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Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitatio 16 // * for the full disclaimer and the limitation of liability. * 17 // * 17 // * * 18 // * This code implementation is the result 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboratio 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distri 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you ag 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publicati 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Sof 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************* 24 // ******************************************************************** 25 // 25 // >> 26 // $Id: G4LivermorePhotoElectricModel.cc 90578 2015-06-04 09:55:07Z gcosmo $ >> 27 // 26 // 28 // 27 // Author: Sebastien Incerti 29 // Author: Sebastien Incerti 28 // 30 October 2008 30 // 30 October 2008 29 // on base of G4LowEnergyPhotoElectric 31 // on base of G4LowEnergyPhotoElectric developed by A.Forti and M.G.Pia 30 // 32 // 31 // 22 Oct 2012 A & V Ivanchenko Migration da 33 // 22 Oct 2012 A & V Ivanchenko Migration data structure to G4PhysicsVector 32 // 1 June 2017 M Bandieramonte: New model ba << 34 // 33 // evaluated data - parameteriza << 34 35 35 #include "G4LivermorePhotoElectricModel.hh" 36 #include "G4LivermorePhotoElectricModel.hh" 36 << 37 #include "G4SystemOfUnits.hh" 37 #include "G4AtomicShell.hh" << 38 #include "G4PhysicalConstants.hh" 38 #include "G4AutoLock.hh" << 39 #include "G4LossTableManager.hh" 39 #include "G4CrossSectionHandler.hh" << 40 #include "G4Electron.hh" 40 #include "G4Electron.hh" 41 #include "G4Gamma.hh" 41 #include "G4Gamma.hh" 42 #include "G4LossTableManager.hh" << 43 #include "G4ParticleChangeForGamma.hh" 42 #include "G4ParticleChangeForGamma.hh" 44 #include "G4PhysicsFreeVector.hh" << 43 #include "G4CrossSectionHandler.hh" 45 #include "G4SauterGavrilaAngularDistribution.h << 44 #include "G4LPhysicsFreeVector.hh" 46 #include "G4SystemOfUnits.hh" << 47 #include "G4VAtomDeexcitation.hh" 45 #include "G4VAtomDeexcitation.hh" 48 #include "G4EmParameters.hh" << 46 #include "G4SauterGavrilaAngularDistribution.hh" 49 #include <thread> << 47 #include "G4AtomicShell.hh" 50 48 51 //....oooOO0OOooo........oooOO0OOooo........oo 49 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 52 50 53 G4ElementData* G4LivermorePhotoElectricModel:: << 51 G4LPhysicsFreeVector* G4LivermorePhotoElectricModel::fCrossSection[] = {0}; 54 G4ElementData* G4LivermorePhotoElectricModel:: << 52 G4LPhysicsFreeVector* G4LivermorePhotoElectricModel::fCrossSectionLE[] = {0}; 55 std::vector<G4double>* G4LivermorePhotoElectri << 53 std::vector<G4double>* G4LivermorePhotoElectricModel::fParam[] = {0}; 56 std::vector<G4double>* G4LivermorePhotoElectri << 54 G4int G4LivermorePhotoElectricModel::fNShells[] = {0}; 57 G4int G4LivermorePhotoElectricModel::fNShells[ << 55 G4int G4LivermorePhotoElectricModel::fNShellsUsed[] = {0}; 58 G4int G4LivermorePhotoElectricModel::fNShellsU << 56 G4ElementData* G4LivermorePhotoElectricModel::fShellCrossSection = 0; 59 G4Material* G4LivermorePhotoElectricModel::fWa << 57 G4Material* G4LivermorePhotoElectricModel::fWater = 0; 60 G4double G4LivermorePhotoElectricModel::fWater << 58 G4double G4LivermorePhotoElectricModel::fWaterEnergyLimit = 0.0; 61 G4String G4LivermorePhotoElectricModel::fDataD << 62 59 63 static std::once_flag applyOnce; << 60 using namespace std; 64 << 65 namespace << 66 { << 67 G4Mutex livPhotoeffMutex = G4MUTEX_INITIALIZ << 68 } << 69 61 70 //....oooOO0OOooo........oooOO0OOooo........oo 62 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 71 63 72 G4LivermorePhotoElectricModel::G4LivermorePhot << 64 G4LivermorePhotoElectricModel::G4LivermorePhotoElectricModel( 73 { << 65 const G4String& nam) 74 verboseLevel = 0; << 66 : G4VEmModel(nam),fParticleChange(0),maxZ(99), >> 67 nShellLimit(100),fDeexcitationActive(false),isInitialised(false), >> 68 fAtomDeexcitation(0) >> 69 { >> 70 verboseLevel= 0; 75 // Verbosity scale: 71 // Verbosity scale: 76 // 0 = nothing << 72 // 0 = nothing 77 // 1 = warning for energy non-conservation << 73 // 1 = warning for energy non-conservation 78 // 2 = details of energy budget 74 // 2 = details of energy budget 79 // 3 = calculation of cross sections, file o 75 // 3 = calculation of cross sections, file openings, sampling of atoms 80 // 4 = entering in methods 76 // 4 = entering in methods 81 77 82 theGamma = G4Gamma::Gamma(); << 78 theGamma = G4Gamma::Gamma(); 83 theElectron = G4Electron::Electron(); 79 theElectron = G4Electron::Electron(); 84 80 