| 1 | (**********************************************************)
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| 2 | (* *)
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| 3 | (* Model for Chiral perturbation Theory at lowest order *)
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| 4 | (* *)
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| 5 | (**********************************************************)
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| 6 |
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| 7 | M$ModelName = "ChiPT";
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| 8 |
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| 9 | M$Information = {Authors -> {"C. Degrande"},
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| 10 | Date->"12/06/2009"
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| 11 | Institutions -> {"Universite catholique de Louvain (CP3)"},
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| 12 | Emails -> {"celine.degrande@uclouvain.be"},
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| 13 | Version -> 1,
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| 14 | URLs->"http://feynrules.phys.ucl.ac.be/view/Main/NLSM"
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| 15 | };
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| 16 |
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| 17 | (********** Index definition *********)
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| 18 |
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| 19 |
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| 20 | (***** Parameter list ******)
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| 21 |
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| 22 | M$Parameters = {
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| 23 | f == {ParameterType -> External,
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| 24 | Value->0.14,
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| 25 | Description->"decay constant"
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| 26 | },
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| 27 | b == {ParameterType -> External,
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| 28 | Value->1/6,
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| 29 | Description->"expansion parameter"
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| 30 | },
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| 31 | c == {ParameterType -> External,
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| 32 | Value->1/120,
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| 33 | Description->"expansion parameter"
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| 34 | },
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| 35 | r == {ParameterType -> External,
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| 36 | Description->"mass term coefficient"
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| 37 | },
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| 38 | m0 == {ParameterType -> External,
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| 39 | Value->0.8,
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| 40 | TeX -> Subscript[m, 0],
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| 41 | Description->"anomalous term coefficient"
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| 42 | },
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| 43 |
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| 44 | md == {ParameterType -> External,
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| 45 | Value->0.008,
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| 46 | TeX -> Subscript[m, d],
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| 47 | Description->"mass of the down quark"
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| 48 | },
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| 49 |
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| 50 | (*isospin limit : mup=md*)
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| 51 | mup == {ParameterType -> Internal, Value->md,
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| 52 | Value->0.004,
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| 53 | TeX -> Subscript[m, u],
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| 54 | Description->"mass of the up quark"
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| 55 | },
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| 56 | ms == {ParameterType -> External,
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| 57 | Value->0.125,
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| 58 | TeX -> Subscript[m, s],
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| 59 | Description->"mass of the strange quark"
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| 60 | },
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| 61 |
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| 62 | T == {ParameterType -> Internal,
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| 63 | Value->ArcTan[2 Sqrt[2]*r*(ms-md)/(r*(ms-md)-3m0^2)]/2,
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| 64 | TeX -> \[Theta],
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| 65 | Description->"mixing angle"
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| 66 | }
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| 67 | }
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| 68 |
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| 69 | (***** Gauge group list ******)
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| 70 |
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| 71 | M$GaugeGroups = {
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| 72 | }
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| 73 |
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| 74 | (***** Particle classes list ******)
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| 75 |
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| 76 | M$ClassesDescription = {S[1] == {ClassName -> pi0,
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| 77 | SelfConjugate -> True,
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| 78 | Mass->0.135,
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| 79 | Width->0
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| 80 | },
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| 81 |
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| 82 | S[2] == {ClassName -> pim,
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| 83 | SelfConjugate -> False,
