| 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 | // $Id: G4RPGSigmaMinusInelastic.cc,v 1.1 2007/07/18 21:04:21 dennis Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 28 | //
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| 29 |
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| 30 | #include "G4RPGSigmaMinusInelastic.hh"
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| 31 | #include "Randomize.hh"
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| 32 |
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| 33 | G4HadFinalState*
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| 34 | G4RPGSigmaMinusInelastic::ApplyYourself( const G4HadProjectile &aTrack,
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| 35 | G4Nucleus &targetNucleus )
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| 36 | {
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| 37 | const G4HadProjectile *originalIncident = &aTrack;
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| 38 | if (originalIncident->GetKineticEnergy()<= 0.1*MeV)
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| 39 | {
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| 40 | theParticleChange.SetStatusChange(isAlive);
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| 41 | theParticleChange.SetEnergyChange(aTrack.GetKineticEnergy());
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| 42 | theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
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| 43 | return &theParticleChange;
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| 44 | }
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| 45 |
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| 46 | // create the target particle
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| 47 |
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| 48 | G4DynamicParticle *originalTarget = targetNucleus.ReturnTargetParticle();
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| 49 |
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| 50 | if( verboseLevel > 1 )
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| 51 | {
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| 52 | const G4Material *targetMaterial = aTrack.GetMaterial();
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| 53 | G4cout << "G4RPGSigmaMinusInelastic::ApplyYourself called" << G4endl;
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| 54 | G4cout << "kinetic energy = " << originalIncident->GetKineticEnergy()/MeV << "MeV, ";
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| 55 | G4cout << "target material = " << targetMaterial->GetName() << ", ";
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| 56 | G4cout << "target particle = " << originalTarget->GetDefinition()->GetParticleName()
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| 57 | << G4endl;
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| 58 | }
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| 59 |
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| 60 | // Fermi motion and evaporation
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| 61 | // As of Geant3, the Fermi energy calculation had not been Done
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| 62 |
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| 63 | G4double ek = originalIncident->GetKineticEnergy()/MeV;
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| 64 | G4double amas = originalIncident->GetDefinition()->GetPDGMass()/MeV;
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| 65 | G4ReactionProduct modifiedOriginal;
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| 66 | modifiedOriginal = *originalIncident;
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| 67 |
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| 68 | G4double tkin = targetNucleus.Cinema( ek );
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| 69 | ek += tkin;
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| 70 | modifiedOriginal.SetKineticEnergy( ek*MeV );
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| 71 | G4double et = ek + amas;
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| 72 | G4double p = std::sqrt( std::abs((et-amas)*(et+amas)) );
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| 73 | G4double pp = modifiedOriginal.GetMomentum().mag()/MeV;
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| 74 | if( pp > 0.0 )
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| 75 | {
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| 76 | G4ThreeVector momentum = modifiedOriginal.GetMomentum();
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| 77 | modifiedOriginal.SetMomentum( momentum * (p/pp) );
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| 78 | }
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| 79 | //
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| 80 | // calculate black track energies
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| 81 | //
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| 82 | tkin = targetNucleus.EvaporationEffects( ek );
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| 83 | ek -= tkin;
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| 84 | modifiedOriginal.SetKineticEnergy( ek*MeV );
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| 85 | et = ek + amas;
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| 86 | p = std::sqrt( std::abs((et-amas)*(et+amas)) );
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| 87 | pp = modifiedOriginal.GetMomentum().mag()/MeV;
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| 88 | if( pp > 0.0 )
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| 89 | {
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| 90 | G4ThreeVector momentum = modifiedOriginal.GetMomentum();
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| 91 | modifiedOriginal.SetMomentum( momentum * (p/pp) );
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| 92 | }
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| 93 | G4ReactionProduct currentParticle = modifiedOriginal;
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| 94 | G4ReactionProduct targetParticle;
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| 95 | targetParticle = *originalTarget;
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| 96 | currentParticle.SetSide( 1 ); // incident always goes in forward hemisphere
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| 97 | targetParticle.SetSide( -1 ); // target always goes in backward hemisphere
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| 98 | G4bool incidentHasChanged = false;
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| 99 | G4bool targetHasChanged = false;
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| 100 | G4bool quasiElastic = false;
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| 101 | G4FastVector<G4ReactionProduct,GHADLISTSIZE> vec; // vec will contain the secondary particles
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| 102 | G4int vecLen = 0;
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| 103 | vec.Initialize( 0 );
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| 104 |
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| 105 | const G4double cutOff = 0.1;
