| 1 | (* This is the FeynRules model file for the phenomenological Symmetry Protected Seesaw with light Dirac neutrinos*)
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| 2 | (* The Dirac type light neutrinos allow to enforce lepton number also in processes involving light neutrinos*)
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| 3 | (* Based on the SM model file *)
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| 4 |
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| 5 | M$ModelName = "pSPSS";
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| 6 |
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| 7 | M$Information = {
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| 8 | Version -> "1.2",
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| 9 | Authors -> {"S. Antusch", "J. Hajer", "B. Oliveira", "J. Rosskopp"},
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| 10 | Institutions -> {"University of Lisbon", "University of Basel"},
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| 11 | Emails -> {"stefan.antusch@unibas.ch", "jan.hajer@tecnico.ulisboa.pt", "b.m.silva.oliveira@tecnico.ulisboa.pt", "johannes.rosskopp@unibas.ch"},
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| 12 | References -> {"S. Antusch, J. Hajer, J. Rosskopp, Simulating heavy neutrino-antineutrino oscillations at colliders (2022)", "S. Antusch, J. Hajer, B. Oliveira, Heavy neutrino-antineutrino oscillations at the FCC-ee (2023)"},
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| 13 | URLs -> "https://feynrules.irmp.ucl.ac.be/wiki/pSPSS",
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| 14 | Date -> "24.01.2024"
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| 15 | };
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| 16 |
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| 17 | (* Change log. *)
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| 18 | (* v1.0: First published version. *)
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| 19 | (* v1.1: Light neutrinos are now Dirac in order to simulate neutral initial states. *)
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| 20 | (* v1.2: Correct light neutrino mass normalisation. *)
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| 21 |
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| 22 | (* Choose whether Feynman gauge is desired. If set to False, unitary gauge is assumed. *)
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| 23 | (* Feynman gauge is especially useful for CalcHEP/CompHEP where the calculation is 10-100 times faster. *)
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| 24 | (* Feynman gauge is not supported in MadGraph and Sherpa. *)
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| 25 |
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| 26 | FeynmanGauge = False;
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| 27 |
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| 28 | (* NLO Variables *)
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| 29 |
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| 30 | FR$LoopSwitches = {{Gf, mW}};
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| 31 | FR$RmDblExt = {ymb -> mb, ymc -> mc, ymdo -> md, yme -> me, ymm -> mmu, yms -> ms, ymt -> mt, ymtau -> mta, ymup -> mup};
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| 32 |
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| 33 | (* Vacuum expectation values *)
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| 34 |
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| 35 | M$vevs = {
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| 36 | {Phi[2], vev},
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| 37 | {PhiNP[2], vevNP}
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| 38 | };
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| 39 |
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| 40 | (* Gauge groups *)
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| 41 |
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| 42 | M$GaugeGroups = {
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| 43 | U1Y == {
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| 44 | Abelian -> True,
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| 45 | CouplingConstant -> g1,
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| 46 | GaugeBoson -> B,
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| 47 | Charge -> Y
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| 48 | },
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| 49 | SU2L == {
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| 50 | Abelian -> False,
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| 51 | CouplingConstant -> gw,
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| 52 | GaugeBoson -> Wi,
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| 53 | StructureConstant -> Eps,
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| 54 | Representations -> {Ta, SU2D},
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| 55 | Definitions -> {
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| 56 | Ta[a_, b_, c_] -> PauliSigma[a, b, c]/2,
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| 57 | FSU2L[i_, j_, k_] :> I Eps[i, j, k]
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| 58 | }
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| 59 | },
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| 60 | SU3C == {
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| 61 | Abelian -> False,
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| 62 | CouplingConstant -> gs,
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| 63 | GaugeBoson -> G,
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| 64 | StructureConstant -> f,
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| 65 | Representations -> {T, Colour},
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| 66 | SymmetricTensor -> dSUN
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| 67 | }
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| 68 | };
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| 69 |
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| 70 | (* Indices *)
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| 71 |
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| 72 | IndexRange[Index[SU2W]] = Unfold[Range[3]];
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| 73 | IndexRange[Index[SU2D]] = Unfold[Range[2]];
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| 74 | IndexRange[Index[Gluon]] = NoUnfold[Range[8]];
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| 75 | IndexRange[Index[Colour]] = NoUnfold[Range[3]];
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| 76 | IndexRange[Index[Generation]] = Range[3];
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| 77 | IndexRange[Index[NeutrinoGeneration]] = NoUnfold[Range[5]];
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| 78 |
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| 79 | IndexStyle[SU2W, j];
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| 80 | IndexStyle[SU2D, k];
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| 81 | IndexStyle[Gluon, a];
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| 82 | IndexStyle[Colour, m];
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| 83 | IndexStyle[Generation, f];
