| 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | // ------------------------------------------------------------
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| 27 | // GEANT 4 class header file
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| 28 | //
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| 29 | // History:
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| 30 | // 17 August 2004 P.Gumplinger and T.MacPhail
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| 31 | // samples Michel spectrum including 1st order
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| 32 | // radiative corrections
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| 33 | // Reference: Florian Scheck "Muon Physics", in Physics Reports
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| 34 | // (Review Section of Physics Letters) 44, No. 4 (1978)
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| 35 | // 187-248. North-Holland Publishing Company, Amsterdam
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| 36 | // at page 210 cc.
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| 37 | //
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| 38 | // W.E. Fisher and F. Scheck, Nucl. Phys. B83 (1974) 25.
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| 39 | //
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| 40 | // ------------------------------------------------------------
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| 41 | //
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| 42 | #include "G4MuonDecayChannelWithSpin.hh"
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| 43 |
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| 44 | #include "Randomize.hh"
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| 45 |
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| 46 | #include "G4DecayProducts.hh"
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| 47 | #include "G4LorentzVector.hh"
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| 48 |
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| 49 | G4MuonDecayChannelWithSpin::G4MuonDecayChannelWithSpin(const G4String& theParentName,
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| 50 | G4double theBR)
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| 51 | : G4MuonDecayChannel(theParentName,theBR)
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| 52 | {
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| 53 | EMMU = 0.*MeV;
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| 54 | EMASS = 0.*MeV;
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| 55 | }
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| 56 |
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| 57 | G4MuonDecayChannelWithSpin::~G4MuonDecayChannelWithSpin()
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| 58 | {
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| 59 | }
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| 60 |
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| 61 | G4DecayProducts *G4MuonDecayChannelWithSpin::DecayIt(G4double)
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| 62 | {
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| 63 | // This version assumes V-A coupling with 1st order radiative correctons,
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| 64 | // the standard model Michel parameter values, but
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| 65 | // gives incorrect energy spectrum for neutrinos
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| 66 |
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| 67 | #ifdef G4VERBOSE
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| 68 | if (GetVerboseLevel()>1) G4cout << "G4MuonDecayChannelWithSpin::DecayIt ";
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| 69 | #endif
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| 70 |
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| 71 | if (parent == 0) FillParent();
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| 72 | if (daughters == 0) FillDaughters();
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| 73 |
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| 74 | // parent mass
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| 75 | G4double parentmass = parent->GetPDGMass();
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| 76 |
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| 77 | EMMU = parentmass;
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| 78 |
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| 79 | //daughters'mass
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| 80 | G4double daughtermass[3];
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| 81 | G4double sumofdaughtermass = 0.0;
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| 82 | for (G4int index=0; index<3; index++){
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| 83 | daughtermass[index] = daughters[index]->GetPDGMass();
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| 84 | sumofdaughtermass += daughtermass[index];
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| 85 | }
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| 86 |
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| 87 | EMASS = daughtermass[0];
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| 88 |
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| 89 | //create parent G4DynamicParticle at rest
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| 90 | G4ThreeVector dummy;
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| 91 | G4DynamicParticle * parentparticle = new G4DynamicParticle( parent, dummy, 0.0);
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| 92 | //create G4Decayproducts
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| 93 | G4DecayProducts *products = new G4DecayProducts(*parentparticle);
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| 94 | delete parentparticle;
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| 95 |
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| 96 | // calcurate electron energy
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| 97 |
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| 98 | G4double michel_rho = 0.75; //Standard Model Michel rho
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| 99 | G4double michel_delta = 0.75; //Standard Model Michel delta
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| 100 | G4double michel_xsi = 1.00; //Standard Model Michel xsi
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| 101 | G4double michel_eta = 0.00; //Standard Model eta
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| 102 |
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| 103 | G4double rndm, x, ctheta;
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| 104 |
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| 105 | G4double FG;
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| 106 | G4double FG_max = 2.00;
