| 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 | // -------------------------------------------------------------------
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| 28 | // GEANT4 Class file
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| 29 | //
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| 30 | // For information related to this code contact:
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| 31 | //
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| 32 | // File name: G4VXResonance
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| 33 | //
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| 34 | // Author:
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| 35 | //
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| 36 | // Creation date: 15 April 1999
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| 37 | //
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| 38 | // Modifications:
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| 39 | //
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| 40 | // -------------------------------------------------------------------
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| 41 |
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| 42 | #include "globals.hh"
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| 43 | #include "G4ios.hh"
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| 44 | #include "G4KineticTrack.hh"
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| 45 | #include "G4VXResonance.hh"
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| 46 | #include "Randomize.hh"
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| 47 | #include "G4Proton.hh"
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| 48 | #include "G4HadTmpUtil.hh"
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| 49 |
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| 50 | G4VXResonance::G4VXResonance()
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| 51 | { }
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| 52 |
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| 53 |
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| 54 | G4VXResonance::~G4VXResonance()
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| 55 | { }
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| 56 |
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| 57 |
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| 58 | G4bool G4VXResonance::operator==(const G4VXResonance &right) const
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| 59 | {
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| 60 | return (this == (G4VXResonance *) &right);
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| 61 | }
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| 62 |
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| 63 |
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| 64 | G4bool G4VXResonance::operator!=(const G4VXResonance &right) const
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| 65 | {
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| 66 | return (this != (G4VXResonance *) &right);
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| 67 | }
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| 68 |
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| 69 |
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| 70 | G4double G4VXResonance::IsospinCorrection(const G4KineticTrack& trk1,
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| 71 | const G4KineticTrack& trk2,
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| 72 | G4int isoOut1, G4int isoOut2,
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| 73 | G4double /*iSpinOut1*/, G4double /*iSpinOut2*/) const
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| 74 | {
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| 75 | G4double result = 0.;
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| 76 |
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| 77 | G4ParticleDefinition* in1 = trk1.GetDefinition();
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| 78 | G4ParticleDefinition* in2 = trk2.GetDefinition();
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| 79 |
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| 80 | G4int isoIn1 = in1->GetPDGiIsospin();
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| 81 | G4int iso3In1 = in1->GetPDGiIsospin3();
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| 82 | G4int isoIn2 = in2->GetPDGiIsospin();
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| 83 | G4int iso3In2 = in2->GetPDGiIsospin3();
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| 84 |
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| 85 | G4int isoProton = G4Proton::ProtonDefinition()->GetPDGiIsospin();
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| 86 | G4int iso3Proton = G4Proton::ProtonDefinition()->GetPDGiIsospin3();
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| 87 |
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| 88 | G4double pWeight = clebsch.Weight(isoProton,iso3Proton, isoProton,iso3Proton, isoOut1,isoOut2);
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| 89 | if (pWeight == 0.) throw G4HadronicException(__FILE__, __LINE__, "G4VXResonance::IsospinCorrection, no resonances - pWeight is zero");
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| 90 |
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| 91 | if (in1->IsShortLived() || in2->IsShortLived())
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| 92 | {
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| 93 | // Resonances in the initial state
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| 94 | G4int iSpinProton = G4Proton::ProtonDefinition()->GetPDGiSpin();
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| 95 | G4double degeneracyFactor = DegeneracyFactor(trk1,trk2,iSpinProton,iSpinProton);
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| 96 |
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| 97 | G4double factor = degeneracyFactor * pWeight;
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| 98 | if (factor > DBL_MIN)
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| 99 | {
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| 100 | // Randomly select the Isospin3 of the initial state resonances
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| 101 | std::vector<G4double> iso = clebsch.GenerateIso3(isoIn1,iso3In1,
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| 102 | isoIn2,iso3In2,
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| 103 | isoProton,isoProton);
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| 104 | G4int isoA = G4lrint(iso[0]);
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| 105 | G4int isoB = G4lrint(iso[1]);
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| 106 | G4double rWeight = clebsch.Weight(isoProton,isoA,
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| 107 | isoProton,isoB,
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| 108 | isoOut1,isoOut2);
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| 109 | result = rWeight / pWeight;
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| 110 | }
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| 111 | }
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| 112 | else
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| 113 | {
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| 114 | G4double weight = clebsch.Weight(isoIn1,iso3In1, isoIn2,iso3In2, isoOut1,isoOut2);
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| 115 | result = weight / pWeight;
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| 116 | }
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| 117 |
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| 118 | return result;
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| 119 | }
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| 120 |
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| 121 |
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| 122 | #include "G4DetailedBalancePhaseSpaceIntegral.hh"
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| 123 |
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| 124 | G4double G4VXResonance::DetailedBalance(const G4KineticTrack& trk1,
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| 125 | const G4KineticTrack& trk2,
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| 126 | G4int isoOut1, G4int isoOut2,
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| 127 | G4double iSpinOut1, G4double iSpinOut2,
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| 128 | G4double mOut1, G4double mOut2) const
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| 129 | {
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| 130 | // To handle the cases when resonances are involved the modified
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| 131 | // detailed balance of P. Danielewicz and G.F. Bertsch, Nucl. Phys. A533(1991) 712
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| 132 | // is used; in other words, the width of the resonances are folded to get the
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| 133 | // mean square of the final state momentum.
