| 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 | // $Id: G4QuasiElasticChannel.cc,v 1.4 2008/04/24 13:26:19 gunter Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-02 $
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| 29 | //
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| 30 |
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| 31 | // Author : Gunter Folger March 2007
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| 32 | // Class Description
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| 33 | // Final state production model for theoretical models of hadron inelastic
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| 34 | // quasi elastic scattering in geant4;
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| 35 | // Class Description - End
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| 36 | //
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| 37 | // Modified:
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| 38 |
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| 39 | #include "G4QuasiElasticChannel.hh"
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| 40 |
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| 41 | #include "G4Fancy3DNucleus.hh"
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| 42 |
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| 43 |
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| 44 | #include "G4HadTmpUtil.hh" //lrint
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| 45 |
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| 46 | //#define debug_scatter
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| 47 |
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| 48 | G4QuasiElasticChannel::G4QuasiElasticChannel()
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| 49 | {
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| 50 | theQuasiElastic=G4QuasiFreeRatios::GetPointer();
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| 51 | }
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| 52 |
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| 53 | G4QuasiElasticChannel::~G4QuasiElasticChannel()
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| 54 | {}
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| 55 |
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| 56 | G4double G4QuasiElasticChannel::GetFraction(G4Nucleus &theNucleus,
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| 57 | const G4DynamicParticle & thePrimary)
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| 58 | {
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| 59 | std::pair<G4double,G4double> ratios;
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| 60 | ratios=theQuasiElastic->GetRatios(thePrimary.GetTotalMomentum(),
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| 61 | thePrimary.GetDefinition()->GetPDGEncoding(),
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| 62 | G4lrint(theNucleus.GetZ()),
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| 63 | G4lrint(theNucleus.GetN()-theNucleus.GetZ()));
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| 64 | #ifdef debug_getFraction
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| 65 | G4cout << "G4QuasiElasticChannel::ratios " << ratios.first << " x " <<ratios.second
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| 66 | << " = " << ratios.first*ratios.second << G4endl;
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| 67 | #endif
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| 68 |
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| 69 | return ratios.first*ratios.second;
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| 70 | }
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| 71 |
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| 72 | G4KineticTrackVector * G4QuasiElasticChannel::Scatter(G4Nucleus &theNucleus,
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| 73 | const G4DynamicParticle & thePrimary)
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| 74 | {
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| 75 |
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| 76 |
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| 77 | G4int A=G4lrint(theNucleus.GetN());
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| 78 | // G4int Z=G4lrint(theNucleus.GetZ());
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| 79 | // build Nucleus and choose random nucleon to scatter with
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| 80 | the3DNucleus.Init(theNucleus.GetN(),theNucleus.GetZ());
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| 81 | const std::vector<G4Nucleon *> nucleons=the3DNucleus.GetNucleons();
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| 82 |
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| 83 | G4int index;
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| 84 | do {
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| 85 | index=G4lrint((A-1)*G4UniformRand());
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| 86 |
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| 87 | } while (index < 0 || index >= static_cast<G4int>(nucleons.size()));
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| 88 |
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| 89 | // G4double an=G4UniformRand()*A;
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| 90 | G4ParticleDefinition * pDef= nucleons[index]->GetDefinition();
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| 91 |
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| 92 | #ifdef debug_scatter
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| 93 | G4cout << " neutron - proton? A, Z, an, pdg" <<" "
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| 94 | << A <<" "<<G4lrint(theNucleus.GetZ())
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| 95 | << " "<<an <<" " << pDef->GetParticleName()<< G4endl;
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| 96 | #endif
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| 97 | // G4LorentzVector pNucleon(G4ThreeVector(0,0,0),pDef->GetPDGMass());
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| 98 | G4LorentzVector pNucleon=nucleons[index]->Get4Momentum();
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| 99 |
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| 100 | std::pair<G4LorentzVector,G4LorentzVector> result;
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| 101 |
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| 102 | result=theQuasiElastic->Scatter(pDef->GetPDGEncoding(),pNucleon,
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| 103 | thePrimary.GetDefinition()->GetPDGEncoding(),
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| 104 | thePrimary.Get4Momentum());
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| 105 |
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| 106 | if (result.first.e() == 0.)
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| 107 | {
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| 108 | G4cout << "Warning - G4QuasiElasticChannel::Scatter no scattering" << G4endl;
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| 109 | return 0; //no scatter
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| 110 | }
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| 111 |
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| 112 | #ifdef debug_scatter
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| 113 | G4LorentzVector EpConservation=pNucleon+thePrimary.Get4Momentum()
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| 114 | - result.first - result.second;
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| 115 | if ( (EpConservation.vect().mag2() > 0.01*MeV*MeV )
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| 116 | || (std::abs(EpConservation.e()) > 0.1 * MeV ) )
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| 117 | {
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| 118 | G4cout << "Warning - G4QuasiElasticChannel::Scatter E-p non conservation : "
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| 119 | << EpConservation << G4endl;
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| 120 | }
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| 121 | #endif
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| 122 |
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| 123 | G4KineticTrackVector * ktv;
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| 124 | ktv=new G4KineticTrackVector();
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| 125 | G4KineticTrack * sPrim=new G4KineticTrack(thePrimary.GetDefinition(),
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| 126 | 0.,G4ThreeVector(0), result.second);
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| 127 | ktv->push_back(sPrim);
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| 128 | G4KineticTrack * sNuc=new G4KineticTrack(pDef,
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| 129 | 0.,G4ThreeVector(0), result.first);
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| 130 | ktv->push_back(sNuc);
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| 131 |
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| 132 | #ifdef debug_scatter
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| 133 | G4cout << " scattered Nucleon : " << result.first << " mass " <<result.first.mag() << G4endl;
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| 134 | G4cout << " scattered Project : " << result.second << " mass " <<result.second.mag() << G4endl;
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| 135 | #endif
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| 136 | return ktv;
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| 137 | }
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