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| 106 | if( originalIncident->GetKineticEnergy()/MeV > cutOff )
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| 107 | Cascade( vec, vecLen,
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| 108 | originalIncident, currentParticle, targetParticle,
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| 109 | incidentHasChanged, targetHasChanged, quasiElastic );
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| 110 |
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| 111 | CalculateMomenta( vec, vecLen,
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| 112 | originalIncident, originalTarget, modifiedOriginal,
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| 113 | targetNucleus, currentParticle, targetParticle,
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| 114 | incidentHasChanged, targetHasChanged, quasiElastic );
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| 115 |
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| 116 | SetUpChange( vec, vecLen,
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| 117 | currentParticle, targetParticle,
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| 118 | incidentHasChanged );
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| 119 |
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| 120 | delete originalTarget;
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| 121 | return &theParticleChange;
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| 122 | }
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| 123 |
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| 124 |
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| 125 | void G4RPGSigmaMinusInelastic::Cascade(
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| 126 | G4FastVector<G4ReactionProduct,GHADLISTSIZE> &vec,
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| 127 | G4int& vecLen,
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| 128 | const G4HadProjectile *originalIncident,
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| 129 | G4ReactionProduct ¤tParticle,
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| 130 | G4ReactionProduct &targetParticle,
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| 131 | G4bool &incidentHasChanged,
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| 132 | G4bool &targetHasChanged,
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| 133 | G4bool &quasiElastic )
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| 134 | {
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| 135 | // Derived from H. Fesefeldt's original FORTRAN code CASSM
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| 136 | //
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| 137 | // SigmaMinus undergoes interaction with nucleon within a nucleus. Check if it is
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| 138 | // energetically possible to produce pions/kaons. In not, assume nuclear excitation
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| 139 | // occurs and input particle is degraded in energy. No other particles are produced.
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| 140 | // If reaction is possible, find the correct number of pions/protons/neutrons
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| 141 | // produced using an interpolation to multiplicity data. Replace some pions or
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| 142 | // protons/neutrons by kaons or strange baryons according to the average
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| 143 | // multiplicity per Inelastic reaction.
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| 144 |
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| 145 | const G4double mOriginal = originalIncident->GetDefinition()->GetPDGMass()/MeV;
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| 146 | const G4double etOriginal = originalIncident->GetTotalEnergy()/MeV;
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| 147 | const G4double targetMass = targetParticle.GetMass()/MeV;
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| 148 | G4double centerofmassEnergy = std::sqrt( mOriginal*mOriginal +
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| 149 | targetMass*targetMass +
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| 150 | 2.0*targetMass*etOriginal );
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| 151 | G4double availableEnergy = centerofmassEnergy-(targetMass+mOriginal);
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| 152 | if( availableEnergy <= G4PionPlus::PionPlus()->GetPDGMass()/MeV )
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| 153 | {
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| 154 | quasiElastic = true;
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| 155 | return;
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| 156 | }
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| 157 | static G4bool first = true;
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| 158 | const G4int numMul = 1200;
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| 159 | const G4int numSec = 60;
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| 160 | static G4double protmul[numMul], protnorm[numSec]; // proton constants
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| 161 | static G4double neutmul[numMul], neutnorm[numSec]; // neutron constants
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| 162 | // np = number of pi+, nm = number of pi-, nz = number of pi0
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| 163 | G4int counter, nt=0, np=0, nm=0, nz=0;
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| 164 | G4double test;
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| 165 | const G4double c = 1.25;
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| 166 | const G4double b[] = { 0.70, 0.70 };
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| 167 | if( first ) // compute normalization constants, this will only be Done once
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| 168 | {
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| 169 | first = false;
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| 170 | G4int i;
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| 171 | for( i=0; i<numMul; ++i )protmul[i] = 0.0;
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| 172 | for( i=0; i<numSec; ++i )protnorm[i] = 0.0;
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| 173 | counter = -1;
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| 174 | for( np=0; np<(numSec/3); ++np )
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| 175 | {
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| 176 | for( nm=std::max(0,np-1); nm<=(np+1); ++nm )
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| 177 | {
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| 178 | for( nz=0; nz<numSec/3; ++nz )
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| 179 | {
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| 180 | if( ++counter < numMul )
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| 181 | {
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| 182 | nt = np+nm+nz;
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| 183 | if( nt>0 && nt<=numSec )