85 // default generator 81 // default generator 86 SetAngularDistribution(new G4SauterGavrilaAn 82 SetAngularDistribution(new G4SauterGavrilaAngularDistribution()); 87 83 88 if (verboseLevel > 0) { << 84 if(verboseLevel>0) { 89 G4cout << "Livermore PhotoElectric is cons << 85 G4cout << "Livermore PhotoElectric is constructed " 90 << " nShellLimit= " << nShellLimit << 86 << " nShellLimit= " << nShellLimit << G4endl; 91 } 87 } 92 88 93 // Mark this model as "applicable" for atomi << 89 //Mark this model as "applicable" for atomic deexcitation 94 SetDeexcitationFlag(true); 90 SetDeexcitationFlag(true); 95 << 91 fSandiaCof.resize(4,0.0); 96 // For water << 92 fCurrSection = 0.0; 97 fSandiaCof.resize(4, 0.0); << 98 } 93 } 99 94 100 //....oooOO0OOooo........oooOO0OOooo........oo 95 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 101 96 102 G4LivermorePhotoElectricModel::~G4LivermorePho 97 G4LivermorePhotoElectricModel::~G4LivermorePhotoElectricModel() 103 { << 98 { 104 if (isInitializer) { << 99 if(IsMaster()) { 105 for (G4int i = 0; i < ZMAXPE; ++i) { << 100 delete fShellCrossSection; 106 if (fParamHigh[i]) { << 101 for(G4int i=0; i<maxZ; ++i) { 107 delete fParamHigh[i]; << 102 delete fParam[i]; 108 fParamHigh[i] = nullptr; << 103 fParam[i] = 0; 109 } << 104 delete fCrossSection[i]; 110 if (fParamLow[i]) { << 105 fCrossSection[i] = 0; 111 delete fParamLow[i]; << 106 delete fCrossSectionLE[i]; 112 fParamLow[i] = nullptr; << 107 fCrossSectionLE[i] = 0; 113 } << 114 } 108 } 115 } 109 } 116 } 110 } 117 111 118 //....oooOO0OOooo........oooOO0OOooo........oo 112 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 119 113 120 void G4LivermorePhotoElectricModel::Initialise << 114 void 121 const G4DataVector&) << 115 G4LivermorePhotoElectricModel::Initialise(const G4ParticleDefinition*, 122 { << 116 const G4DataVector&) 123 if (verboseLevel > 1) { << 117 { 124 G4cout << "Calling G4LivermorePhotoElectri << 118 if (verboseLevel > 2) { >> 119 G4cout << "Calling G4LivermorePhotoElectricModel::Initialise()" << G4endl; >> 120 } >> 121 >> 122 if(IsMaster()) { >> 123 >> 124 if(!fWater) { >> 125 fWater = G4Material::GetMaterial("G4_WATER", false); >> 126 if(fWater) { fWaterEnergyLimit = 13.6*eV; } >> 127 } >> 128 >> 129 if(!fShellCrossSection) { fShellCrossSection = new G4ElementData(); } >> 130 >> 131 char* path = getenv("G4LEDATA"); >> 132 >> 133 G4ProductionCutsTable* theCoupleTable = >> 134 G4ProductionCutsTable::GetProductionCutsTable(); >> 135 G4int numOfCouples = theCoupleTable->GetTableSize(); >> 136 >> 137 for(G4int i=0; i<numOfCouples; ++i) { >> 138 const G4MaterialCutsCouple* couple = >> 139 theCoupleTable->GetMaterialCutsCouple(i); >> 140 const G4Material* material = couple->GetMaterial(); >> 141 const G4ElementVector* theElementVector = material->GetElementVector(); >> 142 G4int nelm = material->GetNumberOfElements(); >> 143 >> 144 for (G4int j=0; j<nelm; ++j) { >> 145 G4int Z = (G4int)(*theElementVector)[j]->GetZ(); >> 146 if(Z < 1) { Z = 1; } >> 147 else if(Z > maxZ) { Z = maxZ; } >> 148 if(!fCrossSection[Z]) { ReadData(Z, path); } >> 149 } >> 150 } >> 151 } >> 152 // >> 153 if (verboseLevel > 2) { >> 154 G4cout << "Loaded cross section files for LivermorePhotoElectric model" >> 155 << G4endl; 125 } 156 } 126 << 157 if(!isInitialised) { 127 // initialise static tables only once << 158 isInitialised = true; 128 std::call_once(applyOnce, [this]() { isIniti << 129 << 130 if (isInitializer) { << 131 G4AutoLock l(&livPhotoeffMutex); << 132 FindDirectoryPath(); << 133 if (fWater == nullptr) { << 134 fWater = G4Material::GetMaterial("G4_WAT << 135 if (fWater == nullptr) { << 136 fWater = G4Material::GetMaterial("Wate << 137 } << 138 if (fWater != nullptr) { << 139 fWaterEnergyLimit = 13.6 * CLHEP::eV; << 140 } << 141 } << 142 << 143 if (fCrossSection == nullptr) { << 144 fCrossSection = new G4ElementData(ZMAXPE << 145 fCrossSection->SetName("PhotoEffXS"); << 146 fCrossSectionLE = new G4ElementData(ZMAX << 147 fCrossSectionLE->SetName("PhotoEffLowXS" << 148 } << 149 << 150 const G4ElementTable* elemTable = G4Elemen << 151 std::size_t numElems = (*elemTable).size() << 152 for (std::size_t ie = 0; ie < numElems; ++ << 153 const G4Element* elem = (*elemTable)[ie] << 154 G4int Z = elem->GetZasInt(); << 155 if (Z < ZMAXPE) { << 156 if (fCrossSection->GetElementData(Z) == null << 157 ReadData(Z); << 158 } << 159 } << 160 } << 161 l.unlock(); << 162 } << 163 << 164 if (verboseLevel > 1) { << 165 G4cout << "Loaded cross section files for << 166 } << 167 if (nullptr == fParticleChange) { << 168 fParticleChange = GetParticleChangeForGamm 