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<< 60 InitialiseProcess(); 81 SetProcessSubType(fIonisation); << 82 SetSecondaryParticle(G4Electron::Electron()) << 83 eth = 2*CLHEP::MeV; << 84 } 61 } 85 62 86 //....oooOO0OOooo........oooOO0OOooo........oo 63 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 87 64 88 G4bool G4ionIonisation::IsApplicable(const G4P << 65 G4ionIonisation::~G4ionIonisation() 89 { << 66 {} 90 return true; << 91 } << 92 67 93 //....oooOO0OOooo........oooOO0OOooo........oo 68 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 94 69 95 G4double G4ionIonisation::MinPrimaryEnergy(con << 70 void G4ionIonisation::InitialiseProcess() 96 const G4Material*, << 97 G4double cut) << 98 { 71 { 99 return p->GetPDGMass()*(std::sqrt(1. + 0.5*c << 72 SetSecondaryParticle(G4Electron::Electron()); >> 73 SetSubCutoffIsDesired(true); >> 74 >> 75 SetDEDXBinning(120); >> 76 SetLambdaBinning(120); >> 77 SetMinKinEnergy(0.1*keV); >> 78 SetMaxKinEnergy(100.0*TeV); >> 79 >> 80 G4VEmModel* em = new G4BraggModel(); >> 81 em->SetLowEnergyLimit(0, 0.1*keV); >> 82 em->SetHighEnergyLimit(0, 2.0*MeV); >> 83 AddEmModel(em, 0); >> 84 G4VEmModel* em1 = new G4BetheBlochModel(); >> 85 em1->SetLowEnergyLimit(0, 2.0*MeV); >> 86 em1->SetHighEnergyLimit(0, 100.0*TeV); >> 87 AddEmModel(em1, 1); >> 88 >> 89 G4VEmFluctuationModel* fm = new G4UniversalFluctuation(); >> 90 AddEmFluctuationModel(fm); 100 } 91 } 101 92 102 //....oooOO0OOooo........oooOO0OOooo........oo 93 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 103 94 104 void G4ionIonisation::InitialiseEnergyLossProc << 95 const G4ParticleDefinition* G4ionIonisation::DefineBaseParticle( 105 const G4ParticleDefinition* part, << 96 const G4ParticleDefinition* p) 106 const G4ParticleDefinition* bpart) << 107 { 97 { 108 const G4ParticleDefinition* ion = G4GenericI << 98 if(!theParticle) theParticle = p; 109 << 99 return theBaseParticle; 110 if(!isInitialised) { << 111 theParticle = part; << 112 << 113 // define base particle << 114 const G4ParticleDefinition* theBaseParticl << 115 const G4int pdg = part->GetPDGEncoding(); << 116 << 117 if(part == bpart) { << 118 theBaseParticle = nullptr; << 119 } else if(nullptr != bpart) { << 120 theBaseParticle = bpart; << 121 } else if(part == ion || pdg == 1000020040 << 122 theBaseParticle = nullptr; << 123 } else { << 124 theBaseParticle = ion; << 125 } << 126 SetBaseParticle(theBaseParticle); << 127 << 128 // model limit defined for protons << 129 eth = 2*CLHEP::MeV*part->GetPDGMass()/CLHE << 130 << 131 G4EmParameters* param = G4EmParameters::In << 132 G4double emin = param->MinKinEnergy(); << 133 G4double emax = param->MaxKinEnergy(); << 134 << 135 // define model of energy loss fluctuation << 136 if (nullptr == FluctModel()) { << 137 SetFluctModel(G4EmStandUtil::ModelOfFluc << 138 } << 139 << 140 if (nullptr == EmModel(0)) { << 141 if (pdg == 1000020040) { << 142 SetEmModel(new G4BraggIonModel()); << 143 } else { << 144 SetEmModel(new G4BraggModel()); << 145 } << 146 } << 147 // to compute ranges correctly we have to << 148 // model even if activation limit is high << 149 EmModel(0)->SetLowEnergyLimit(emin); << 150 << 151 // high energy limit may be eth or DBL_MAX << 152 G4double emax1 = (EmModel(0)->HighEnergyLi << 153 EmModel(0)->SetHighEnergyLimit(emax1); << 154 AddEmModel(1, EmModel(0), FluctModel()); << 155 << 156 // second model is used if the first does << 157 if(emax1 < emax) { << 158 if (nullptr == EmModel(1)) { SetEmModel( << 159 EmModel(1)->SetLowEnergyLimit(emax1); << 160 << 161 // for extremely heavy particles upper l << 162 // should be increased << 163 emax = std::max(emax, eth*10); << 164 EmModel(1)->SetHighEnergyLimit(emax); << 165 AddEmModel(2, EmModel(1), FluctModel()); << 166 } << 167 isInitialised = true; << 168 } << 169 } 100 } 170 101 171 //....oooOO0OOooo........oooOO0OOooo........oo 102 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 172 103 173 void G4ionIonisation::ProcessDescription(std:: << 104 void G4ionIonisation::PrintInfoDefinition() const 174 { 105 { 175 out << " Ion ionisation"; << 106 G4VEnergyLossSTD::PrintInfoDefinition(); 176 G4VEnergyLossProcess::ProcessDescription(out << 107 >> 108 G4cout << " Scaling relation is used to proton dE/dx and range" >> 109 << G4endl >> 110 << " Bether-Bloch model for Escaled > 2 MeV, " >> 111 << "parametrisation of Bragg peak below." >> 112 << G4endl; 177 } 113 } 178 114 179 //....oooOO0OOooo........oooOO0OOooo........oo 115 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... >> 116 180 117