| 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 | // ------------------------------------------------------------
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| 29 | // GEANT 4 class implementation file
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| 30 | //
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| 31 | // ---------------- G4Fancy3DNucleus ----------------
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| 32 | // by Gunter Folger, May 1998.
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| 33 | // class for a 3D nucleus, arranging nucleons in space and momentum.
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| 34 | // ------------------------------------------------------------
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| 35 |
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| 36 | #include "G4Fancy3DNucleus.hh"
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| 37 | #include "G4NuclearFermiDensity.hh"
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| 38 | #include "G4NuclearShellModelDensity.hh"
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| 39 | #include "G4NucleiPropertiesTable.hh"
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| 40 | #include "Randomize.hh"
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| 41 | #include "G4ios.hh"
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| 42 | #include <algorithm>
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| 43 | #include "G4HadronicException.hh"
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| 44 |
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| 45 | G4Fancy3DNucleus::G4Fancy3DNucleus()
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| 46 | : nucleondistance(0.8*fermi)
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| 47 | {
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| 48 | theDensity=0;
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| 49 | theNucleons=0;
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| 50 | currentNucleon=-1;
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| 51 | myA=0;
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| 52 | myZ=0;
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| 53 | //G4cout <<"G4Fancy3DNucleus::G4Fancy3DNucleus()"<<G4endl;
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| 54 | }
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| 55 |
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| 56 | G4Fancy3DNucleus::~G4Fancy3DNucleus()
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| 57 | {
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| 58 | if(theNucleons) delete [] theNucleons;
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| 59 | if(theDensity) delete theDensity;
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| 60 | }
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| 61 |
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| 62 |
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| 63 | void G4Fancy3DNucleus::Init(G4double theA, G4double theZ)
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| 64 | {
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| 65 | // G4cout << "G4Fancy3DNucleus::Init(theA, theZ) called"<<G4endl;
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| 66 | currentNucleon=-1;
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| 67 | if(theNucleons) delete [] theNucleons;
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| 68 |
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| 69 | // this was delected already:
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| 70 | // std::for_each(theRWNucleons.begin(), theRWNucleons.end(), DeleteNucleon());
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| 71 | theRWNucleons.clear();
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| 72 |
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| 73 | myZ = G4int(theZ);
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| 74 | myA= ( G4UniformRand()>theA-G4int(theA) ) ? G4int(theA) : G4int(theA)+1;
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| 75 |
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| 76 | theNucleons = new G4Nucleon[myA];
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| 77 |
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| 78 | // G4cout << "myA, myZ" << myA << ", " << myZ << G4endl;
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| 79 |
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| 80 | if(theDensity) delete theDensity;
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| 81 | if ( myA < 17 ) {
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| 82 | theDensity = new G4NuclearShellModelDensity(myA, myZ);
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| 83 | } else {
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| 84 | theDensity = new G4NuclearFermiDensity(myA, myZ);
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| 85 | }
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| 86 |
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| 87 | theFermi.Init(myA, myZ);
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| 88 |
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| 89 | ChooseNucleons();
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| 90 |
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| 91 | ChoosePositions();
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| 92 |
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| 93 | // CenterNucleons(); // This would introduce a bias
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| 94 |
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| 95 | ChooseFermiMomenta();
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| 96 |
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| 97 | G4double Ebinding= BindingEnergy()/myA;
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| 98 |
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| 99 | for (G4int aNucleon=0; aNucleon < myA; aNucleon++)
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| 100 | {
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| 101 | theNucleons[aNucleon].SetBindingEnergy(Ebinding);
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| 102 | }
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| 103 |
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| 104 |
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| 105 | return;
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| 106 | }
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| 107 |
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| 108 | G4bool G4Fancy3DNucleus::StartLoop()
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| 109 | {
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| 110 | currentNucleon=0;
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| 111 | return theNucleons;
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| 112 | }
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| 113 |
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| 114 | G4Nucleon * G4Fancy3DNucleus::GetNextNucleon()
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| 115 | {
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| 116 | return ( currentNucleon>=0 && currentNucleon<myA ) ?