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| 184 | {
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| 185 | protmul[counter] = Pmltpc(np,nm,nz,nt,b[0],c);
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| 186 | protnorm[nt-1] += protmul[counter];
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| 187 | }
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| 188 | }
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| 189 | }
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| 190 | }
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| 191 | }
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| 192 | for( i=0; i<numMul; ++i )neutmul[i] = 0.0;
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| 193 | for( i=0; i<numSec; ++i )neutnorm[i] = 0.0;
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| 194 | counter = -1;
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| 195 | for( np=0; np<numSec/3; ++np )
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| 196 | {
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| 197 | for( nm=np; nm<=(np+2); ++nm )
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| 198 | {
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| 199 | for( nz=0; nz<numSec/3; ++nz )
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| 200 | {
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| 201 | if( ++counter < numMul )
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| 202 | {
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| 203 | nt = np+nm+nz;
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| 204 | if( nt>0 && nt<=numSec )
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| 205 | {
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| 206 | neutmul[counter] = Pmltpc(np,nm,nz,nt,b[1],c);
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| 207 | neutnorm[nt-1] += neutmul[counter];
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| 208 | }
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| 209 | }
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| 210 | }
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| 211 | }
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| 212 | }
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| 213 | for( i=0; i<numSec; ++i )
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| 214 | {
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| 215 | if( protnorm[i] > 0.0 )protnorm[i] = 1.0/protnorm[i];
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| 216 | if( neutnorm[i] > 0.0 )neutnorm[i] = 1.0/neutnorm[i];
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| 217 | }
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| 218 | } // end of initialization
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| 219 |
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| 220 | const G4double expxu = 82.; // upper bound for arg. of exp
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| 221 | const G4double expxl = -expxu; // lower bound for arg. of exp
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| 222 | G4ParticleDefinition *aNeutron = G4Neutron::Neutron();
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| 223 | G4ParticleDefinition *aProton = G4Proton::Proton();
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| 224 | G4ParticleDefinition *aLambda = G4Lambda::Lambda();
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| 225 | G4ParticleDefinition *aSigmaZero = G4SigmaZero::SigmaZero();
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| 226 |
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| 227 | // energetically possible to produce pion(s) --> inelastic scattering
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| 228 |
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| 229 | G4double n, anpn;
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| 230 | GetNormalizationConstant( availableEnergy, n, anpn );
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| 231 | G4double ran = G4UniformRand();
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| 232 | G4double dum, excs = 0.0;
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| 233 | if( targetParticle.GetDefinition() == aProton )
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| 234 | {
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| 235 | counter = -1;
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| 236 | for( np=0; np<numSec/3 && ran>=excs; ++np )
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| 237 | {
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| 238 | for( nm=std::max(0,np-1); nm<=(np+1) && ran>=excs; ++nm )
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| 239 | {
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| 240 | for( nz=0; nz<numSec/3 && ran>=excs; ++nz )
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| 241 | {
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| 242 | if( ++counter < numMul )
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| 243 | {
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| 244 | nt = np+nm+nz;
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| 245 | if( nt>0 && nt<=numSec )
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| 246 | {
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| 247 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
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| 248 | dum = (pi/anpn)*nt*protmul[counter]*protnorm[nt-1]/(2.0*n*n);
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| 249 | if( std::fabs(dum) < 1.0 )
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| 250 | {
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| 251 | if( test >= 1.0e-10 )excs += dum*test;
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| 252 | }
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| 253 | else
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| 254 | excs += dum*test;
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| 255 | }
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| 256 | }
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| 257 | }
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| 258 | }
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| 259 | }
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| 260 | if( ran >= excs ) // 3 previous loops continued to the end
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| 261 | {
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| 262 | quasiElastic = true;
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| 263 | return;
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| 264 | }
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| 265 | np--; nm--; nz--;
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| 266 | G4int ncht = std::max( 1, np-nm+2 );
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| 267 | switch( ncht )
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| 268 | {
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| 269 | case 1:
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| 270 | if( G4UniformRand() < 0.5 )
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| 271 | currentParticle.SetDefinitionAndUpdateE( aLambda );
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| 272 | else