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| 84 | IndexStyle[NeutrinoGeneration, h];
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| 85 |
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| 86 | (* Interaction orders (as used by MG5) *)
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| 87 |
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| 88 | M$InteractionOrderHierarchy = {
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| 89 | {QCD, 1},
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| 90 | {NP, 1},
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| 91 | {QED, 2}
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| 92 | };
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| 93 |
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| 94 | (* Parameters *)
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| 95 |
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| 96 | M$Parameters = {
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| 97 |
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| 98 | (* External parameters SM *)
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| 99 |
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| 100 | aEWM1 == {
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| 101 | ParameterType -> External,
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| 102 | BlockName -> SMINPUTS,
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| 103 | OrderBlock -> 1,
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| 104 | Value -> 127.9,
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| 105 | InteractionOrder -> {QED, -2},
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| 106 | Description -> "Inverse of the EW coupling constant at the Z pole"
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| 107 | },
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| 108 | Gf == {
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| 109 | ParameterType -> External,
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| 110 | BlockName -> SMINPUTS,
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| 111 | OrderBlock -> 2,
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| 112 | Value -> 1.16637*^-5,
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| 113 | InteractionOrder -> {QED, 2},
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| 114 | TeX -> Subscript[G, F],
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| 115 | Description -> "Fermi constant"
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| 116 | },
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| 117 | aS == {
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| 118 | ParameterType -> External,
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| 119 | BlockName -> SMINPUTS,
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| 120 | OrderBlock -> 3,
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| 121 | Value -> 0.1184,
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| 122 | InteractionOrder -> {QCD, 2},
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| 123 | TeX -> Subscript[\[Alpha], s],
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| 124 | Description -> "Strong coupling constant at the Z pole"
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| 125 | },
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| 126 | ymdo == {
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| 127 | ParameterType -> External,
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| 128 | BlockName -> YUKAWA,
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| 129 | OrderBlock -> 1,
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| 130 | Value -> 5.04*^-3,
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| 131 | Description -> "Down Yukawa mass"
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| 132 | },
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| 133 | ymup == {
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| 134 | ParameterType -> External,
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| 135 | BlockName -> YUKAWA,
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| 136 | OrderBlock -> 2,
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| 137 | Value -> 2.55*^-3,
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| 138 | Description -> "Up Yukawa mass"
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| 139 | },
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| 140 | yms == {
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| 141 | ParameterType -> External,
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| 142 | BlockName -> YUKAWA,
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| 143 | OrderBlock -> 3,
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| 144 | Value -> 0.101,
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| 145 | Description -> "Strange Yukawa mass"
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| 146 | },
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| 147 | ymc == {
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| 148 | ParameterType -> External,
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| 149 | BlockName -> YUKAWA,
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| 150 | OrderBlock -> 4,
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| 151 | Value -> 1.27,
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| 152 | Description -> "Charm Yukawa mass"
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| 153 | },
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| 154 | ymb == {
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| 155 | ParameterType -> External,
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| 156 | BlockName -> YUKAWA,
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| 157 | OrderBlock -> 5,
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| 158 | Value -> 4.7,
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| 159 | Description -> "Bottom Yukawa mass"
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| 160 | },
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| 161 | ymt == {
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| 162 | ParameterType -> External,
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| 163 | BlockName -> YUKAWA,
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| 164 | OrderBlock -> 6,
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| 165 | Value -> 172,
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| 166 | Description -> "Top Yukawa mass"
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| 167 | },
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| 168 | yme == {
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| 169 | ParameterType -> External,
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| 170 | BlockName -> YUKAWA,
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| 171 | OrderBlock -> 11,
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| 172 | Value -> 5.11*^-4,
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| 173 | Description -> "Electron Yukawa mass"
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| 174 | },
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| 175 | ymm == {
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| 176 | ParameterType -> External,
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| 177 | BlockName -> YUKAWA,
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| 178 | OrderBlock -> 13,