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| 117 | theNucleons+currentNucleon++ : 0;
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| 118 | }
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| 119 |
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| 120 |
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| 121 | const std::vector<G4Nucleon *> & G4Fancy3DNucleus::GetNucleons()
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| 122 | {
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| 123 | if ( theRWNucleons.size()==0 )
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| 124 | {
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| 125 | for (G4int i=0; i< myA; i++)
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| 126 | {
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| 127 | theRWNucleons.push_back(theNucleons+i);
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| 128 | }
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| 129 | }
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| 130 | return theRWNucleons;
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| 131 | }
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| 132 |
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| 133 | G4double G4Fancy3DNucleus::BindingEnergy()
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| 134 | {
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| 135 | return G4NucleiPropertiesTable::GetBindingEnergy(myZ,myA);
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| 136 | }
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| 137 |
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| 138 | G4double G4Fancy3DNucleus::GetNuclearRadius()
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| 139 | {
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| 140 | return GetNuclearRadius(0.5);
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| 141 | }
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| 142 |
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| 143 | G4double G4Fancy3DNucleus::GetNuclearRadius(const G4double maxRelativeDensity)
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| 144 | {
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| 145 | return theDensity->GetRadius(maxRelativeDensity);
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| 146 | }
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| 147 |
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| 148 | G4double G4Fancy3DNucleus::GetOuterRadius()
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| 149 | {
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| 150 | G4double maxradius2=0;
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| 151 |
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| 152 | for (int i=0; i<myA; i++)
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| 153 | {
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| 154 | if ( theNucleons[i].GetPosition().mag2() > maxradius2 )
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| 155 | {
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| 156 | maxradius2=theNucleons[i].GetPosition().mag2();
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| 157 | }
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| 158 | }
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| 159 | return std::sqrt(maxradius2)+nucleondistance;
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| 160 | }
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| 161 |
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| 162 | G4double G4Fancy3DNucleus::GetMass()
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| 163 | {
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| 164 | return myZ*G4Proton::Proton()->GetPDGMass() +
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| 165 | (myA-myZ)*G4Neutron::Neutron()->GetPDGMass() -
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| 166 | BindingEnergy();
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| 167 | }
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| 168 |
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| 169 |
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| 170 |
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| 171 | void G4Fancy3DNucleus::DoLorentzBoost(const G4LorentzVector & theBoost)
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| 172 | {
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| 173 | for (G4int i=0; i<myA; i++){
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| 174 | theNucleons[i].Boost(theBoost);
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| 175 | }
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| 176 | }
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| 177 |
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| 178 | void G4Fancy3DNucleus::DoLorentzBoost(const G4ThreeVector & theBeta)
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| 179 | {
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| 180 | for (G4int i=0; i<myA; i++){
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| 181 | theNucleons[i].Boost(theBeta);
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| 182 | }
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| 183 | }
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| 184 |
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| 185 | void G4Fancy3DNucleus::DoLorentzContraction(const G4ThreeVector & theBeta)
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| 186 | {
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| 187 | G4double factor=(1-std::sqrt(1-theBeta.mag2()))/theBeta.mag2(); // (gamma-1)/gamma/beta**2
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| 188 | for (G4int i=0; i< myA; i++)
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| 189 | {
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| 190 | G4ThreeVector rprime=theNucleons[i].GetPosition() -
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| 191 | factor * (theBeta*theNucleons[i].GetPosition()) *
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| 192 | // theNucleons[i].GetPosition();
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| 193 | theBeta;
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| 194 | theNucleons[i].SetPosition(rprime);
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| 195 | }
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| 196 | }
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| 197 |
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| 198 | void G4Fancy3DNucleus::DoLorentzContraction(const G4LorentzVector & theBoost)
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| 199 | {
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| 200 | G4ThreeVector beta= 1/theBoost.e() * theBoost.vect();
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| 201 | // DoLorentzBoost(beta);
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| 202 | DoLorentzContraction(beta);
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| 203 | }
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| 204 |
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| 205 |
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| 206 |