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| 134 |
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| 135 | G4ParticleDefinition* in1 = trk1.GetDefinition();
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| 136 | G4ParticleDefinition* in2 = trk2.GetDefinition();
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| 137 | if(in1->IsShortLived() && in2->IsShortLived())
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| 138 | {
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| 139 | throw G4HadronicException(__FILE__, __LINE__, "Detailed balance for resonance scattering still on the schedule.");
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| 140 | }
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| 141 |
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| 142 | G4double result = 0.;
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| 143 |
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| 144 | G4int isoIn1 = in1->GetPDGiIsospin();
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| 145 | G4int iso3In1 = in1->GetPDGiIsospin3();
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| 146 | G4int isoIn2 = in2->GetPDGiIsospin();
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| 147 | G4int iso3In2 = in2->GetPDGiIsospin3();
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| 148 | G4double weight = clebsch.Weight(isoIn1, iso3In1, isoIn2, iso3In2, isoOut1, isoOut2);
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| 149 |
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| 150 | if (weight > 00001)
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| 151 | {
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| 152 | // adding spin counting here ...... does not look quite consistent, but is correct anyway.
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| 153 | // revisit in the next design iteration @@
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| 154 | G4double degeneracy = DegeneracyFactor(trk1,trk2,iSpinOut1,iSpinOut2);
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| 155 | G4double factor = degeneracy * weight;
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| 156 |
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| 157 | // now the phase-space
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| 158 | G4double s = (trk1.Get4Momentum() + trk2.Get4Momentum()).mag2();
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| 159 | G4double m1 = in1->GetPDGMass();
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| 160 | G4double m2 = in2->GetPDGMass();
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| 161 |
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| 162 | // on-shell
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| 163 | G4double pinitial2 = (s - (m1+m2) * (m1+m2)) * (s - (m1-m2) * (m1-m2)) / (4.0*s);
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| 164 | G4double pfinal2 = (s - (mOut1+mOut2) * (mOut1+mOut2)) * (s - ( mOut1-mOut2) * (mOut1-mOut2)) / (4.0*s);
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| 165 | G4double relativeMomsquared = pfinal2/pinitial2;
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| 166 |
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| 167 | // resonance-nucleon scattering - inverse channel
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| 168 | if(in1->IsShortLived())
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| 169 | {
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| 170 | G4DetailedBalancePhaseSpaceIntegral theI(in1);
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| 171 | relativeMomsquared = 1./theI.GetPhaseSpaceIntegral(std::sqrt(s));
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| 172 | }
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| 173 | else if(in2->IsShortLived())
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| 174 | {
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| 175 | G4DetailedBalancePhaseSpaceIntegral theI(in2);
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| 176 | relativeMomsquared = 1./theI.GetPhaseSpaceIntegral(std::sqrt(s));
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| 177 | }
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| 178 |
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| 179 | result = factor * relativeMomsquared;
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| 180 | }
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| 181 |
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| 182 | return result;
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| 183 | }
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| 184 |
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| 185 |
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| 186 | G4double G4VXResonance::DegeneracyFactor(const G4KineticTrack& trk1,
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| 187 | const G4KineticTrack& trk2,
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| 188 | G4double iSpinOut1, G4double iSpinOut2) const
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| 189 | {
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| 190 | G4double value = 0.;
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| 191 |
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| 192 | G4ParticleDefinition* in1 = trk1.GetDefinition();
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| 193 | G4ParticleDefinition* in2 = trk2.GetDefinition();
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| 194 |
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| 195 | G4double sIn1 = in1->GetPDGiSpin() + 1.;
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| 196 | G4double sIn2 = in2->GetPDGiSpin() + 1.;
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| 197 |
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| 198 | G4double denom = sIn1 * sIn2;
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| 199 | if (denom > 0.)
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| 200 | {
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| 201 | value = (iSpinOut1+1) * (iSpinOut2+1) / denom;
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| 202 | }
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| 203 | return value;
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| 204 | }
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| 205 |
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| 206 |
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