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| 84 | Mass->0.14,
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| 85 | Width->0
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| 86 | },
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| 87 |
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| 88 | S[3] == {ClassName -> K0,
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| 89 | SelfConjugate -> False,
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| 90 | Mass->0.5,
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| 91 | Width->0
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| 92 | },
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| 93 |
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| 94 | S[4] == {ClassName -> Km,
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| 95 | SelfConjugate -> False,
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| 96 | Mass->0.5,
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| 97 | Width->0
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| 98 | },
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| 99 |
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| 100 | S[5] == {ClassName -> eta,
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| 101 | SelfConjugate -> True,
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| 102 | Mass->0.55,
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| 103 | Width->0
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| 104 | },
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| 105 |
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| 106 | S[6] == {ClassName -> etap,
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| 107 | SelfConjugate -> True,
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| 108 | Mass->0.96,
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| 109 | Width->0
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| 110 | }
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| 111 |
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| 112 | }
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| 113 |
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| 114 | pip = anti[pim];
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| 115 | pipbar=pim;
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| 116 |
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| 117 | Kp = anti[Km];
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| 118 | Kpbar = Km;
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| 119 |
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| 120 | (*matrix of the pseudo goldstone boson*)
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| 121 |
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| 122 | Pion = {{pi0 + (Cos[T] eta + Sin[T] etap)/Sqrt[3] + Sqrt[2/3] (-Sin[T] eta + Cos[T] etap),
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| 123 | Sqrt[2]*pip,
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| 124 | Sqrt[2]*Kp}, {Sqrt[2]*pim, -pi0 + (Cos[T] eta + Sin[T] etap)/Sqrt[3] +
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| 125 | Sqrt[2/3] (-Sin[T] eta + Cos[T] etap), Sqrt[2]*K0}, {Sqrt[2]*Km,
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| 126 | Sqrt[2]*K0bar, -2 (Cos[T] eta + Sin[T] etap)/Sqrt[3] +
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| 127 | Sqrt[2/3] (-Sin[T] eta + Cos[T] etap)}};
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| 128 |
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| 129 | (*mass matrix of the light quarks*)
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| 130 |
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| 131 | M = DiagonalMatrix[{mup, md, ms}];
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| 132 |
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| 133 | (*U developed at the pi^6*)
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| 134 |
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| 135 | U = IdentityMatrix[3] + I Sqrt[2] Pion/f - MatrixPower[Pion, 2]/f^2 -
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| 136 | 2 Sqrt[2] I b MatrixPower[Pion, 3]/f^3 +
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| 137 | 4 (b - 1/8) MatrixPower[Pion, 4]/f^4 + I 4 Sqrt[2]*c MatrixPower[Pion, 5]/f^5 - 8*(c+b^2/2-b/2+1/16) MatrixPower[Pion, 6]/f^6;
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| 138 | Ubar = IdentityMatrix[3] - I Sqrt[2] Pion/f - MatrixPower[Pion, 2]/f^2 +
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| 139 | 2 Sqrt[2] I b MatrixPower[Pion, 3]/f^3 +
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| 140 | 4 (b - 1/8) MatrixPower[Pion, 4]/f^4 - I 4 Sqrt[2]*c MatrixPower[Pion, 5]/f^5 - 8*(c+b^2/2-b/2+1/16) MatrixPower[Pion, 6]/f^6;
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| 141 |
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| 142 | (*U at the order pi^5 to speed up the compution of Lkin*)
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| 143 |
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| 144 | Uk = IdentityMatrix[3] + I Sqrt[2] Pion/f - MatrixPower[Pion, 2]/f^2 -
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| 145 | 2 Sqrt[2] I b MatrixPower[Pion, 3]/f^3 +
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| 146 | 4 (b - 1/8) MatrixPower[Pion, 4]/f^4 + I 4 Sqrt[2]*c MatrixPower[Pion, 5]/f^5;
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| 147 | Ukbar = IdentityMatrix[3] - I Sqrt[2] Pion/f - MatrixPower[Pion, 2]/f^2 +
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| 148 | 2 Sqrt[2] I b MatrixPower[Pion, 3]/f^3 +
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| 149 | 4 (b - 1/8) MatrixPower[Pion, 4]/f^4 - I 4 Sqrt[2]*c MatrixPower[Pion, 5]/f^5;
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| 150 |
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| 151 | (*Lagrangian*)
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| 152 |
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| 153 | Lkin := f^2/8 Tr[del[Uk,mu].del[Ukbar,mu]];
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| 154 | Lm := r*f^2/8 Tr[M.U+M.Ubar];
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| 155 | La := -f^2 m0^2/12 Tr[Pion/f-2 (b-1/6) MatrixPower[Pion, 3]/f^3 + 4 (c-b/2+3/40) MatrixPower[Pion, 5]/f^5]^2;
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| 156 |
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| 157 | L := Lkin+Lm+La;
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| 158 |
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