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| 207 | void G4Fancy3DNucleus::CenterNucleons()
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| 208 | {
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| 209 | G4ThreeVector center;
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| 210 |
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| 211 | for (G4int i=0; i<myA; i++ )
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| 212 | {
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| 213 | center+=theNucleons[i].GetPosition();
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| 214 | }
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| 215 | center *= -1./myA;
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| 216 | DoTranslation(center);
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| 217 | }
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| 218 |
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| 219 | void G4Fancy3DNucleus::DoTranslation(const G4ThreeVector & theShift)
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| 220 | {
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| 221 | for (G4int i=0; i<myA; i++ )
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| 222 | {
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| 223 | G4ThreeVector tempV = theNucleons[i].GetPosition() + theShift;
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| 224 | theNucleons[i].SetPosition(tempV);
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| 225 | }
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| 226 | }
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| 227 |
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| 228 | const G4VNuclearDensity * G4Fancy3DNucleus::GetNuclearDensity() const
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| 229 | {
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| 230 | return theDensity;
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| 231 | }
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| 232 |
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| 233 | //----------------------- private Implementation Methods-------------
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| 234 |
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| 235 | void G4Fancy3DNucleus::ChooseNucleons()
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| 236 | {
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| 237 | G4int protons=0,nucleons=0;
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| 238 |
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| 239 | while (nucleons < myA )
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| 240 | {
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| 241 | if ( protons < myZ && G4UniformRand() < (G4double)(myZ-protons)/(G4double)(myA-nucleons) )
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| 242 | {
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| 243 | protons++;
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| 244 | theNucleons[nucleons++].SetParticleType(G4Proton::Proton());
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| 245 | }
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| 246 | else if ( (nucleons-protons) < (myA-myZ) )
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| 247 | {
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| 248 | theNucleons[nucleons++].SetParticleType(G4Neutron::Neutron());
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| 249 | }
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| 250 | else G4cout << "G4Fancy3DNucleus::ChooseNucleons not efficient" << G4endl;
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| 251 | }
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| 252 | return;
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| 253 | }
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| 254 |
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| 255 | void G4Fancy3DNucleus::ChoosePositions()
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| 256 | {
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| 257 | G4int i=0;
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| 258 | G4ThreeVector aPos, delta;
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| 259 | std::vector<G4ThreeVector> places;
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| 260 | places.reserve(myA);
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| 261 | G4bool freeplace;
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| 262 | static G4double nd2 = sqr(nucleondistance);
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| 263 | G4double maxR=GetNuclearRadius(0.01); // there are no nucleons at a
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| 264 | // relative Density of 0.01
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| 265 | G4int jr=0;
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| 266 | G4int jx,jy;
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| 267 | G4double arand[600];
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| 268 | G4double *prand=arand;
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| 269 | // G4int Attempt=0;
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| 270 | while ( i < myA )
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| 271 | {
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| 272 | do
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| 273 | {
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| 274 | // ++Attempt;
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| 275 | if ( jr < 3 )
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| 276 | {
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| 277 | jr=std::min(600,9*(myA - i));
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| 278 | CLHEP::RandFlat::shootArray(jr, prand );
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| 279 | }
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| 280 | jx=--jr;
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| 281 | jy=--jr;
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| 282 | aPos=G4ThreeVector( (2*arand[jx]-1.),
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| 283 | (2*arand[jy]-1.),
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| 284 | (2*arand[--jr]-1.));
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| 285 | } while (aPos.mag2() > 1. );
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| 286 | aPos *=maxR;
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| 287 | G4double density=theDensity->GetRelativeDensity(aPos);
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| 288 | if (G4UniformRand() < density)
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| 289 | {
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| 290 | freeplace= true;
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| 291 | std::vector<G4ThreeVector>::iterator iplace;
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| 292 | for( iplace=places.begin(); iplace!=places.end() && freeplace;++iplace)
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| 293 | {
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| 294 | delta = *iplace - aPos;