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| 107 |
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| 108 | G4double W_mue = (EMMU*EMMU+EMASS*EMASS)/(2.*EMMU);
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| 109 | G4double x0 = EMASS/W_mue;
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| 110 |
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| 111 | G4double x0_squared = x0*x0;
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| 112 |
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| 113 | // ***************************************************
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| 114 | // x0 <= x <= 1. and -1 <= y <= 1
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| 115 | //
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| 116 | // F(x,y) = f(x)*g(x,y); g(x,y) = 1.+g(x)*y
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| 117 | // ***************************************************
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| 118 |
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| 119 | // ***** sampling F(x,y) directly (brute force) *****
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| 120 |
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| 121 | do{
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| 122 |
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| 123 | // Sample the positron energy by sampling from F
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| 124 |
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| 125 | rndm = G4UniformRand();
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| 126 |
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| 127 | x = x0 + rndm*(1.-x0);
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| 128 |
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| 129 | G4double x_squared = x*x;
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| 130 |
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| 131 | G4double F_IS, F_AS, G_IS, G_AS;
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| 132 |
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| 133 | F_IS = 1./6.*(-2.*x_squared+3.*x-x0_squared);
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| 134 | F_AS = 1./6.*std::sqrt(x_squared-x0_squared)*(2.*x-2.+std::sqrt(1.-x0_squared));
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| 135 |
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| 136 | G_IS = 2./9.*(michel_rho-0.75)*(4.*x_squared-3.*x-x0_squared);
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| 137 | G_IS = G_IS + michel_eta*(1.-x)*x0;
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| 138 |
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| 139 | G_AS = 3.*(michel_xsi-1.)*(1.-x);
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| 140 | G_AS = G_AS+2.*(michel_xsi*michel_delta-0.75)*(4.*x-4.+std::sqrt(1.-x0_squared));
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| 141 | G_AS = 1./9.*std::sqrt(x_squared-x0_squared)*G_AS;
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| 142 |
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| 143 | F_IS = F_IS + G_IS;
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| 144 | F_AS = F_AS + G_AS;
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| 145 |
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| 146 | // *** Radiative Corrections ***
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| 147 |
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| 148 | G4double R_IS = F_c(x,x0);
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| 149 |
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| 150 | G4double F = 6.*F_IS + R_IS/std::sqrt(x_squared-x0_squared);
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| 151 |
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| 152 | // *** Radiative Corrections ***
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| 153 |
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| 154 | G4double R_AS = F_theta(x,x0);
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| 155 |
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| 156 | rndm = G4UniformRand();
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| 157 |
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| 158 | ctheta = 2.*rndm-1.;
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| 159 |
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| 160 | G4double G = 6.*F_AS - R_AS/std::sqrt(x_squared-x0_squared);
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| 161 |
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| 162 | FG = std::sqrt(x_squared-x0_squared)*F*(1.+(G/F)*ctheta);
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| 163 |
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| 164 | if(FG>FG_max){
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| 165 | G4cout<<"***Problem in Muon Decay *** : FG > FG_max"<<G4endl;
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| 166 | FG_max = FG;
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| 167 | }
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| 168 |
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| 169 | rndm = G4UniformRand();
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| 170 |
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| 171 | }while(FG<rndm*FG_max);
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| 172 |
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| 173 | G4double energy = x * W_mue;
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| 174 |
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| 175 | rndm = G4UniformRand();
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| 176 |
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| 177 | G4double phi = twopi * rndm;
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| 178 |
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| 179 | if(energy < EMASS) energy = EMASS;
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| 180 |
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| 181 | // calculate daughter momentum
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| 182 | G4double daughtermomentum[3];
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| 183 |
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| 184 | daughtermomentum[0] = std::sqrt(energy*energy - EMASS*EMASS);
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| 185 |
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| 186 | G4double stheta = std::sqrt(1.-ctheta*ctheta);
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| 187 | G4double cphi = std::cos(phi);
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| 188 | G4double sphi = std::sin(phi);
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| 189 |
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| 190 | //Coordinates of the decay positron with respect to the muon spin
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| 191 |