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| 179 | Value -> 0.10566,
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| 180 | Description -> "Muon Yukawa mass"
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| 181 | },
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| 182 | ymtau == {
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| 183 | ParameterType -> External,
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| 184 | BlockName -> YUKAWA,
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| 185 | OrderBlock -> 15,
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| 186 | Value -> 1.777,
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| 187 | Description -> "Tau Yukawa mass"
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| 188 | },
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| 189 | cabi == {
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| 190 | ParameterType -> External,
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| 191 | BlockName -> CKMBLOCK,
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| 192 | OrderBlock -> 1,
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| 193 | Value -> 0.227736,
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| 194 | TeX -> Subscript[\[Theta], c],
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| 195 | Description -> "Cabibbo angle"
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| 196 | },
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| 197 |
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| 198 | (* External parameters pSPSS *)
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| 199 |
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| 200 | Mmaj == {
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| 201 | ParameterType -> External,
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| 202 | BlockName -> pSPSS,
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| 203 | Value -> 20,
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| 204 | TeX -> Subscript[m, M],
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| 205 | Description -> "Heavy neutrino Majorana mass"
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| 206 | },
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| 207 | deltaM == {
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| 208 | ParameterType -> External,
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| 209 | BlockName -> pSPSS,
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| 210 | Value -> 1*^-12,
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| 211 | TeX -> Subscript[\[Delta], m],
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| 212 | Description -> "Heavy neutrino mass splitting"
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| 213 | },
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| 214 | theta1 == {
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| 215 | ParameterType -> External,
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| 216 | BlockName -> pSPSS,
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| 217 | Value -> 0,
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| 218 | InteractionOrder -> {NP, 1},
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| 219 | TeX -> Subscript[\[Theta], 1],
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| 220 | Description -> "Active sterile mixing 1"
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| 221 | },
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| 222 | theta2 == {
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| 223 | ParameterType -> External,
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| 224 | BlockName -> pSPSS,
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| 225 | Value -> 1*^-4,
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| 226 | InteractionOrder -> {NP, 1},
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| 227 | TeX -> Subscript[\[Theta], 2],
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| 228 | Description -> "Active sterile mixing 2"
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| 229 | },
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| 230 | theta3 == {
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| 231 | ParameterType -> External,
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| 232 | BlockName -> pSPSS,
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| 233 | Value -> 0,
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| 234 | InteractionOrder -> {NP, 1},
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| 235 | TeX -> Subscript[\[Theta], 3],
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| 236 | Description -> "Active sterile mixing 3"
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| 237 | },
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| 238 | damping == {
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| 239 | ParameterType -> External,
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| 240 | BlockName -> pSPSS,
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| 241 | Value -> 0,
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| 242 | Description -> "Damping parameter"
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| 243 | },
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| 244 |
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| 245 | (* Internal Parameters pSPSS *)
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| 246 |
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| 247 | thetasqr == {
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| 248 | ParameterType -> Internal,
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| 249 | Definitions -> {thetasqr -> theta1 * Conjugate[theta1] + theta2 * Conjugate[theta2] + theta3 * Conjugate[theta3]},
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| 250 | Description -> "Heavy neutrino Yukawa mass 1"
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| 251 | },
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| 252 | mn4 == {
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| 253 | ParameterType -> Internal,
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| 254 | Value -> Mmaj * (1 + thetasqr / 2) - deltaM / 2,
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| 255 | TeX -> Subscript[M, 4],
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| 256 | Description -> "n4 mass"
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| 257 | },
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| 258 | mn5 == {
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| 259 | ParameterType -> Internal,
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| 260 | Value -> Mmaj * (1 + thetasqr / 2) + deltaM / 2,
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| 261 | TeX -> Subscript[M, 5],
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| 262 | Description -> "n5 mass"
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| 263 | },
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| 264 | vevNP == { (* Necessary to get the correct interaction order for new Yukawas *)
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| 265 | ParameterType -> Internal,
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| 266 | Value -> 2 * mW * sw / ee / Sqrt[2],
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| 267 | InteractionOrder -> {NP, -1},
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| 268 | TeX -> v,