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| 295 | freeplace= delta.mag2() > nd2;
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| 296 | }
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| 297 |
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| 298 | if ( freeplace )
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| 299 | {
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| 300 | G4double pFermi=theFermi.GetFermiMomentum(theDensity->GetDensity(aPos));
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| 301 | // protons must at least have binding energy of CoulombBarrier, so
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| 302 | // assuming the Fermi energy corresponds to a potential, we must place these such
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| 303 | // that the Fermi Energy > CoulombBarrier
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| 304 | if (theNucleons[i].GetDefinition() == G4Proton::Proton())
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| 305 | {
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| 306 | G4double eFermi= std::sqrt( sqr(pFermi) + sqr(theNucleons[i].GetDefinition()->GetPDGMass()) )
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| 307 | - theNucleons[i].GetDefinition()->GetPDGMass();
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| 308 | if (eFermi <= CoulombBarrier() ) freeplace=false;
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| 309 | }
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| 310 | }
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| 311 | if ( freeplace )
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| 312 | {
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| 313 | theNucleons[i].SetPosition(aPos);
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| 314 | places.push_back(aPos);
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| 315 | ++i;
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| 316 | }
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| 317 | }
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| 318 | }
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| 319 | // G4cout << "Att " << myA << " " << Attempt << G4endl;
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| 320 |
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| 321 | }
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| 322 |
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| 323 | void G4Fancy3DNucleus::ChooseFermiMomenta()
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| 324 | {
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| 325 | G4int i;
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| 326 | G4double density;
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| 327 | G4ThreeVector * momentum=new G4ThreeVector[myA];
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| 328 |
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| 329 | G4double * fermiM=new G4double[myA];
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| 330 |
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| 331 | for (G4int ntry=0; ntry<1 ; ntry ++ )
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| 332 | {
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| 333 | for (i=0; i < myA; i++ ) // momenta for all, including last, in case we swap nucleons
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| 334 | {
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| 335 | density = theDensity->GetDensity(theNucleons[i].GetPosition());
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| 336 | fermiM[i] = theFermi.GetFermiMomentum(density);
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| 337 | G4ThreeVector mom=theFermi.GetMomentum(density);
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| 338 | if (theNucleons[i].GetDefinition() == G4Proton::Proton())
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| 339 | {
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| 340 | G4double eMax = std::sqrt(sqr(fermiM[i]) +sqr(theNucleons[i].GetDefinition()->GetPDGMass()) )
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| 341 | - CoulombBarrier();
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| 342 | if ( eMax > theNucleons[i].GetDefinition()->GetPDGMass() )
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| 343 | {
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| 344 | G4double pmax2= sqr(eMax) - sqr(theNucleons[i].GetDefinition()->GetPDGMass());
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| 345 | fermiM[i] = std::sqrt(pmax2);
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| 346 | while ( mom.mag2() > pmax2 )
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| 347 | {
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| 348 | mom=theFermi.GetMomentum(density, fermiM[i]);
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| 349 | }
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| 350 | } else
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| 351 | {
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| 352 | G4cerr << "G4Fancy3DNucleus: difficulty finding proton momentum" << G4endl;
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| 353 | mom=0;
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| 354 | }
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| 355 |
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| 356 | }
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| 357 | momentum[i]= mom;
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| 358 | }
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| 359 |
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| 360 | if (ReduceSum(momentum,fermiM) )
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| 361 | break;
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| 362 | // G4cout <<" G4FancyNucleus: iterating to find momenta: "<< ntry<< G4endl;
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| 363 | }
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| 364 |
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| 365 | // G4ThreeVector sum;
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| 366 | // for (G4int index=0; index<myA;sum+=momentum[index++])
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| 367 | // ;
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| 368 | // G4cout << "final sum / mag() " << sum << " / " << sum.mag() << G4endl;
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| 369 |
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| 370 |
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| 371 | G4double energy;
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| 372 | for ( i=0; i< myA ; i++ )
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| 373 | {
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| 374 | energy = theNucleons[i].GetParticleType()->GetPDGMass()
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| 375 | - BindingEnergy()/myA;
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| 376 | G4LorentzVector tempV(momentum[i],energy);
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| 377 | theNucleons[i].SetMomentum(tempV);
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| 378 | }