159 fParticleChange = GetParticleChangeForGamma(); >> 160 169 fAtomDeexcitation = G4LossTableManager::In 161 fAtomDeexcitation = G4LossTableManager::Instance()->AtomDeexcitation(); 170 } 162 } 171 << 172 fDeexcitationActive = false; 163 fDeexcitationActive = false; 173 if (nullptr != fAtomDeexcitation) { << 164 if(fAtomDeexcitation) { 174 fDeexcitationActive = fAtomDeexcitation->I << 165 fDeexcitationActive = fAtomDeexcitation->IsFluoActive(); 175 } 166 } 176 167 177 if (verboseLevel > 1) { << 168 if (verboseLevel > 0) { 178 G4cout << "LivermorePhotoElectric model is << 169 G4cout << "LivermorePhotoElectric model is initialized " << G4endl >> 170 << G4endl; 179 } 171 } 180 } 172 } 181 173 182 //....oooOO0OOooo........oooOO0OOooo........oo 174 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 183 175 184 G4double << 176 G4double G4LivermorePhotoElectricModel::CrossSectionPerVolume( 185 G4LivermorePhotoElectricModel::CrossSectionPer << 177 const G4Material* material, 186 << 178 const G4ParticleDefinition* p, 187 << 179 G4double energy, 188 G4double, G4double) << 180 G4double, G4double) 189 { 181 { 190 fCurrSection = 0.0; 182 fCurrSection = 0.0; 191 if (fWater && (material == fWater || materia << 183 if(fWater && (material == fWater || 192 if (energy <= fWaterEnergyLimit) { << 184 material->GetBaseMaterial() == fWater)) { >> 185 if(energy <= fWaterEnergyLimit) { 193 fWater->GetSandiaTable()->GetSandiaCofWa 186 fWater->GetSandiaTable()->GetSandiaCofWater(energy, fSandiaCof); 194 187 195 G4double energy2 = energy * energy; << 188 G4double energy2 = energy*energy; 196 G4double energy3 = energy * energy2; << 189 G4double energy3 = energy*energy2; 197 G4double energy4 = energy2 * energy2; << 190 G4double energy4 = energy2*energy2; 198 << 191 199 fCurrSection = material->GetDensity() << 192 fCurrSection = material->GetDensity()* 200 * (fSandiaCof[0] / energy << 193 (fSandiaCof[0]/energy + fSandiaCof[1]/energy2 + 201 fSandiaCof[2] / energy3 + fSandiaCof[3] << 194 fSandiaCof[2]/energy3 + fSandiaCof[3]/energy4); 202 } << 195 } 203 } 196 } 204 if (0.0 == fCurrSection) { << 197 if(0.0 == fCurrSection) { 205 fCurrSection = G4VEmModel::CrossSectionPer 198 fCurrSection = G4VEmModel::CrossSectionPerVolume(material, p, energy); 206 } 199 } 207 return fCurrSection; 200 return fCurrSection; 208 } 201 } 209 202 210 //....oooOO0OOooo........oooOO0OOooo........oo 203 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 211 204 212 G4double << 205 G4double G4LivermorePhotoElectricModel::ComputeCrossSectionPerAtom( 213 G4LivermorePhotoElectricModel::ComputeCrossSec << 206 const G4ParticleDefinition*, 214 << 207 G4double energy, 215 G4double ZZ, G4double, << 208 G4double ZZ, G4double, 216 G4double, G4double) << 209 G4double, G4double) 217 { 210 { 218 if (verboseLevel > 3) { 211 if (verboseLevel > 3) { 219 G4cout << "\n G4LivermorePhotoElectricMode << 212 G4cout << "G4LivermorePhotoElectricModel::ComputeCrossSectionPerAtom():" 220 << " Z= " << ZZ << " R(keV)= " << << 213 << " Z= " << ZZ << " R(keV)= " << energy/keV << G4endl; 221 } 214 } 222 G4double cs = 0.0; 215 G4double cs = 0.0; 223 G4int Z = G4lrint(ZZ); 216 G4int Z = G4lrint(ZZ); 224 if (Z >= ZMAXPE || Z <= 0) { << 217 if(Z < 1 || Z >= maxZ) { return cs; } 225 return cs; << 226 } << 227 // if element was not initialised << 228 218 >> 219 // if element was not initialised 229 // do initialisation safely for MT mode 220 // do initialisation safely for MT mode 230 if (fCrossSection->GetElementData(Z) == null << 221 if(!fCrossSection[Z]) { 231 InitialiseOnFly(Z); << 222 InitialiseForElement(0, Z); 232 if (fCrossSection->GetElementData(Z) == nu << 223 if(!fCrossSection[Z]) { return cs; } 233 } << 224 } 234 << 225 235 // 7: rows in the parameterization file; 5: << 226 G4int idx = fNShells[Z]*6 - 4; 236 G4int idx = fNShells[Z] * 7 - 5; << 227 if (energy < (*(fParam[Z]))[idx-1]) { energy = (*(fParam[Z]))[idx-1]; } 237 << 228 238 energy = std::max(energy, (*(fParamHigh[Z])) << 229 G4double x1 = 1.0/energy; 239 << 230 G4double x2 = x1*x1; 240 G4double x1 = 1.0 / energy; << 231 G4double x3 = x2*x1; 241 G4double x2 = x1 * x1; << 232 242 G4double x3 = x2 * x1; << 233 // parameterisation 243 << 234 if(energy >= (*(fParam[Z]))[0]) { 244 // high energy parameterisation << 235 G4double x4 = x2*x2; 245 if (energy >= (*(fParamHigh[Z]))[0]) { << 236 cs = x1*((*(fParam[Z]))[idx] + x1*(*(fParam[Z]))[idx+1] 246 G4double x4 = x2 * x2; << 237 + x2*(*(fParam[Z]))[idx+2] + x3*(*(fParam[Z]))[idx+3] 247 G4double x5 = x4 * x1; << 238 + x4*(*(fParam[Z]))[idx+4]); 248 << 239 // high energy part 249 cs = x1 * << 240 } else