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| 269 | Description -> "Higgs vacuum expectation value for NP interactions"
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| 270 | },
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| 271 | yvn1 == {
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| 272 | ParameterType -> Internal,
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| 273 | Value -> Mmaj * theta1 / vevNP,
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| 274 | TeX -> Superscript[y, Subscript[\[Nu], 1]],
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| 275 | Description -> "Heavy neutrino Yukawa 1"
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| 276 | },
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| 277 | yvn2 == {
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| 278 | ParameterType -> Internal,
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| 279 | Value -> Mmaj * theta2 / vevNP,
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| 280 | TeX -> Superscript[y, Subscript[\[Nu], 2]],
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| 281 | Description -> "Heavy neutrino Yukawa 2"
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| 282 | },
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| 283 | yvn3 == {
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| 284 | ParameterType -> Internal,
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| 285 | Value -> Mmaj * theta3 / vevNP,
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| 286 | TeX -> Superscript[y, Subscript[\[Nu], 3]],
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| 287 | Description -> "Heavy neutrino Yukawa 3"
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| 288 | },
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| 289 | yvn == {
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| 290 | ParameterType -> Internal,
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| 291 | Indices -> {Index[Generation]},
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| 292 | Definitions -> {yvn[1] -> yvn1, yvn[2] -> yvn2, yvn[3] -> yvn3},
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| 293 | Description -> "Heavy neutrino Yukawas"
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| 294 | },
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| 295 | Un == {
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| 296 | ParameterType -> Internal,
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| 297 | Indices -> {Index[NeutrinoGeneration], Index[NeutrinoGeneration]},
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| 298 | ComplexParameter -> True,
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| 299 | Definitions -> {
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| 300 | Un[1, 1] -> 1 - theta1 * Conjugate[theta1] / 2,
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| 301 | Un[2, 1] -> - theta1 * Conjugate[theta2] / 2,
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| 302 | Un[3, 1] -> - theta1 * Conjugate[theta3] / 2,
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| 303 | Un[4, 1] -> 0,
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| 304 | Un[5, 1] -> - theta1,
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| 305 | Un[1, 2] -> - theta2 * Conjugate[theta1] / 2,
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| 306 | Un[2, 2] -> 1 - theta2 * Conjugate[theta2] / 2,
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| 307 | Un[3, 2] -> -theta2 * Conjugate[theta3] / 2,
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| 308 | Un[4, 2] -> 0,
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| 309 | Un[5, 2] -> - theta2,
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| 310 | Un[1, 3] -> - theta3 * Conjugate[theta1] / 2,
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| 311 | Un[2, 3] -> - theta3 * Conjugate[theta2] / 2,
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| 312 | Un[3, 3] -> 1 - theta3 * Conjugate[theta3] / 2,
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| 313 | Un[4, 3] -> 0,
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| 314 | Un[5, 3] -> - theta3,
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| 315 | Un[1, 4] -> -I * Conjugate[theta1] / Sqrt[2],
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| 316 | Un[2, 4] -> -I * Conjugate[theta2] / Sqrt[2],
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| 317 | Un[3, 4] -> -I * Conjugate[theta3] / Sqrt[2],
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| 318 | Un[4, 4] -> I / Sqrt[2],
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| 319 | Un[5, 4] -> -I * (1 - thetasqr / 2) / Sqrt[2],
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| 320 | Un[1, 5] -> Conjugate[theta1] / Sqrt[2],
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| 321 | Un[2, 5] -> Conjugate[theta2] / Sqrt[2],
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| 322 | Un[3, 5] -> Conjugate[theta3] / Sqrt[2],
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| 323 | Un[4, 5] -> 1 / Sqrt[2],
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| 324 | Un[5, 5] -> (1 - thetasqr / 2) / Sqrt[2]
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| 325 | },
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| 326 | Description -> "Neutrino 5x5 mixing matrix"
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| 327 | },
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| 328 | UnCL == {
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| 329 | ParameterType -> Internal,
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| 330 | Indices -> {Index[Generation], Index[NeutrinoGeneration]},
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| 331 | ComplexParameter -> True,
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| 332 | Definitions -> {UnCL[i_?NumericQ, j_?NumericQ] :> Un[i, j]},
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| 333 | Description -> "Charged lepton neutrino 3x5 mixing matrix"
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| 334 | },
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| 335 |
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| 336 | (* Internal Parameters SM *)
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| 337 |
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| 338 | aEW == {
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| 339 | ParameterType -> Internal,
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| 340 | Value -> 1/aEWM1,
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| 341 | InteractionOrder -> {QED, 2},
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| 342 | TeX -> Subscript[\[Alpha], EW],
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| 343 | Description -> "Electroweak coupling contant"
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| 344 | },
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| 345 | mW == {
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| 346 | ParameterType -> Internal,
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| 347 | Value -> Sqrt[mZ^2 / 2 + Sqrt[mZ^4 / 4 - Pi / Sqrt[2] * aEW / Gf * mZ^2]],
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| 348 | TeX -> Subscript[M, W],
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| 349 | Description -> "W mass"
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| 350 | },
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| 351 | sw2 == {