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| 192 | G4double px = stheta*cphi;
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| 193 | G4double py = stheta*sphi;
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| 194 | G4double pz = ctheta;
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| 195 |
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| 196 | G4ThreeVector direction0(px,py,pz);
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| 197 |
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| 198 | direction0.rotateUz(parent_polarization);
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| 199 |
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| 200 | G4DynamicParticle * daughterparticle0
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| 201 | = new G4DynamicParticle( daughters[0], daughtermomentum[0]*direction0);
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| 202 |
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| 203 | products->PushProducts(daughterparticle0);
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| 204 |
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| 205 |
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| 206 | // daughter 1 ,2 (neutrinos)
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| 207 | // create neutrinos in the C.M frame of two neutrinos
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| 208 | G4double energy2 = parentmass*(1.0 - x/2.0);
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| 209 | G4double vmass = std::sqrt((energy2-daughtermomentum[0])*(energy2+daughtermomentum[0]));
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| 210 | G4double beta = -1.0*daughtermomentum[0]/energy2;
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| 211 | G4double costhetan = 2.*G4UniformRand()-1.0;
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| 212 | G4double sinthetan = std::sqrt((1.0-costhetan)*(1.0+costhetan));
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| 213 | G4double phin = twopi*G4UniformRand()*rad;
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| 214 | G4double sinphin = std::sin(phin);
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| 215 | G4double cosphin = std::cos(phin);
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| 216 |
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| 217 | G4ThreeVector direction1(sinthetan*cosphin,sinthetan*sinphin,costhetan);
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| 218 | G4DynamicParticle * daughterparticle1
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| 219 | = new G4DynamicParticle( daughters[1], direction1*(vmass/2.));
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| 220 | G4DynamicParticle * daughterparticle2
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| 221 | = new G4DynamicParticle( daughters[2], direction1*(-1.0*vmass/2.));
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| 222 |
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| 223 | // boost to the muon rest frame
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| 224 | G4LorentzVector p4;
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| 225 | p4 = daughterparticle1->Get4Momentum();
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| 226 | p4.boost( direction0.x()*beta, direction0.y()*beta, direction0.z()*beta);
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| 227 | daughterparticle1->Set4Momentum(p4);
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| 228 | p4 = daughterparticle2->Get4Momentum();
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| 229 | p4.boost( direction0.x()*beta, direction0.y()*beta, direction0.z()*beta);
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| 230 | daughterparticle2->Set4Momentum(p4);
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| 231 | products->PushProducts(daughterparticle1);
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| 232 | products->PushProducts(daughterparticle2);
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| 233 | daughtermomentum[1] = daughterparticle1->GetTotalMomentum();
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| 234 | daughtermomentum[2] = daughterparticle2->GetTotalMomentum();
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| 235 |
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| 236 | // output message
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| 237 | #ifdef G4VERBOSE
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| 238 | if (GetVerboseLevel()>1) {
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| 239 | G4cout << "G4MuonDecayChannelWithSpin::DecayIt ";
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| 240 | G4cout << " create decay products in rest frame " <<G4endl;
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| 241 | products->DumpInfo();
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| 242 | }
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| 243 | #endif
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| 244 | return products;
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| 245 | }
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| 246 |
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| 247 | G4double G4MuonDecayChannelWithSpin::R_c(G4double x){
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| 248 |
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| 249 | G4int n_max = (int)(100.*x);
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| 250 |
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| 251 | if(n_max<10)n_max=10;
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| 252 |
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| 253 | G4double L2 = 0.0;
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| 254 |
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| 255 | for(G4int n=1; n<=n_max; n++){
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| 256 | L2 += std::pow(x,n)/(n*n);
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| 257 | }
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| 258 |
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| 259 | G4double omega = std::log(EMMU/EMASS);
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| 260 |
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| 261 | G4double r_c;
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| 262 |
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| 263 | r_c = 2.*L2-(pi*pi/3.)-2.;
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| 264 | r_c = r_c + omega * (1.5+2.*std::log((1.-x)/x));
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| 265 | r_c = r_c - std::log(x)*(2.*std::log(x)-1.);
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| 266 | r_c = r_c + (3.*std::log(x)-1.-1./x)*std::log(1.-x);
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| 267 |
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| 268 | return r_c;
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| 269 | }
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