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| 379 |
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| 380 | delete [] momentum;
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| 381 | delete [] fermiM;
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| 382 | }
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| 383 |
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| 384 | class G4Fancy3DNucleusHelper // Helper class
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| 385 | {
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| 386 | public:
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| 387 | G4Fancy3DNucleusHelper(const G4ThreeVector &vec,const G4double size,const G4int index)
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| 388 | : Vector(vec), Size(size), anInt(index) {}
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| 389 | int operator ==(const G4Fancy3DNucleusHelper &right) const
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| 390 | {
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| 391 | return this==&right;
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| 392 | }
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| 393 | int operator < (const G4Fancy3DNucleusHelper &right) const
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| 394 | {
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| 395 | return size()<right.size();
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| 396 | }
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| 397 | const G4ThreeVector& vector() const
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| 398 | {
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| 399 | return Vector;
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| 400 | }
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| 401 | G4double size() const
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| 402 | {
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| 403 | return Size;
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| 404 | }
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| 405 | G4int index() const
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| 406 | {
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| 407 | return anInt;
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| 408 | }
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| 409 | G4Fancy3DNucleusHelper operator =(const G4Fancy3DNucleusHelper &right)
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| 410 | {
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| 411 | Vector = right.Vector;
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| 412 | Size = right.Size;
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| 413 | anInt = right.anInt;
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| 414 | return *this;
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| 415 | }
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| 416 |
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| 417 | private:
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| 418 | G4Fancy3DNucleusHelper(): Vector(0), Size(0), anInt(0) {G4cout << "def ctor for MixMasch" << G4endl;}
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| 419 | G4ThreeVector Vector;
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| 420 | G4double Size;
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| 421 | G4int anInt;
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| 422 | };
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| 423 |
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| 424 | G4bool G4Fancy3DNucleus::ReduceSum(G4ThreeVector * momentum, G4double *pFermiM)
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| 425 | {
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| 426 | G4ThreeVector sum;
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| 427 | G4double PFermi=pFermiM[myA-1];
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| 428 |
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| 429 | for (G4int i=0; i < myA-1 ; i++ )
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| 430 | { sum+=momentum[i]; }
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| 431 |
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| 432 | // check if have to do anything at all..
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| 433 | if ( sum.mag() <= PFermi )
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| 434 | {
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| 435 | momentum[myA-1]=-sum;
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| 436 | return true;
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| 437 | }
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| 438 |
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| 439 | // find all possible changes in momentum, changing only the component parallel to sum
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| 440 | G4ThreeVector testDir=sum.unit();
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| 441 | std::vector<G4Fancy3DNucleusHelper> testSums; // Sorted on delta.mag()
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| 442 |
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| 443 | for ( G4int aNucleon=0; aNucleon < myA-1; aNucleon++){
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| 444 | G4ThreeVector delta=2*((momentum[aNucleon]*testDir)* testDir);
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| 445 | testSums.push_back(G4Fancy3DNucleusHelper(delta,delta.mag(),aNucleon));
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| 446 | }
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| 447 | std::sort(testSums.begin(), testSums.end());
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| 448 |
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| 449 | // reduce Momentum Sum until the next would be allowed.
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| 450 | G4int index=testSums.size();
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|---|
| 451 | while ( (sum-testSums[--index].vector()).mag()>PFermi && index>0)
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|---|
| 452 | {
|
|---|
| 453 | // Only take one which improve, ie. don't change sign and overshoot...
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|---|
| 454 | if ( sum.mag() > (sum-testSums[index].vector()).mag() ) {
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|---|
| 455 | momentum[testSums[index].index()]-=testSums[index].vector();
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|---|
| 456 | sum-=testSums[index].vector();
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|---|
| 457 | }
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|---|
| 458 | }
|
|---|
| 459 |
|
|---|
| 460 | if ( (sum-testSums[index].vector()).mag() <= PFermi )
|
|---|
| 461 | {
|
|---|
| 462 | G4int best=-1;
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|---|
| 463 | G4double pBest=2*PFermi; // anything larger than PFermi
|
|---|
| 464 | for ( G4int aNucleon=0; aNucleon<=index; aNucleon++)
|
|---|
| 465 | {
|
|---|
| 466 | // find the momentum closest to choosen momentum for last Nucleon.