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| 352 | ParameterType -> Internal,
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| 353 | Value -> 1 - (mW / mZ)^2,
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| 354 | Description -> "Squared Sin of the Weinberg angle"
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| 355 | },
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| 356 | ee == {
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| 357 | ParameterType -> Internal,
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| 358 | Value -> Sqrt[4 Pi aEW],
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| 359 | InteractionOrder -> {QED, 1},
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| 360 | TeX -> e,
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| 361 | Description -> "Electric coupling constant"
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| 362 | },
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| 363 | cw == {
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| 364 | ParameterType -> Internal,
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| 365 | Value -> Sqrt[1 - sw2],
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| 366 | TeX -> Subscript[c, w],
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| 367 | Description -> "Cosine of the Weinberg angle"
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| 368 | },
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| 369 | sw == {
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| 370 | ParameterType -> Internal,
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| 371 | Value -> Sqrt[sw2],
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| 372 | TeX -> Subscript[s, w],
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| 373 | Description -> "Sine of the Weinberg angle"
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| 374 | },
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| 375 | gw == {
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| 376 | ParameterType -> Internal,
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| 377 | Definitions -> {gw -> ee/sw},
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| 378 | InteractionOrder -> {QED, 1},
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| 379 | TeX -> Subscript[g, w],
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| 380 | Description -> "Weak coupling constant at the Z pole"
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| 381 | },
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| 382 | g1 == {
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| 383 | ParameterType -> Internal,
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| 384 | Definitions -> {g1 -> ee/cw},
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| 385 | InteractionOrder -> {QED, 1},
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| 386 | TeX -> Subscript[g, 1],
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| 387 | Description -> "U(1)Y coupling constant at the Z pole"
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| 388 | },
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| 389 | gs == {
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| 390 | ParameterType -> Internal,
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| 391 | Value -> Sqrt[4 Pi aS],
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| 392 | InteractionOrder -> {QCD, 1},
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| 393 | TeX -> Subscript[g, s],
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| 394 | ParameterName -> G,
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| 395 | Description -> "Strong coupling constant at the Z pole"
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| 396 | },
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| 397 | vev == {
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| 398 | ParameterType -> Internal,
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| 399 | Value -> 2 * mW * sw / ee / Sqrt[2],
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| 400 | InteractionOrder -> {QED, -1},
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| 401 | TeX -> v,
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| 402 | Description -> "Higgs vacuum expectation value"
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| 403 | },
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| 404 | lam == {
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| 405 | ParameterType -> Internal,
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| 406 | Value -> MH^2 / (4 * vev^2),
|
|---|
| 407 | InteractionOrder -> {QED, 2},
|
|---|
| 408 | TeX -> \[Lambda],
|
|---|
| 409 | Description -> "Higgs quartic coupling"
|
|---|
| 410 | },
|
|---|
| 411 | muH == {
|
|---|
| 412 | ParameterType -> Internal,
|
|---|
| 413 | Value -> Sqrt[2] Sqrt[lam] vev,
|
|---|
| 414 | TeX -> \[Mu],
|
|---|
| 415 | Description -> "Coefficient of the quadratic piece of the Higgs potential"
|
|---|
| 416 | },
|
|---|
| 417 | yl == {
|
|---|
| 418 | ParameterType -> Internal,
|
|---|
| 419 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 420 | Definitions -> {yl[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 421 | Value -> {
|
|---|
| 422 | yl[1, 1] -> yme / vev,
|
|---|
| 423 | yl[2, 2] -> ymm / vev,
|
|---|
| 424 | yl[3, 3] -> ymtau / vev
|
|---|
| 425 | },
|
|---|
| 426 | InteractionOrder -> {QED, 1},
|
|---|
| 427 | ParameterName -> {
|
|---|
| 428 | yl[1, 1] -> ye,
|
|---|
| 429 | yl[2, 2] -> ym,
|
|---|
| 430 | yl[3, 3] -> ytau
|
|---|
| 431 | },
|
|---|
| 432 | TeX -> Superscript[y, l],
|
|---|
| 433 | Description -> "Lepton Yukawa couplings"
|
|---|
| 434 | },
|
|---|
| 435 | yu == {
|
|---|
| 436 | ParameterType -> Internal,
|
|---|
| 437 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 438 | Definitions -> {yu[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 439 | Value -> {
|
|---|
| 440 | yu[1, 1] -> ymup / vev,
|
|---|
| 441 | yu[2, 2] -> ymc / vev,
|
|---|
| 442 | yu[3, 3] -> ymt / vev
|
|---|
| 443 | },
|
|---|
| 444 | InteractionOrder -> {QED, 1},
|
|---|
| 445 | ParameterName -> {
|
|---|
| 446 | yu[1, 1] -> yup,
|
|---|
| 447 | yu[2, 2] -> yc,
|
|---|
| 448 | yu[3, 3] -> yt
|
|---|
| 449 | },
|
|---|
| 450 | TeX -> Superscript[y, u],
|
|---|
| 451 | Description -> "Up-type Yukawa couplings"
|
|---|
| 452 | },
|
|---|
| 453 | yd == {
|
|---|
| 454 | ParameterType -> Internal,
|
|---|
| 455 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 456 | Definitions -> {yd[i_?NumericQ, j_?NumericQ] :> 0 /; (i =!= j)},
|
|---|
| 457 | Value -> {
|
|---|
| 458 | yd[1, 1] -> ymdo / vev,
|
|---|
| 459 | yd[2, 2] -> yms / vev,
|
|---|
| 460 | yd[3, 3] -> ymb / vev
|
|---|
| 461 | },
|
|---|
| 462 | InteractionOrder -> {QED, 1},
|
|---|
| 463 | ParameterName -> {
|
|---|
| 464 | yd[1, 1] -> ydo,
|
|---|
| 465 | yd[2, 2] -> ys,
|
|---|
| 466 | yd[3, 3] -> yb
|
|---|
| 467 | },
|
|---|
| 468 | TeX -> Superscript[y, d],
|
|---|
| 469 | Description -> "Down-type Yukawa couplings"
|
|---|
| 470 | },
|
|---|
| 471 | CKM == { (* N. B. : only Cabibbo mixing! *)
|
|---|
| 472 | ParameterType -> Internal,
|
|---|
| 473 | Indices -> {Index[Generation], Index[Generation]},
|
|---|
| 474 | Unitary -> True,
|
|---|
| 475 | Value -> {
|
|---|
| 476 | CKM[1, 1] -> Cos[cabi],
|
|---|
| 477 | CKM[1, 2] -> Sin[cabi],
|
|---|
| 478 | CKM[1, 3] -> 0,
|
|---|
| 479 | CKM[2, 1] -> -Sin[cabi],
|
|---|