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| 273 | currentParticle.SetDefinitionAndUpdateE( aSigmaZero );
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| 274 | incidentHasChanged = true;
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| 275 | break;
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| 276 | case 2:
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| 277 | if( G4UniformRand() >= 0.5 )
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| 278 | {
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| 279 | if( G4UniformRand() < 0.5 )
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| 280 | currentParticle.SetDefinitionAndUpdateE( aLambda );
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| 281 | else
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| 282 | currentParticle.SetDefinitionAndUpdateE( aSigmaZero );
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| 283 | incidentHasChanged = true;
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| 284 | targetParticle.SetDefinitionAndUpdateE( aNeutron );
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| 285 | targetHasChanged = true;
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| 286 | }
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| 287 | break;
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| 288 | default:
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| 289 | targetParticle.SetDefinitionAndUpdateE( aNeutron );
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| 290 | targetHasChanged = true;
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| 291 | break;
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| 292 | }
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| 293 | }
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| 294 | else // target must be a neutron
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| 295 | {
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| 296 | counter = -1;
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| 297 | for( np=0; np<numSec/3 && ran>=excs; ++np )
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| 298 | {
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| 299 | for( nm=np; nm<=(np+2) && ran>=excs; ++nm )
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| 300 | {
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| 301 | for( nz=0; nz<numSec/3 && ran>=excs; ++nz )
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| 302 | {
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| 303 | if( ++counter < numMul )
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| 304 | {
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| 305 | nt = np+nm+nz;
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| 306 | if( nt>0 && nt<=numSec )
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| 307 | {
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| 308 | test = std::exp( std::min( expxu, std::max( expxl, -(pi/4.0)*(nt*nt)/(n*n) ) ) );
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| 309 | dum = (pi/anpn)*nt*neutmul[counter]*neutnorm[nt-1]/(2.0*n*n);
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| 310 | if( std::fabs(dum) < 1.0 )
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| 311 | {
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| 312 | if( test >= 1.0e-10 )excs += dum*test;
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| 313 | }
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| 314 | else
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| 315 | excs += dum*test;
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| 316 | }
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| 317 | }
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| 318 | }
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| 319 | }
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| 320 | }
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| 321 | if( ran >= excs ) // 3 previous loops continued to the end
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| 322 | {
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| 323 | quasiElastic = true;
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| 324 | return;
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| 325 | }
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| 326 | np--; nm--; nz--;
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| 327 | G4int ncht = std::max( 1, np-nm+3 );
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| 328 | switch( ncht )
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| 329 | {
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| 330 | case 1:
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| 331 | if( G4UniformRand() < 0.5 )
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| 332 | currentParticle.SetDefinitionAndUpdateE( aLambda );
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| 333 | else
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| 334 | currentParticle.SetDefinitionAndUpdateE( aSigmaZero );
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| 335 | incidentHasChanged = true;
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| 336 | targetParticle.SetDefinitionAndUpdateE( aProton );
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| 337 | targetHasChanged = true;
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| 338 | break;
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| 339 | case 2:
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| 340 | if( G4UniformRand() < 0.5 )
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| 341 | {
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| 342 | if( G4UniformRand() < 0.5 )
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| 343 | currentParticle.SetDefinitionAndUpdateE( aLambda );
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| 344 | else
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| 345 | currentParticle.SetDefinitionAndUpdateE( aSigmaZero );
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| 346 | incidentHasChanged = true;
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| 347 | }
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| 348 | else
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| 349 | {
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| 350 | targetParticle.SetDefinitionAndUpdateE( aProton );
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| 351 | targetHasChanged = true;
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| 352 | }
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| 353 | break;
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| 354 | default:
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| 355 | break;
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| 356 | }
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| 357 | }
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| 358 | SetUpPions( np, nm, nz, vec, vecLen );
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| 359 | return;
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| 360 | }
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| 361 |
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| 362 | /* end of file */
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| 363 |
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