if(energy >= (*(fParam[Z]))[1]) { 250 ((*(fParamHigh[Z]))[idx] + x1 * (*(fPara << 241 cs = x3*(fCrossSection[Z])->Value(energy); 251 + x2 * (*(fParamHigh[Z]))[idx + 2] + x3 << 242 252 + x4 * (*(fParamHigh[Z]))[idx + 4] + x5 << 243 // low energy part 253 } << 244 } else { 254 // low energy parameterisation << 245 cs = x3*(fCrossSectionLE[Z])->Value(energy); 255 else if (energy >= (*(fParamLow[Z]))[0]) { << 246 } 256 G4double x4 = x2 * x2; << 247 if (verboseLevel > 1) { 257 G4double x5 = x4 * x1; // this variable u << 248 G4cout << "LivermorePhotoElectricModel: E(keV)= " << energy/keV 258 cs = x1 * << 249 << " Z= " << Z << " cross(barn)= " << cs/barn << G4endl; 259 ((*(fParamLow[Z]))[idx] + x1 * (*(fParam << 260 + x2 * (*(fParamLow[Z]))[idx + 2] + x3 << 261 + x4 * (*(fParamLow[Z]))[idx + 4] + x5 << 262 } << 263 // Tabulated values above k-shell ionization << 264 else if (energy >= (*(fParamHigh[Z]))[1]) { << 265 cs = x3 * (fCrossSection->GetElementData(Z << 266 } << 267 // Tabulated values below k-shell ionization << 268 else { << 269 cs = x3 * (fCrossSectionLE->GetElementData << 270 } << 271 if (verboseLevel > 1) { << 272 G4cout << "G4LivermorePhotoElectricModel: << 273 << " cross(barn)= " << cs / barn << << 274 } 250 } 275 return cs; 251 return cs; 276 } 252 } 277 253 278 //....oooOO0OOooo........oooOO0OOooo........oo 254 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 279 255 280 void G4LivermorePhotoElectricModel::SampleSeco << 256 void 281 << 257 G4LivermorePhotoElectricModel::SampleSecondaries( 282 << 258 std::vector<G4DynamicParticle*>* fvect, 283 << 259 const G4MaterialCutsCouple* couple, >> 260 const G4DynamicParticle* aDynamicGamma, >> 261 G4double, >> 262 G4double) 284 { 263 { 285 G4double gammaEnergy = aDynamicGamma->GetKin 264 G4double gammaEnergy = aDynamicGamma->GetKineticEnergy(); 286 if (verboseLevel > 3) { 265 if (verboseLevel > 3) { 287 G4cout << "G4LivermorePhotoElectricModel:: 266 G4cout << "G4LivermorePhotoElectricModel::SampleSecondaries() Egamma(keV)= " 288 << gammaEnergy / keV << G4endl; << 267 << gammaEnergy/keV << G4endl; 289 } 268 } 290 << 269 291 // kill incident photon 270 // kill incident photon 292 fParticleChange->ProposeTrackStatus(fStopAnd << 271 fParticleChange->ProposeTrackStatus(fStopAndKill); 293 fParticleChange->SetProposedKineticEnergy(0. 272 fParticleChange->SetProposedKineticEnergy(0.); 294 273 295 // low-energy photo-effect in water - full a 274 // low-energy photo-effect in water - full absorption 296 const G4Material* material = couple->GetMate 275 const G4Material* material = couple->GetMaterial(); 297 if (fWater && (material == fWater || materia << 276 if(fWater && (material == fWater || 298 if (gammaEnergy <= fWaterEnergyLimit) { << 277 material->GetBaseMaterial() == fWater)) { 299 fParticleChange->ProposeLocalEnergyDepos << 278 if(gammaEnergy <= fWaterEnergyLimit) { >> 279 fParticleChange->ProposeLocalEnergyDeposit(gammaEnergy); 300 return; 280 return; 301 } 281 } 302 } 282 } 303 << 283 304 // Returns the normalized direction of the m 284 // Returns the normalized direction of the momentum 305 G4ThreeVector photonDirection = aDynamicGamm << 285 G4ThreeVector photonDirection = aDynamicGamma->GetMomentumDirection(); 306 286 307 // Select randomly one element in the curren 287 // Select randomly one element in the current material >> 288 //G4cout << "Select random atom Egamma(keV)= " << gammaEnergy/keV << G4endl; 308 const G4Element* elm = SelectRandomAtom(mate 289 const G4Element* elm = SelectRandomAtom(material, theGamma, gammaEnergy); 309 G4int Z = elm->GetZasInt(); << 290 G4int Z = G4lrint(elm->GetZ()); 310 291 311 // Select the ionised shell in the current a << 292 // Select the ionised shell in the current atom according to shell 312 // cross sections << 293 // cross sections >> 294 // G4cout << "Select random shell Z= " << Z << G4endl; 313 295 314 // If element was not initialised gamma shou << 296 if(Z >= maxZ) { Z = maxZ-1; } 315 if (Z >= ZMAXPE || fCrossSection->GetElement << 297 >> 298 // element was not initialised gamma should be absorbed >> 299 if(!fCrossSection[Z]) { 316 fParticleChange->ProposeLocalEnergyDeposit 300 fParticleChange->ProposeLocalEnergyDeposit(gammaEnergy); 317 return; 301 return; 318 } 302 } 319 << 303 320 // SAMPLING OF THE SHELL INDEX << 304 // shell index 321 std::size_t shellIdx = 0; << 305 size_t shellIdx = 0; 322 std::size_t nn = fNShellsUsed[Z]; << 306 size_t nn = fNShellsUsed[Z]; 323 if (nn > 1) { << 307 324 if (gammaEnergy >= (*(fParamHigh[Z]))[0]) << 308 if(nn > 1) { 325 G4double x1 = 1.0 / gammaEnergy; << 309 if(gammaEnergy >= (*(fParam[Z]))[0]) { 326 G4double x2 = x1 * x1; << 310 G4double x1 = 1.0/gammaEnergy; 327 G4double x3 = x2 * x1; << 311 G4double x2 = x1*x1; 328 G4double x4 = x3 * x1; << 312 G4double x3 = x2*x1; 329 G4double x5 = x4 * x1; << 313 G4double x4 = x3*x1; 330 std::size_t idx = nn * 7 - 5; << 314 G4int idx = nn*6 - 4; 331 // when do sampling common factors are n 315 // when do sampling common factors are not taken into account 332 // so cross section is not real 316 // so cross section is not real 333 << 317 G4double cs0 = G4UniformRand()*((*(fParam[Z]))[idx] 334 G4double rand = G4UniformRand(); << 318 + x1*(*(fParam[Z]))[idx+1] 335 G4double cs0 = rand * << 319 + x2*(*(fParam[Z]))[idx+2] 336 ((*(fParamHigh[Z]))[idx] + x1 * (*(fPa << 320 + x3*(*(fParam[Z]))[idx+3] 337 + x2 * (*(fParamHigh[Z]))[idx + 2] + x << 321 + x4*(*(fParam[Z]))[idx+4]); 338 + x4 * (*(fParamHigh[Z]))[idx + 4] + x << 322 for(shellIdx=0; shellIdx<nn; ++shellIdx) { 339 << 323 idx = shellIdx*6 + 2; 340 for (shellIdx = 0; shellIdx < nn; ++shel << 324 if(gammaEnergy > (*(fParam[Z]))[idx-1]) { 341 idx = shellIdx * 7 + 2; << 325 G4double cs = (*(fParam[Z]))[idx] + x1*(*(fParam[Z]))[idx+1] 342 if (gammaEnergy > (*(fParamHigh[Z]))[i << 326 + x2*(*(fParam[Z]))[idx+2] + x3*(*(fParam[Z]))[idx+3] 343 G4double cs = (*(fParamHigh[Z]))[idx << 327 + x4*(*(fParam[Z]))[idx+4]; 344 + x2 * (*(fParamHigh[Z]))[idx + 2] << 328 if(cs >= cs0) { break; } 345 + x4 * (*(fParamHigh[Z]))[idx + 4] << 329 } 346 << 347 if (cs >= cs0) { << 348 break; << 349 } << 350 } << 351 } << 352 if (shellIdx >= nn) { << 353 shellIdx = nn - 1; << 354 } << 355 } << 356 else if (gammaEnergy >= (*(fParamLow[Z]))[ << 357 G4double x1 = 1.0 / gammaEnergy; << 358 G4double x2 = x1 * x1; << 359 G4double x3 = x2 * x1; << 360 G4double x4 = x3 * x1; << 361 G4double x5 = x4 * x1; << 362 std::size_t idx = nn * 7 - 5; << 363 // when do sampling common factors are n << 364 // so cross section is not real << 365 G4double cs0 = G4UniformRand() * << 366 ((*(fParamLow[Z]))[idx] + x1 * (*(fPar << 367 + x2 * (*(fParamLow[Z]))[idx + 2] + x3 << 368 + x4 * (*(fParamLow[Z]))[idx + 4] + x5 << 369 for (shellIdx = 0; shellIdx < nn; ++shel << 370 idx = shellIdx * 7 + 2; << 371 if (gammaEnergy > (*(fParamLow[Z]))[id << 372 G4double cs = (*(fParamLow[Z]))[idx] << 373 + x2 * (*(fParamLow[Z]))[idx + 2] << 374 + x4 * (*(fParamLow[Z]))[idx + 4] << 375 if (cs >= cs0) { << 376 break; << 377 } << 378 } << 379 } << 380 if (shellIdx >= nn) { << 381 shellIdx = nn - 1; << 382 } 330 } 383 } << 331 if(shellIdx >= nn) { shellIdx = nn-1; } 384 else { << 332 >> 333 } else { >> 334 385 // when do sampling common factors are n 335 // when do sampling common factors are not taken into account 386 // so cross section is not real 336 // so cross section is not real 387 G4double cs = G4UniformRand(); 337 G4double cs = G4UniformRand(); 388 338 389 if (gammaEnergy >= (*(fParamHigh[Z]))[1] << 339 if(gammaEnergy >= (*(fParam[Z]))[1]) { 390 // above K-shell binding energy << 340 cs *= (fCrossSection[Z])->Value(gammaEnergy); 391 cs *= fCrossSection->GetElementData(Z) << 341 } else { 392 } << 342 cs *= (fCrossSectionLE[Z])->Value(gammaEnergy); 393 else { << 394 // below K-shell binding energy << 395 cs *= fCrossSectionLE->GetElementData( << 396 } 343 } 397 344 398 for (G4int j = 0; j < (G4int)nn; ++j) { << 345 for(size_t j=0; j<nn; ++j) { 399 shellIdx = (std::size_t)fCrossSection- << 346 shellIdx = (size_t)fShellCrossSection->GetComponentID(Z, j); 400 if (gammaEnergy > (*(fParamLow[Z]))[7 << 347 if(gammaEnergy > (*(fParam[Z]))[6*shellIdx+1]) { 401 cs -= fCrossSection->GetValueForComp << 348 cs -= fShellCrossSection->GetValueForComponent(Z, j, gammaEnergy); 402 } << 349 } 403 if (cs <= 0.0 || j + 1 == (G4int)nn) { << 350 if(cs <= 0.0 || j+1 == nn) { break; } 404 break; << 405 } << 406 } 351 } 407 } 352 } 408 } 353 } 409 // END: SAMPLING OF THE SHELL << 410 354 411 G4double bindingEnergy = (*(fParamHigh[Z]))[ << 355 G4double bindingEnergy = (*(fParam[Z]))[shellIdx*6 + 1]; 412 const G4AtomicShell* shell = nullptr; << 356 //G4cout << "Z= " << Z << " shellIdx= " << shellIdx >> 357 // << " nShells= " << fNShells[Z] >> 358 // << " Ebind(keV)= " << bindingEnergy/keV >> 359 // << " Egamma(keV)= " << gammaEnergy/keV << G4endl; >> 360 >> 361 const G4AtomicShell* shell = 0; 413 362 414 // no de-excitation from the last shell 363 // no de-excitation from the last shell 415 if (fDeexcitationActive && shellIdx + 1 < nn << 364 if(fDeexcitationActive && shellIdx + 1 < nn) { 416 auto as = G4AtomicShellEnumerator(shellIdx << 365 G4AtomicShellEnumerator as = G4AtomicShellEnumerator(shellIdx); 