| 480 | CKM[2, 2] -> Cos[cabi],
|
|---|
| 481 | CKM[2, 3] -> 0,
|
|---|
| 482 | CKM[3, 1] -> 0,
|
|---|
| 483 | CKM[3, 2] -> 0,
|
|---|
| 484 | CKM[3, 3] -> 1
|
|---|
| 485 | },
|
|---|
| 486 | TeX -> Superscript[V, CKM],
|
|---|
| 487 | Description -> "CKM-Matrix"
|
|---|
| 488 | }
|
|---|
| 489 | };
|
|---|
| 490 |
|
|---|
| 491 | (* Particle classes *)
|
|---|
| 492 |
|
|---|
| 493 | M$ClassesDescription = {
|
|---|
| 494 |
|
|---|
| 495 | (* Gauge bosons: physical vector fields *)
|
|---|
| 496 |
|
|---|
| 497 | V[1] == {
|
|---|
| 498 | ClassName -> A,
|
|---|
| 499 | SelfConjugate -> True,
|
|---|
| 500 | Mass -> 0,
|
|---|
| 501 | Width -> 0,
|
|---|
| 502 | ParticleName -> "a",
|
|---|
| 503 | PDG -> 22,
|
|---|
| 504 | PropagatorLabel -> "a",
|
|---|
| 505 | PropagatorType -> W,
|
|---|
| 506 | PropagatorArrow -> None,
|
|---|
| 507 | FullName -> "Photon"
|
|---|
| 508 | },
|
|---|
| 509 | V[2] == {
|
|---|
| 510 | ClassName -> Z,
|
|---|
| 511 | SelfConjugate -> True,
|
|---|
| 512 | Mass -> {mZ, 91.1876},
|
|---|
| 513 | Width -> {WZ, 2.4952},
|
|---|
| 514 | ParticleName -> "Z",
|
|---|
| 515 | PDG -> 23,
|
|---|
| 516 | PropagatorLabel -> "Z",
|
|---|
| 517 | PropagatorType -> Sine,
|
|---|
| 518 | PropagatorArrow -> None,
|
|---|
| 519 | FullName -> "Z"
|
|---|
| 520 | },
|
|---|
| 521 | V[3] == {
|
|---|
| 522 | ClassName -> W,
|
|---|
| 523 | SelfConjugate -> False,
|
|---|
| 524 | Mass -> {mW, Internal},
|
|---|
| 525 | Width -> {WW, 2.085},
|
|---|
| 526 | ParticleName -> "W+",
|
|---|
| 527 | AntiParticleName -> "W-",
|
|---|
| 528 | QuantumNumbers -> {Q -> 1},
|
|---|
| 529 | PDG -> 24,
|
|---|
| 530 | PropagatorLabel -> "W",
|
|---|
| 531 | PropagatorType -> Sine,
|
|---|
| 532 | PropagatorArrow -> Forward,
|
|---|
| 533 | FullName -> "W"
|
|---|
| 534 | },
|
|---|
| 535 | V[4] == {
|
|---|
| 536 | ClassName -> G,
|
|---|
| 537 | SelfConjugate -> True,
|
|---|
| 538 | Indices -> {Index[Gluon]},
|
|---|
| 539 | Mass -> 0,
|
|---|
| 540 | Width -> 0,
|
|---|
| 541 | ParticleName -> "g",
|
|---|
| 542 | PDG -> 21,
|
|---|
| 543 | PropagatorLabel -> "G",
|
|---|
| 544 | PropagatorType -> C,
|
|---|
| 545 | PropagatorArrow -> None,
|
|---|
| 546 | FullName -> "G"
|
|---|
| 547 | },
|
|---|
| 548 |
|
|---|
| 549 | (* Ghosts: related to physical gauge bosons *)
|
|---|
| 550 |
|
|---|
| 551 | U[1] == {
|
|---|
| 552 | ClassName -> ghA,
|
|---|
| 553 | SelfConjugate -> False,
|
|---|
| 554 | Ghost -> A,
|
|---|
| 555 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 556 | Mass -> 0,
|
|---|
| 557 | Width -> 0,
|
|---|
| 558 | PropagatorLabel -> "uA",
|
|---|
| 559 | PropagatorType -> GhostDash,
|
|---|
| 560 | PropagatorArrow -> Forward
|
|---|
| 561 | },
|
|---|
| 562 | U[2] == {
|
|---|
| 563 | ClassName -> ghZ,
|
|---|
| 564 | SelfConjugate -> False,
|
|---|
| 565 | Ghost -> Z,
|
|---|
| 566 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 567 | Mass -> {mZ, 91.1876},
|
|---|
| 568 | Width -> {WZ, 2.4952},
|
|---|
| 569 | PropagatorLabel -> "uZ",
|
|---|
| 570 | PropagatorType -> GhostDash,
|
|---|
| 571 | PropagatorArrow -> Forward
|
|---|
| 572 | },
|
|---|
| 573 | U[31] == {
|
|---|
| 574 | ClassName -> ghWp,
|
|---|
| 575 | SelfConjugate -> False,
|
|---|
| 576 | Ghost -> W,
|
|---|
| 577 | QuantumNumbers -> {GhostNumber -> 1, Q -> 1},
|
|---|
| 578 | Mass -> {mW, Internal},
|
|---|
| 579 | Width -> {WW, 2.085},
|
|---|
| 580 | PropagatorLabel -> "uWp",
|
|---|
| 581 | PropagatorType -> GhostDash,
|
|---|
| 582 | PropagatorArrow -> Forward
|
|---|
| 583 | },
|
|---|
| 584 | U[32] == {
|
|---|
| 585 | ClassName -> ghWm,
|
|---|
| 586 | SelfConjugate -> False,
|
|---|
| 587 | Ghost -> Wbar,
|
|---|
| 588 | QuantumNumbers -> {GhostNumber -> 1, Q -> -1},
|
|---|
| 589 | Mass -> {mW, Internal},
|
|---|
| 590 | Width -> {WW, 2.085},
|
|---|
| 591 | PropagatorLabel -> "uWm",
|
|---|
| 592 | PropagatorType -> GhostDash,
|
|---|
| 593 | PropagatorArrow -> Forward
|
|---|
| 594 | },
|
|---|
| 595 | U[4] == {
|
|---|
| 596 | ClassName -> ghG,
|
|---|
| 597 | SelfConjugate -> False,
|
|---|
| 598 | Indices -> {Index[Gluon]},
|
|---|
| 599 | Ghost -> G,
|
|---|
| 600 | PDG -> 82,
|
|---|
| 601 | QuantumNumbers -> {GhostNumber -> 1},
|
|---|
| 602 | Mass -> 0,
|
|---|
| 603 | Width -> 0,
|
|---|
| 604 | PropagatorLabel -> "uG",
|
|---|
| 605 | PropagatorType -> GhostDash,
|
|---|
| 606 | PropagatorArrow -> Forward
|
|---|
| 607 | },
|
|---|
| 608 |
|
|---|
| 609 | (* Gauge bosons: unphysical vector fields *)
|
|---|
| 610 |
|
|---|
| 611 | V[11] == {
|
|---|
| 612 | ClassName -> B,
|
|---|
| 613 | Unphysical -> True,
|
|---|
| 614 | SelfConjugate -> True,
|
|---|
| 615 | Definitions -> {B[mu_] -> -sw Z[mu] + cw A[mu]}
|
|---|
| 616 | },
|
|---|
| 617 | V[12] == {
|
|---|
| 618 | ClassName -> Wi,
|
|---|
| 619 | Unphysical -> True,
|
|---|
| 620 | SelfConjugate -> True,
|
|---|
| 621 | Indices -> {Index[SU2W]},
|
|---|
| 622 | FlavorIndex -> SU2W,
|
|---|
| 623 | Definitions -> {
|
|---|
| 624 | Wi[mu_, 1] -> (Wbar[mu] + W[mu]) / Sqrt[2],
|
|---|
| 625 | Wi[mu_, 2] -> (Wbar[mu] - W[mu]) / (I * Sqrt[2]),
|
|---|
| 626 | Wi[mu_, 3] -> cw Z[mu] + sw A[mu]
|
|---|
| 627 | }
|
|---|
| 628 | },
|
|---|
| 629 |
|
|---|
| 630 | (* Ghosts: related to unphysical gauge bosons *)
|
|---|
| 631 |
|
|---|
| 632 | U[11] == {
|
|---|
| 633 | ClassName -> ghB,
|
|---|
| 634 | Unphysical -> True,
|
|---|
| 635 | SelfConjugate -> False,
|
|---|
| 636 | Ghost -> B,
|
|---|
| 637 | Definitions -> {ghB -> -sw ghZ + cw ghA}
|
|---|
| 638 | },
|
|---|
| 639 | U[12] == {
|
|---|
| 640 | ClassName -> ghWi,
|
|---|
| 641 | Unphysical -> True,
|
|---|
| 642 | SelfConjugate -> False,
|
|---|
| 643 | Ghost -> Wi,
|
|---|
| 644 | Indices -> {Index[SU2W]},
|
|---|
| 645 | FlavorIndex -> SU2W,
|
|---|
| 646 | Definitions -> {
|
|---|
| 647 | ghWi[1] -> (ghWp + ghWm) / Sqrt[2],
|
|---|
| 648 | ghWi[2] -> (ghWm - ghWp) / (I * Sqrt[2]),
|
|---|
| 649 | ghWi[3] -> cw ghZ + sw ghA
|
|---|
| 650 | }
|
|---|
| 651 | },
|
|---|
| 652 |
|
|---|
| 653 | (* Fermions: physical fields *)
|
|---|
| 654 |
|
|---|
| 655 | F[1] == {
|
|---|
| 656 | ClassName -> vl,
|
|---|
| 657 | ClassMembers -> {ve, vm, vt},
|
|---|
| 658 | Indices -> {Index[Generation]},
|
|---|
| 659 | FlavorIndex -> Generation,
|
|---|
| 660 | SelfConjugate -> False,
|
|---|
| 661 | Mass -> 0,
|
|---|
| 662 | Width -> 0,
|
|---|
| 663 | PropagatorLabel -> {"v", "ve", "vm", "vt"},
|
|---|
| 664 | PropagatorType -> S,
|
|---|
| 665 | PropagatorArrow -> Forward,
|
|---|
| 666 | PDG -> {12, 14, 16},
|
|---|
| 667 | ParticleName -> {"ve", "vm", "vt"},
|
|---|
| 668 | AntiParticleName -> {"ve~", "vm~", "vt~"},
|
|---|
| 669 | FullName -> {"Electron-neutrino", "Muon-neutrino", "Tau-neutrino"}
|
|---|
| 670 | },
|
|---|
| 671 | F[2] == {
|
|---|
| 672 | ClassName -> l,
|
|---|
| 673 | ClassMembers -> {e, mu, ta},
|
|---|
| 674 | Indices -> {Index[Generation]},
|
|---|
| 675 | FlavorIndex -> Generation,
|
|---|
| 676 | SelfConjugate -> False,
|
|---|
| 677 | Mass -> {Ml, {me, 5.11*^-4}, {mmu, 0.10566}, {mta, 1.777}},
|
|---|
| 678 | Width -> 0,
|
|---|
| 679 | QuantumNumbers -> {Q -> -1},
|
|---|
| 680 | PropagatorLabel -> {"l", "e", "mu", "ta"},
|
|---|
| 681 | PropagatorType -> Straight,
|
|---|
| 682 | PropagatorArrow -> Forward,
|
|---|
| 683 | PDG -> {11, 13, 15},
|
|---|
| 684 | ParticleName -> {"e-", "mu-", "ta-"},
|
|---|
| 685 | AntiParticleName -> {"e+", "mu+", "ta+"},
|
|---|
| 686 | FullName -> {"Electron", "Muon", "Tau"}
|
|---|
