1+Sa*H2) ghWibar[3].ghB -gw*(v+Ca*H1+Sa*H2) ghWibar[3].ghWi[3] +gw phic[1] ghWibar[3].ghWi[2]
|
|---|
| 1181 | -gw phic[2] ghWibar[3].ghWi[1] +gt (v+Ca*H1+Sa*H2) ghWibar[3].ghBp ) +
|
|---|
| 1182 | 1/4*g1*v (-g1*(v+Ca*H1+Sa*H2) ghBbar.ghB +gw*(v+Ca*H1+Sa*H2) ghBbar.ghWi[3] -gw phic[1] ghBbar.ghWi[2] +gw phic[2] ghBbar.ghWi[1] -gt*(v+Ca*H1+Sa*H2) ghBbar.ghBp) +
|
|---|
| 1183 | 1/4*gt*v (-g1*(v+Ca*H1+Sa*H2) ghBpbar.ghB +gw*(v+Ca*H1+Sa*H2) ghBpbar.ghWi[3] -gw phic[1] ghBpbar.ghWi[2] +gw phic[2] ghBpbar.ghWi[1] -gt (v+Ca*H1+Sa*H2) ghBpbar.ghBp) -
|
|---|
| 1184 | 4*g1p^2*x*(x-Sa*H1+Ca*H2) ghBpbar.ghBp
|
|---|
| 1185 | ;
|
|---|
| 1186 |
|
|---|
| 1187 | (***********Now add the pieces together.********************)
|
|---|
| 1188 | LGhostG + LGhostWi + LGhostB + LGhostphi + LGhostBp ]
|
|---|
| 1189 |
|
|---|
| 1190 | ,
|
|---|
| 1191 |
|
|---|
| 1192 | (*If unitary gauge, only include the gluonic ghost.*)
|
|---|
| 1193 | Block[{dBRSTG,LGhostG},
|
|---|
| 1194 |
|
|---|
| 1195 | (***********First the pure gauge piece.**********************)
|
|---|
| 1196 | dBRSTG[mu_,a_] := 1/gs Module[{a2, a3}, del[ghG[a], mu] + gs f[a,a2,a3] G[mu,a2] ghG[a3]];
|
|---|
| 1197 | LGhostG := - gs ghGbar[a].del[dBRSTG[mu,a],mu];
|
|---|
| 1198 |
|
|---|
| 1199 | (***********Now add the pieces together.********************)
|
|---|
| 1200 | LGhostG]
|
|---|
| 1201 |
|
|---|
| 1202 | ];
|
|---|
| 1203 |
|
|---|
| 1204 | (*********Total SM Lagrangian*******)
|
|---|
| 1205 | LmZp := LGauge + LHiggs + LFermions + LYukawa + LGhost;
|
|---|