417 shell = fAtomDeexcitation->GetAtomicShell( 366 shell = fAtomDeexcitation->GetAtomicShell(Z, as); 418 } 367 } 419 368 420 // If binding energy of the selected shell i 369 // If binding energy of the selected shell is larger than photon energy 421 // do not generate secondaries 370 // do not generate secondaries 422 if (gammaEnergy < bindingEnergy) { << 371 if(gammaEnergy < bindingEnergy) { 423 fParticleChange->ProposeLocalEnergyDeposit 372 fParticleChange->ProposeLocalEnergyDeposit(gammaEnergy); 424 return; 373 return; 425 } 374 } 426 375 427 // Primary outcoming electron 376 // Primary outcoming electron 428 G4double eKineticEnergy = gammaEnergy - bind 377 G4double eKineticEnergy = gammaEnergy - bindingEnergy; 429 G4double edep = bindingEnergy; 378 G4double edep = bindingEnergy; 430 379 431 // Calculate direction of the photoelectron 380 // Calculate direction of the photoelectron 432 G4ThreeVector electronDirection = GetAngular << 381 G4ThreeVector electronDirection = 433 aDynamicGamma, eKineticEnergy, (G4int)shel << 382 GetAngularDistribution()->SampleDirection(aDynamicGamma, 434 << 383 eKineticEnergy, 435 // The electron is created << 384 shellIdx, 436 auto electron = << 385 couple->GetMaterial()); 437 new G4DynamicParticle(theElectron, electro << 386 >> 387 // The electron is created >> 388 G4DynamicParticle* electron = new G4DynamicParticle (theElectron, >> 389 electronDirection, >> 390 eKineticEnergy); 438 fvect->push_back(electron); 391 fvect->push_back(electron); 439 392 440 // Sample deexcitation 393 // Sample deexcitation 441 if (nullptr != shell) { << 394 if(shell) { 442 G4int index = couple->GetIndex(); 395 G4int index = couple->GetIndex(); 443 if (fAtomDeexcitation->CheckDeexcitationAc << 396 if(fAtomDeexcitation->CheckDeexcitationActiveRegion(index)) { 444 std::size_t nbefore = fvect->size(); << 397 G4int nbefore = fvect->size(); 445 398 446 fAtomDeexcitation->GenerateParticles(fve 399 fAtomDeexcitation->GenerateParticles(fvect, shell, Z, index); 447 std::size_t nafter = fvect->size(); << 400 G4int nafter = fvect->size(); 448 if (nafter > nbefore) { << 401 if(nafter > nbefore) { 449 G4double esec = 0.0; << 402 G4double esec = 0.0; 450 for (std::size_t j = nbefore; j < naft << 403 for (G4int j=nbefore; j<nafter; ++j) { 451 G4double e = ((*fvect)[j])->GetKinet << 404 452 if (esec + e > edep) { << 405 G4double e = ((*fvect)[j])->GetKineticEnergy(); 453 // correct energy in order to have << 406 if(esec + e > edep) { 454 e = edep - esec; << 407 // correct energy in order to have energy balance 455 ((*fvect)[j])->SetKineticEnergy(e) << 408 e = edep - esec; 456 esec += e; << 409 ((*fvect)[j])->SetKineticEnergy(e); 457 // delete the rest of secondaries << 410 esec += e; 458 for (std::size_t jj = nafter - 1; << 411 // delete the rest of secondaries (should not happens) 459 delete (*fvect)[jj]; << 412 for (G4int jj=nafter-1; jj>j; --jj) { 460 fvect->pop_back(); << 413 delete (*fvect)[jj]; 461 } << 414 fvect->pop_back(); 462 break; << 415 } 463 } << 416 break; 464 esec += e; << 417 } 465 } << 418 esec += e; >> 419 } 466 edep -= esec; 420 edep -= esec; 467 } 421 } 468 } 422 } 469 } 423 } 470 // energy balance - excitation energy left 424 // energy balance - excitation energy left 471 if (edep > 0.0) { << 425 if(edep > 0.0) { 472 fParticleChange->ProposeLocalEnergyDeposit 426 fParticleChange->ProposeLocalEnergyDeposit(edep); 473 } 427 } 474 } 428 } 475 429 476 //....oooOO0OOooo........oooOO0OOooo........oo 430 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 477 431 478 const G4String& G4LivermorePhotoElectricModel: << 432 void >> 433 G4LivermorePhotoElectricModel::ReadData(G4int Z, const char* path) 479 { 434 { 480 // no check in this method - environment var << 435 if (verboseLevel > 1) 481 if (fDataDirectory.empty()) { << 436 { 482 auto param = G4EmParameters::Instance(); << 437 G4cout << "Calling ReadData() of G4LivermoreGammaConversionModel" 483 std::ostringstream ost; << 438 << G4endl; 484 if (param->LivermoreDataDir() == "livermor << 485 ost << param->GetDirLEDATA() << "/liverm << 486 } << 487 else { << 488 ost << param->GetDirLEDATA() << "/epics2 << 489 } << 490 fDataDirectory = ost.str(); << 491 } << 492 return fDataDirectory; << 493 } << 494 << 495 //....oooOO0OOooo........oooOO0OOooo........oo << 496 << 497 void G4LivermorePhotoElectricModel::ReadData(G << 498 { << 499 if (Z <= 0 || Z >= ZMAXPE) { << 500 G4cout << "G4LivermorePhotoElectricModel:: << 501 << Z << " is out of range - request ignor << 502 return; << 503 } << 504 if (verboseLevel > 1) { << 505 G4cout << "G4LivermorePhotoElectricModel:: << 