| 687 | },
|
|---|
| 688 | F[3] == {
|
|---|
| 689 | ClassName -> uq,
|
|---|
| 690 | ClassMembers -> {u, c, t},
|
|---|
| 691 | Indices -> {Index[Generation], Index[Colour]},
|
|---|
| 692 | FlavorIndex -> Generation,
|
|---|
| 693 | SelfConjugate -> False,
|
|---|
| 694 | Mass -> {Mu, {mup, 2.55*^-3}, {mc, 1.27}, {mt, 172}},
|
|---|
| 695 | Width -> {0, 0, {WT, 1.50833649}},
|
|---|
| 696 | QuantumNumbers -> {Q -> 2/3},
|
|---|
| 697 | PropagatorLabel -> {"uq", "u", "c", "t"},
|
|---|
| 698 | PropagatorType -> Straight,
|
|---|
| 699 | PropagatorArrow -> Forward,
|
|---|
| 700 | PDG -> {2, 4, 6},
|
|---|
| 701 | ParticleName -> {"u", "c", "t"},
|
|---|
| 702 | AntiParticleName -> {"u~", "c~", "t~"},
|
|---|
| 703 | FullName -> {"u-quark", "c-quark", "t-quark"}
|
|---|
| 704 | },
|
|---|
| 705 | F[4] == {
|
|---|
| 706 | ClassName -> dq,
|
|---|
| 707 | ClassMembers -> {d, s, b},
|
|---|
| 708 | Indices -> {Index[Generation], Index[Colour]},
|
|---|
| 709 | FlavorIndex -> Generation,
|
|---|
| 710 | SelfConjugate -> False,
|
|---|
| 711 | Mass -> {Md, {md, 5.04*^-3}, {ms, 0.101}, {mb, 4.7}},
|
|---|
| 712 | Width -> 0,
|
|---|
| 713 | QuantumNumbers -> {Q -> -1/3},
|
|---|
| 714 | PropagatorLabel -> {"dq", "d", "s", "b"},
|
|---|
| 715 | PropagatorType -> Straight,
|
|---|
| 716 | PropagatorArrow -> Forward,
|
|---|
| 717 | PDG -> {1, 3, 5},
|
|---|
| 718 | ParticleName -> {"d", "s", "b"},
|
|---|
| 719 | AntiParticleName -> {"d~", "s~", "b~"},
|
|---|
| 720 | FullName -> {"d-quark", "s-quark", "b-quark"}
|
|---|
| 721 | },
|
|---|
| 722 |
|
|---|
| 723 | (* Fermions: physical fields of the pSPSS *)
|
|---|
| 724 |
|
|---|
| 725 | F[5] == {
|
|---|
| 726 | ClassName -> n4,
|
|---|
| 727 | SelfConjugate -> True,
|
|---|
| 728 | Mass -> {mn4, Internal},
|
|---|
| 729 | Width -> {Wn4, 1*^-5},
|
|---|
| 730 | PropagatorLabel -> {"n4"},
|
|---|
| 731 | PropagatorType -> Straight,
|
|---|
| 732 | PropagatorArrow -> None,
|
|---|
| 733 | PDG -> 8000011,
|
|---|
| 734 | ParticleName -> {"n4"},
|
|---|
| 735 | FullName -> {"Heavy neutrino n4"}
|
|---|
| 736 | },
|
|---|
| 737 | F[6] == {
|
|---|
| 738 | ClassName -> n5,
|
|---|
| 739 | SelfConjugate -> True,
|
|---|
| 740 | Mass -> {mn5, Internal},
|
|---|
| 741 | Width -> {Wn5, 1*^-5},
|
|---|
| 742 | PropagatorLabel -> {"n5"},
|
|---|
| 743 | PropagatorType -> Straight,
|
|---|
| 744 | PropagatorArrow -> None,
|
|---|
| 745 | PDG -> 8000012,
|
|---|
| 746 | ParticleName -> {"n5"},
|
|---|
| 747 | FullName -> {"Heavy neutrino n5"}
|
|---|
| 748 | },
|
|---|
| 749 |
|
|---|
| 750 | (* Fermions: unphysical fields of the pSPSS *)
|
|---|
| 751 |
|
|---|
| 752 | F[8] == {
|
|---|
| 753 | ClassName -> nL,
|
|---|
| 754 | Unphysical -> True,
|
|---|
| 755 | Indices -> {Index[NeutrinoGeneration]},
|
|---|
| 756 | FlavorIndex -> NeutrinoGeneration,
|
|---|
| 757 | SelfConjugate -> False,
|
|---|
| 758 | Definitions -> {
|
|---|
| 759 | nL[sp1_, 1] :> vl[sp1, 1]*Sqrt[2],
|
|---|
| 760 | nL[sp1_, 2] :> vl[sp1, 2]*Sqrt[2],
|
|---|
| 761 | nL[sp1_, 3] :> vl[sp1, 3]*Sqrt[2],
|
|---|
| 762 | nL[sp1_, 4] :> n4[sp1],
|
|---|
| 763 | nL[sp1_, 5] :> n5[sp1]
|
|---|
| 764 | }
|
|---|
| 765 | },
|
|---|
| 766 | F[9] == {
|
|---|
| 767 | ClassName -> N1L,
|
|---|
| 768 | Unphysical -> True,
|
|---|
| 769 | SelfConjugate -> True,
|
|---|
| 770 | Definitions -> {
|
|---|
| 771 | N1L[sp1_] :> Module[{sp2, hh}, ProjM[sp1, sp2] Un[4, hh] nL[sp2, hh]]
|
|---|
| 772 | }
|
|---|
| 773 | },
|
|---|
| 774 | F[10] == {
|
|---|
| 775 | ClassName -> N2L,
|
|---|
| 776 | Unphysical -> True,
|
|---|
| 777 | SelfConjugate -> True,
|
|---|
| 778 | Definitions -> {
|
|---|
| 779 | N2L[sp1_] :> Module[{sp2, hh}, ProjM[sp1, sp2] Un[5, hh] nL[sp2, hh]]
|
|---|
| 780 | }
|
|---|
| 781 | },
|
|---|
| 782 | F[11] == {
|
|---|
| 783 | ClassName -> LL,
|
|---|
| 784 | Unphysical -> True,
|
|---|
| 785 | Indices -> {Index[SU2D], Index[Generation]},
|
|---|
| 786 | FlavorIndex -> SU2D,
|
|---|
| 787 | SelfConjugate -> False,
|
|---|
| 788 | QuantumNumbers -> {Y -> -1/2},
|
|---|
| 789 | Definitions -> {
|
|---|
| 790 | LL[sp1_, 1, ff_] :> Module[{sp2, hh}, ProjM[sp1, sp2] UnCL[ff, hh] nL[sp2, hh]],
|
|---|
| 791 | LL[sp1_, 2, ff_] :> Module[{sp2}, ProjM[sp1, sp2] l[sp2, ff]]
|
|---|
| 792 | }
|
|---|
| 793 | },
|
|---|
| 794 |
|
|---|
| 795 | (* Fermions: unphysical fields *)
|
|---|
| 796 |
|
|---|
| 797 | F[12] == {
|
|---|
| 798 | ClassName -> lR,
|
|---|
| 799 | Unphysical -> True,
|
|---|
| 800 | Indices -> {Index[Generation]},
|
|---|
| 801 | FlavorIndex -> Generation,
|
|---|
| 802 | SelfConjugate -> False,
|
|---|
| 803 | QuantumNumbers -> {Y -> -1},
|
|---|
| 804 | Definitions -> {
|
|---|
| 805 | lR[sp1_, ff_] :> Module[{sp2}, ProjP[sp1, sp2] l[sp2, ff]]
|
|---|
| 806 | }
|
|---|
| 807 | },
|
|---|
| 808 | F[13] == {
|
|---|
| 809 | ClassName -> QL,
|
|---|
| 810 | Unphysical -> True,
|
|---|
| 811 | Indices -> {Index[SU2D], Index[Generation], Index[Colour]},
|
|---|
| 812 | FlavorIndex -> SU2D,
|
|---|
| 813 | SelfConjugate -> False,
|
|---|
| 814 | QuantumNumbers -> {Y -> 1/6},
|
|---|
| 815 | Definitions -> {
|
|---|
| 816 | QL[sp1_, 1, ff_, cc_] :> Module[{sp2}, ProjM[sp1, sp2] uq[sp2, ff, cc]],
|
|---|
| 817 | QL[sp1_, 2, ff_, cc_] :> Module[{sp2, ff2}, CKM[ff, ff2] ProjM[sp1, sp2] dq[sp2, ff2, cc]] }
|
|---|
| 818 | },
|
|---|
| 819 | F[14] == {
|
|---|
| 820 | ClassName -> uR,
|
|---|
| 821 | Unphysical -> True,
|
|---|
| 822 | Indices -> {Index[Generation], Index[Colour]},
|
|---|
| 823 | FlavorIndex -> Generation,
|
|---|
| 824 | SelfConjugate -> False,
|
|---|
| 825 | QuantumNumbers -> {Y -> 2/3},
|
|---|
| 826 | Definitions -> {
|
|---|
| 827 | uR[sp1_, ff_, cc_] :> Module[{sp2}, ProjP[sp1, sp2] uq[sp2, ff, cc]]
|
|---|
| 828 | }
|
|---|
| 829 | },
|
|---|
| 830 | F[15] == {
|
|---|
| 831 | ClassName -> dR,
|
|---|
| 832 | Unphysical -> True,
|
|---|
| 833 | Indices -> {Index[Generation], Index[Colour]},
|
|---|
| 834 | FlavorIndex -> Generation,
|
|---|
| 835 | SelfConjugate -> False,
|
|---|
| 836 | QuantumNumbers -> {Y -> -1/3},
|
|---|
| 837 | Definitions -> {
|
|---|
| 838 | dR[sp1_, ff_, cc_] :> Module[{sp2}, ProjP[sp1, sp2] dq[sp2, ff, cc]]
|
|---|
| 839 | }
|
|---|
| 840 | },
|
|---|
| 841 |
|
|---|
| 842 | (* Higgs: physical scalars *)
|
|---|
| 843 |
|
|---|
| 844 | S[1] == {
|
|---|
| 845 | ClassName -> H,
|
|---|
| 846 | SelfConjugate -> True,
|
|---|
| 847 | Mass -> {MH, 125},
|
|---|
| 848 | Width -> {WH, 0.00407},
|
|---|
| 849 | PropagatorLabel -> "H",
|
|---|
| 850 | PropagatorType -> D,
|
|---|
| 851 | PropagatorArrow -> None,
|
|---|
| 852 | PDG -> 25,
|
|---|
| 853 | ParticleName -> "H",
|
|---|
| 854 | FullName -> "H"
|
|---|
| 855 | },
|
|---|
| 856 |
|
|---|
| 857 | (* Higgs: physical scalars *)
|
|---|
| 858 |
|
|---|
| 859 | S[2] == {
|
|---|
| 860 | ClassName -> G0,
|
|---|
| 861 | SelfConjugate -> True,
|
|---|
| 862 | Goldstone -> Z,
|
|---|
| 863 | Mass -> {mZ, 91.1876},
|
|---|
| 864 | Width -> {WZ, 2.4952},
|
|---|
| 865 | PropagatorLabel -> "Go",
|
|---|
| 866 | PropagatorType -> D,
|
|---|
| 867 | PropagatorArrow -> None,
|
|---|
| 868 | PDG -> 250,
|
|---|
| 869 | ParticleName -> "G0",
|
|---|
| 870 | FullName -> "G0"
|
|---|
| 871 | },
|
|---|
| 872 | S[3] == {
|
|---|
| 873 | ClassName -> GP,
|
|---|
| 874 | SelfConjugate -> False,
|
|---|
| 875 | Goldstone -> W,
|
|---|
| 876 | Mass -> {mW, Internal},
|
|---|
| 877 | QuantumNumbers -> {Q -> 1},
|
|---|
| 878 | Width -> {WW, 2.085},
|
|---|
| 879 | PropagatorLabel -> "GP",