|
|---|
| 467 | G4double pTry=(testSums[aNucleon].vector()-sum).mag();
|
|---|
| 468 | if ( pTry < PFermi
|
|---|
| 469 | && std::abs(momentum[myA-1].mag() - pTry ) < pBest )
|
|---|
| 470 | {
|
|---|
| 471 | pBest=std::abs(momentum[myA-1].mag() - pTry );
|
|---|
| 472 | best=aNucleon;
|
|---|
| 473 | }
|
|---|
| 474 | }
|
|---|
| 475 | if ( best < 0 )
|
|---|
| 476 | {
|
|---|
| 477 | G4String text = "G4Fancy3DNucleus.cc: Logic error in ReduceSum()";
|
|---|
| 478 | throw G4HadronicException(__FILE__, __LINE__, text);
|
|---|
| 479 | }
|
|---|
| 480 | momentum[testSums[best].index()]-=testSums[best].vector();
|
|---|
| 481 | momentum[myA-1]=testSums[best].vector()-sum;
|
|---|
| 482 |
|
|---|
| 483 | testSums.clear();
|
|---|
| 484 | return true;
|
|---|
| 485 |
|
|---|
| 486 | }
|
|---|
| 487 | testSums.clear();
|
|---|
| 488 |
|
|---|
| 489 | // try to compensate momentum using another Nucleon....
|
|---|
| 490 |
|
|---|
| 491 | G4int swapit=-1;
|
|---|
| 492 | while (swapit<myA-1)
|
|---|
| 493 | {
|
|---|
| 494 | if ( pFermiM[++swapit] > PFermi ) break;
|
|---|
| 495 | }
|
|---|
| 496 | if (swapit == myA-1 ) return false;
|
|---|
| 497 |
|
|---|
| 498 | // Now we have a nucleon with a bigger Fermi Momentum.
|
|---|
| 499 | // Exchange with last nucleon.. and iterate.
|
|---|
| 500 | // G4cout << " Nucleon to swap with : " << swapit << G4endl;
|
|---|
| 501 | // G4cout << " Fermi momentum test, and better.. " << PFermi << " / "
|
|---|
| 502 | // << theFermi.GetFermiMomentum(density) << G4endl;
|
|---|
| 503 | // cout << theNucleons[swapit]<< G4endl << theNucleons[myA-1] << G4endl;
|
|---|
| 504 | // cout << momentum[swapit] << G4endl << momentum[myA-1] << G4endl;
|
|---|
| 505 | G4Nucleon swap= theNucleons[swapit];
|
|---|
| 506 | G4ThreeVector mom_swap=momentum[swapit];
|
|---|
| 507 | G4double pf=pFermiM[swapit];
|
|---|
| 508 | theNucleons[swapit]=theNucleons[myA-1];
|
|---|
| 509 | momentum[swapit]=momentum[myA-1];
|
|---|
| 510 | pFermiM[swapit]=pFermiM[myA-1];
|
|---|
| 511 | theNucleons[myA-1]=swap;
|
|---|
| 512 | momentum[myA-1]=mom_swap;
|
|---|
| 513 | pFermiM[myA-1]=pf;
|
|---|
| 514 | // cout << "after swap" <<G4endl<< theNucleons[swapit] << G4endl << theNucleons[myA-1] << G4endl;
|
|---|
| 515 | // cout << momentum[swapit] << G4endl << momentum[myA-1] << G4endl;
|
|---|
| 516 | return ReduceSum(momentum,pFermiM);
|
|---|
| 517 | }
|
|---|
| 518 |
|
|---|
| 519 | G4double G4Fancy3DNucleus::CoulombBarrier()
|
|---|
| 520 | {
|
|---|
| 521 | G4double coulombBarrier = (1.44/1.14) * MeV * myZ / (1.0 + std::pow(G4double(myA),1./3.));
|
|---|
| 522 | return coulombBarrier;
|
|---|
| 523 | }
|
|---|