506 } 439 } 507 440 508 if (fCrossSection->GetElementData(Z) != null << 441 if(fCrossSection[Z]) { return; } 509 return; << 442 >> 443 const char* datadir = path; >> 444 >> 445 if(!datadir) >> 446 { >> 447 datadir = getenv("G4LEDATA"); >> 448 if(!datadir) >> 449 { >> 450 G4Exception("G4LivermorePhotoElectricModel::ReadData()", >> 451 "em0006",FatalException, >> 452 "Environment variable G4LEDATA not defined"); >> 453 return; >> 454 } 510 } 455 } 511 456 512 // spline for photoeffect total x-section ab << 457 // spline for photoeffect total x-section above K-shell 513 // but below the parameterized ones << 458 fCrossSection[Z] = new G4LPhysicsFreeVector(); 514 << 459 fCrossSection[Z]->SetSpline(true); 515 G4bool spline = (G4EmParameters::Instance()- << 516 G4int number = G4EmParameters::Instance()->N << 517 auto pv = new G4PhysicsFreeVector(spline); << 518 460 519 // fDataDirectory will be defined after thes << 520 std::ostringstream ost; 461 std::ostringstream ost; 521 ost << FindDirectoryPath() << "pe-cs-" << Z << 462 ost << datadir << "/livermore/phot/pe-cs-" << Z <<".dat"; 522 std::ifstream fin(ost.str().c_str()); 463 std::ifstream fin(ost.str().c_str()); 523 if (!fin.is_open()) { << 464 if( !fin.is_open()) { 524 G4ExceptionDescription ed; 465 G4ExceptionDescription ed; 525 ed << "G4LivermorePhotoElectricModel data << 466 ed << "G4LivermorePhotoElectricModel data file <" << ost.str().c_str() 526 << ost.str().c_str() << "> is not opene << 467 << "> is not opened!" << G4endl; 527 G4Exception("G4LivermorePhotoElectricModel << 468 G4Exception("G4LivermorePhotoElectricModel::ReadData()", 528 "G4LEDATA version should be G4 << 469 "em0003",FatalException, >> 470 ed,"G4LEDATA version should be G4EMLOW6.32 or later."); 529 return; 471 return; >> 472 } else { >> 473 if(verboseLevel > 3) { G4cout << "File " << ost.str().c_str() >> 474 << " is opened by G4LivermorePhotoElectricModel" << G4endl;} >> 475 fCrossSection[Z]->Retrieve(fin, true); >> 476 fCrossSection[Z]->ScaleVector(MeV, barn); >> 477 fin.close(); 530 } 478 } 531 if (verboseLevel > 3) { << 532 G4cout << "File " << ost.str().c_str() << << 533 << G4endl; << 534 } << 535 pv->Retrieve(fin, true); << 536 pv->ScaleVector(MeV, barn); << 537 pv->FillSecondDerivatives(); << 538 pv->EnableLogBinSearch(number); << 539 fCrossSection->InitialiseForElement(Z, pv); << 540 fin.close(); << 541 479 542 // read high-energy fit parameters << 480 fParam[Z] = new std::vector<G4double>; 543 fParamHigh[Z] = new std::vector<G4double>; << 481 >> 482 // read fit parameters 544 G4int n1 = 0; 483 G4int n1 = 0; 545 G4int n2 = 0; 484 G4int n2 = 0; 546 G4double x; 485 G4double x; 547 std::ostringstream ost1; 486 std::ostringstream ost1; 548 ost1 << fDataDirectory << "pe-high-" << Z << << 487 ost1 << datadir << "/livermore/phot/pe-" << Z <<".dat"; 549 std::ifstream fin1(ost1.str().c_str()); 488 std::ifstream fin1(ost1.str().c_str()); 550 if (!fin1.is_open()) { << 489 if( !fin1.is_open()) { 551 G4ExceptionDescription ed; << 552 ed << "G4LivermorePhotoElectricModel data << 553 << ost1.str().c_str() << "> is not open << 554 G4Exception("G4LivermorePhotoElectricModel << 555 "G4LEDATA version should be G4 << 556 return; << 557 } << 558 if (verboseLevel > 3) { << 559 G4cout << "File " << ost1.str().c_str() << << 560 << G4endl; << 561 } << 562 fin1 >> n1; << 563 if (fin1.fail()) { << 564 return; << 565 } << 566 if (0 > n1 || n1 >= INT_MAX) { << 567 n1 = 0; << 568 } << 569 << 570 fin1 >> n2; << 571 if (fin1.fail()) { << 572 return; << 573 } << 574 if (0 > n2 || n2 >= INT_MAX) { << 575 n2 = 0; << 576 } << 577 << 578 fin1 >> x; << 579 if (fin1.fail()) { << 580 return; << 581 } << 582 << 583 fNShells[Z] = n1; << 584 fParamHigh[Z]->reserve(7 * n1 + 1); << 585 fParamHigh[Z]->push_back(x * MeV); << 586 for (G4int i = 0; i < n1; ++i) { << 587 for (G4int j = 0; j < 7; ++j) { << 588 fin1 >> x; << 589 if (0 == j) { << 590 x *= MeV; << 591 } << 592 else { << 593 x *= barn; << 594 } << 595 fParamHigh[Z]->push_back(x); << 596 } << 597 } << 598 fin1.close(); << 599 << 600 // read low-energy fit parameters << 601 fParamLow[Z] = new std::vector<G4double>; << 602 G4int n1_low = 0; << 603 G4int n2_low = 0; << 604 G4double x_low; << 605 std::ostringstream ost1_low; << 606 ost1_low << fDataDirectory << "pe-low-" << Z << 607 std::ifstream fin1_low(ost1_low.str().c_str( << 608 if (!fin1_low.is_open()) { << 609 G4ExceptionDescription ed; 490 G4ExceptionDescription ed; 610 ed << "G4LivermorePhotoElectricModel data << 491 ed << "G4LivermorePhotoElectricModel data file <" << ost1.str().c_str() 611 << "> is not opened!" << G4endl; 