|
|---|
| 880 | PropagatorType -> D,
|
|---|
| 881 | PropagatorArrow -> None,
|
|---|
| 882 | PDG -> 251,
|
|---|
| 883 | ParticleName -> "G+",
|
|---|
| 884 | AntiParticleName -> "G-",
|
|---|
| 885 | FullName -> "GP"
|
|---|
| 886 | },
|
|---|
| 887 |
|
|---|
| 888 | (* Higgs: unphysical scalars *)
|
|---|
| 889 |
|
|---|
| 890 | S[11] == {
|
|---|
| 891 | ClassName -> Phi,
|
|---|
| 892 | Unphysical -> True,
|
|---|
| 893 | Indices -> {Index[SU2D]},
|
|---|
| 894 | FlavorIndex -> SU2D,
|
|---|
| 895 | SelfConjugate -> False,
|
|---|
| 896 | QuantumNumbers -> {Y -> 1/2},
|
|---|
| 897 | Definitions -> {
|
|---|
| 898 | Phi[1] -> -I GP,
|
|---|
| 899 | Phi[2] -> vev + (H + I G0) / Sqrt[2]
|
|---|
| 900 | }
|
|---|
| 901 | },
|
|---|
| 902 |
|
|---|
| 903 | (* pSPSS Higgs necessary to get the correct interaction order for new Yukawas *)
|
|---|
| 904 |
|
|---|
| 905 | S[12] == {
|
|---|
| 906 | ClassName -> PhiNP,
|
|---|
| 907 | Unphysical -> True,
|
|---|
| 908 | Indices -> {Index[SU2D]},
|
|---|
| 909 | FlavorIndex -> SU2D,
|
|---|
| 910 | SelfConjugate -> False,
|
|---|
| 911 | QuantumNumbers -> {Y -> 1/2},
|
|---|
| 912 | Definitions -> {
|
|---|
| 913 | PhiNP[1] -> -I GP,
|
|---|
| 914 | PhiNP[2] -> vevNP + (H + I G0) / Sqrt[2]
|
|---|
| 915 | }
|
|---|
| 916 | }
|
|---|
| 917 | };
|
|---|
| 918 |
|
|---|
| 919 | (* Gauge Parameters (FeynArts) *)
|
|---|
| 920 |
|
|---|
| 921 | GaugeXi[V[1]] = GaugeXi[A];
|
|---|
| 922 | GaugeXi[V[2]] = GaugeXi[Z];
|
|---|
| 923 | GaugeXi[V[3]] = GaugeXi[W];
|
|---|
| 924 | GaugeXi[V[4]] = GaugeXi[G];
|
|---|
| 925 | GaugeXi[S[1]] = 1;
|
|---|
| 926 | GaugeXi[S[2]] = GaugeXi[Z];
|
|---|
| 927 | GaugeXi[S[3]] = GaugeXi[W];
|
|---|
| 928 | GaugeXi[U[1]] = GaugeXi[A];
|
|---|
| 929 | GaugeXi[U[2]] = GaugeXi[Z];
|
|---|
| 930 | GaugeXi[U[4]] = GaugeXi[G];
|
|---|
| 931 | GaugeXi[U[31]] = GaugeXi[W];
|
|---|
| 932 | GaugeXi[U[32]] = GaugeXi[W];
|
|---|
| 933 |
|
|---|
| 934 | (* Helper function *)
|
|---|
| 935 |
|
|---|
| 936 | RemoveHigherOrder[Lag_] := Block[{tmp, epsilon, x1, x2, x3},
|
|---|
| 937 | tmp = Lag // ExpandIndices // OptimizeIndex;
|
|---|
| 938 | tmp = Series[tmp /. {
|
|---|
| 939 | theta1 -> epsilon x1,
|
|---|
| 940 | theta2 -> epsilon x2,
|
|---|
| 941 | theta3 -> epsilon x3
|
|---|
| 942 | }, {epsilon, 0, 2}];
|
|---|
| 943 | tmp /. {
|
|---|
| 944 | x1 -> theta1 / epsilon,
|
|---|
| 945 | x2 -> theta2 / epsilon,
|
|---|
| 946 | x3 -> theta3 / epsilon
|
|---|
| 947 | } // Normal
|
|---|
| 948 | ];
|
|---|
| 949 |
|
|---|
| 950 | (* Lagrangian *)
|
|---|
| 951 |
|
|---|
| 952 | LGauge := Block[{mu, nu, ii, aa},
|
|---|
| 953 | - ExpandIndices[
|
|---|
| 954 | 1/4 FS[B, mu, nu] FS[B, mu, nu] +
|
|---|
| 955 | 1/4 FS[Wi, mu, nu, ii] FS[Wi, mu, nu, ii] +
|
|---|
| 956 | 1/4 FS[G, mu, nu, aa] FS[G, mu, nu, aa],
|
|---|
| 957 | FlavorExpand -> SU2W
|
|---|
| 958 | ]
|
|---|
| 959 | ];
|
|---|
| 960 |
|
|---|
| 961 | preLFermions := Block[{mu},
|
|---|
| 962 | I * ExpandIndices[
|
|---|
| 963 | QLbar.Ga[mu].DC[QL, mu] +
|
|---|
| 964 | LLbar.Ga[mu].DC[LL, mu] +
|
|---|
| 965 | N1Lbar.Ga[mu].del[N1L, mu] +
|
|---|
| 966 | N2Lbar.Ga[mu].del[N2L, mu] +
|
|---|
| 967 | uRbar.Ga[mu].DC[uR, mu] +
|
|---|
| 968 | dRbar.Ga[mu].DC[dR, mu] +
|
|---|
| 969 | lRbar.Ga[mu].DC[lR, mu],
|
|---|
| 970 | FlavorExpand -> {SU2W, SU2D, NeutrinoGeneration}
|
|---|
| 971 | ] /. {
|
|---|
| 972 | CKM[a_, b_] Conjugate[CKM[a_, c_]] -> IndexDelta[b, c],
|
|---|
| 973 | CKM[b_, a_] Conjugate[CKM[c_, a_]] -> IndexDelta[b, c]
|
|---|
| 974 | }
|
|---|
| 975 | ];
|
|---|
| 976 | LFermions := LFermions = RemoveHigherOrder[preLFermions];
|
|---|
| 977 |
|
|---|
| 978 | LHiggs := Block[{ii, mu, feynmangaugerules},
|
|---|
| 979 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar -> 0}, {}];
|
|---|
| 980 | ExpandIndices[
|
|---|
| 981 | DC[Phibar[ii], mu] DC[Phi[ii], mu] +
|
|---|
| 982 | muH^2 Phibar[ii] Phi[ii] -
|
|---|
| 983 | lam Phibar[ii] Phi[ii] Phibar[jj] Phi[jj],
|
|---|
| 984 | FlavorExpand -> {SU2D, SU2W}
|
|---|
| 985 | ] /. feynmangaugerules
|
|---|
| 986 | ];
|
|---|
| 987 |
|
|---|
| 988 | LYukawa := Block[{sp, ii, jj, cc, ff1, ff2, ff3, yuk, feynmangaugerules},
|
|---|
| 989 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar -> 0}, {}];
|
|---|
| 990 | yuk = - ExpandIndices[
|
|---|
| 991 | yd[ff2, ff3] CKM[ff1, ff2] QLbar[sp, ii, ff1, cc].dR [sp, ff3, cc] Phi[ii] +
|
|---|
| 992 | yl[ff1, ff3] LLbar[sp, ii, ff1].lR [sp, ff3] Phi[ii] +
|
|---|
| 993 | yu[ff1, ff2] QLbar[sp, ii, ff1, cc].uR [sp, ff2, cc] Phibar[jj] Eps[ii, jj],
|
|---|
| 994 | FlavorExpand -> SU2D
|
|---|
| 995 | ];
|
|---|
| 996 | yuk = yuk /. {
|
|---|
| 997 | CKM[a_, b_] Conjugate[CKM[a_, c_]] -> IndexDelta[b, c],
|
|---|
| 998 | CKM[b_, a_] Conjugate[CKM[c_, a_]] -> IndexDelta[b, c]
|
|---|
| 999 | };
|
|---|
| 1000 | yuk + HC[yuk] /. feynmangaugerules
|
|---|
| 1001 | ];
|
|---|
| 1002 |
|
|---|
| 1003 | preLNP := Block[{sp1, ff1, ii, jj, yuk, feynmangaugerules},
|
|---|
| 1004 | feynmangaugerules = If[Not[FeynmanGauge], {G0|GP|GPbar -> 0}, {}];
|
|---|
| 1005 | yuk = - ExpandIndices[
|
|---|
| 1006 | Mmaj CC[N1Lbar[sp1]].N2L[sp1] +
|
|---|
| 1007 | yvn[ff1] (CC[N1Lbar[sp1]].LL[sp1, ii, ff1] PhiNPbar[jj] Eps[ii, jj]),
|
|---|
| 1008 | FlavorExpand -> {SU2D, NeutrinoGeneration}
|
|---|
| 1009 | ];
|
|---|
| 1010 | yuk + HC[yuk] /. feynmangaugerules
|
|---|
| 1011 | ];
|
|---|
| 1012 | LNP := LNP = RemoveHigherOrder[preLNP];
|
|---|
| 1013 |
|
|---|
| 1014 | LGhost := Block[{LGh1, LGhw, LGhs, LGhphi, mu, generators, gh, ghbar, Vectorize, phi1, phi2, togoldstones, doublet, doublet0},
|
|---|
| 1015 | (* Pure gauge piece *)
|
|---|
| 1016 | LGh1 = - ghBbar.del[DC[ghB, mu], mu];
|
|---|
| 1017 | LGhw = - ghWibar[ii].del[DC[ghWi[ii], mu], mu];
|
|---|
| 1018 | LGhs = - ghGbar[ii].del[DC[ghG[ii], mu], mu];
|
|---|
| 1019 | (* Scalar pieces: see Peskin pages 739-742 *)
|
|---|
| 1020 | gh = {ghB, ghWi[1], ghWi[2], ghWi[3]};
|
|---|
| 1021 | ghbar = {ghBbar, ghWibar[1], ghWibar[2], ghWibar[3]};
|
|---|
| 1022 | generators = {
|
|---|
| 1023 | -I g1 IdentityMatrix[2] / 2,
|
|---|
| 1024 | -I gw PauliSigma[1] / 2,
|
|---|
| 1025 | -I gw PauliSigma[2] / 2,
|
|---|
| 1026 | -I gw PauliSigma[3] / 2
|
|---|
| 1027 | };
|
|---|
| 1028 | (* phi1 and phi2 are the real degrees of freedom of GP *)
|
|---|
| 1029 | doublet = Expand[{-(I phi1 + phi2) / Sqrt[2], Phi[2]} /. MR$Definitions /. vev -> 0];
|
|---|
| 1030 | doublet0 = {0, vev};
|
|---|
| 1031 | (* Vectorize transforms a doublet in a vector in the phi-basis, i.e. the basis of real degrees of freedom *)
|
|---|
| 1032 | Vectorize[{a_, b_}] := Simplify[{
|
|---|
| 1033 | Sqrt[2] Re[Expand[a]],
|
|---|
| 1034 | Sqrt[2] Im[Expand[a]],
|
|---|
| 1035 | Sqrt[2] Re[Expand[b]],
|
|---|
| 1036 | Sqrt[2] Im[Expand[b]]
|
|---|
| 1037 | } /. {Im[_] -> 0, Re[num_] -> num}];
|
|---|
| 1038 | togoldstones := {
|
|---|
| 1039 | phi1 -> (GPbar + GP) / Sqrt[2],
|
|---|
| 1040 | phi2 -> (GPbar - GP) / (I Sqrt[2])
|
|---|
| 1041 | };
|
|---|
| 1042 | LGhphi = Plus@@Flatten[Table[-ghbar[[kkk]].gh[[lll]] Vectorize[generators[[kkk]].doublet0].Vectorize[generators[[lll]].(doublet + doublet0)], {kkk, 4}, {lll, 4}]] /. togoldstones;
|
|---|
| 1043 | ExpandIndices[LGhs + If[FeynmanGauge, LGh1 + LGhw + LGhphi, 0], FlavorExpand -> SU2W]
|
|---|
| 1044 | ];
|
|---|
| 1045 |
|
|---|
| 1046 | LSM := LGauge + LFermions + LHiggs + LYukawa + LGhost; (* contains sterile neutrino kinetic terms *)
|
|---|
| 1047 | LpSPSS := LSM + LNP;
|
|---|