492 << "> is not opened!" << G4endl; 612 G4Exception("G4LivermorePhotoElectricModel << 493 G4Exception("G4LivermorePhotoElectricModel::ReadData()", 613 "G4LEDATA version should be G4 << 494 "em0003",FatalException, 614 return; << 495 ed,"G4LEDATA version should be G4EMLOW6.32 or later."); 615 } << 496 return; 616 if (verboseLevel > 3) { << 497 } else { 617 G4cout << "File " << ost1_low.str().c_str( << 498 if(verboseLevel > 3) { 618 << G4endl; << 499 G4cout << "File " << ost1.str().c_str() 619 } << 500 << " is opened by G4LivermorePhotoElectricModel" << G4endl; 620 fin1_low >> n1_low; << 501 } 621 if (fin1_low.fail()) { << 502 fin1 >> n1; 622 return; << 503 if(fin1.fail()) { return; } 623 } << 504 if(0 > n1 || n1 >= INT_MAX) { n1 = 0; } 624 if (0 > n1_low || n1_low >= INT_MAX) { << 505 625 n1_low = 0; << 506 fin1 >> n2; 626 } << 507 if(fin1.fail()) { return; } 627 << 508 if(0 > n2 || n2 >= INT_MAX) { n2 = 0; } 628 fin1_low >> n2_low; << 509 629 if (fin1_low.fail()) { << 510 fin1 >> x; 630 return; << 511 if(fin1.fail()) { return; } 631 } << 512 632 if (0 > n2_low || n2_low >= INT_MAX) { << 513 fNShells[Z] = n1; 633 n2_low = 0; << 514 fParam[Z]->reserve(6*n1+1); 634 } << 515 fParam[Z]->push_back(x*MeV); 635 << 516 for(G4int i=0; i<n1; ++i) { 636 fin1_low >> x_low; << 517 for(G4int j=0; j<6; ++j) { 637 if (fin1_low.fail()) { << 518 fin1 >> x; 638 return; << 519 if(0 == j) { x *= MeV; } 639 } << 520 else { x *= barn; } 640 << 521 fParam[Z]->push_back(x); 641 fNShells[Z] = n1_low; << 522 } 642 fParamLow[Z]->reserve(7 * n1_low + 1); << 523 } 643 fParamLow[Z]->push_back(x_low * MeV); << 524 fin1.close(); 644 for (G4int i = 0; i < n1_low; ++i) { << 525 } 645 for (G4int j = 0; j < 7; ++j) { << 526 // there is a possibility to used only main shells 646 fin1_low >> x_low; << 527 if(nShellLimit < n2) { n2 = nShellLimit; } 647 if (0 == j) { << 528 fShellCrossSection->InitialiseForComponent(Z, n2); 648 x_low *= MeV; << 649 } << 650 else { << 651 x_low *= barn; << 652 } << 653 fParamLow[Z]->push_back(x_low); << 654 } << 655 } << 656 fin1_low.close(); << 657 << 658 // there is a possibility to use only main s << 659 if (nShellLimit < n2) { << 660 n2 = nShellLimit; << 661 } << 662 fCrossSection->InitialiseForComponent(Z, n2) << 663 fNShellsUsed[Z] = n2; 529 fNShellsUsed[Z] = n2; 664 530 665 if (1 < n2) { << 531 if(1 < n2) { 666 std::ostringstream ost2; 532 std::ostringstream ost2; 667 ost2 << fDataDirectory << "pe-ss-cs-" << Z << 533 ost2 << datadir << "/livermore/phot/pe-ss-cs-" << Z <<".dat"; 668 std::ifstream fin2(ost2.str().c_str()); 534 std::ifstream fin2(ost2.str().c_str()); 669 if (!fin2.is_open()) { << 535 if( !fin2.is_open()) { 670 G4ExceptionDescription ed; 536 G4ExceptionDescription ed; 671 ed << "G4LivermorePhotoElectricModel dat << 537 ed << "G4LivermorePhotoElectricModel data file <" << ost2.str().c_str() 672 << G4endl; << 538 << "> is not opened!" << G4endl; 673 G4Exception("G4LivermorePhotoElectricMod << 539 G4Exception("G4LivermorePhotoElectricModel::ReadData()", 674 "G4LEDATA version should be << 540 "em0003",FatalException, >> 541 ed,"G4LEDATA version should be G4EMLOW6.32 or later."); 675 return; 542 return; 676 } << 543 } else { 677 if (verboseLevel > 3) { << 544 if(verboseLevel > 3) { 678 G4cout << "File " << ost2.str().c_str() << 545 G4cout << "File " << ost2.str().c_str() 679 << G4endl; << 546 << " is opened by G4LivermorePhotoElectricModel" << G4endl; 680 } << 547 } 681 548 682 G4int n3, n4; << 549 G4int n3, n4; 683 G4double y; << 550 G4double y; 684 for (G4int i = 0; i < n2; ++i) { << 551 for(G4int i=0; i<n2; ++i) { 685 fin2 >> x >> y >> n3 >> n4; << 552 fin2 >> x >> y >> n3 >> n4; 686 auto v = new G4PhysicsFreeVector(n3, x, << 553 G4LPhysicsFreeVector* v = new G4LPhysicsFreeVector(n3, x, y); 687 for (G4int j = 0; j < n3; ++j) { << 554 for(G4int j=0; j<n3; ++j) { 688 fin2 >> x >> y; << 555 fin2 >> x >> y; 689 v->PutValues(j, x * CLHEP::MeV, y * CL << 556 v->PutValues(j, x*MeV, y*barn); >> 557 } >> 558 fShellCrossSection->AddComponent(Z, n4, v); 690 } 559 } 691 v->EnableLogBinSearch(number); << 560 fin2.close(); 692 fCrossSection->AddComponent(Z, n4, v); << 693 } 561 } 694 fin2.close(); << 695 } 562 } 696 563 697 // no spline for photoeffect total x-section 564 // no spline for photoeffect total x-section below K-shell 698 if (1 < fNShells[Z]) { << 565 if(1 < fNShells[Z]) { 699 auto pv1 = new G4PhysicsFreeVector(false); << 566 fCrossSectionLE[Z] = new G4LPhysicsFreeVector(); >> 567 700 std::ostringstream ost3; 568 std::ostringstream ost3; 701 ost3 << fDataDirectory << "pe-le-cs-" << Z << 569 ost3 << datadir << "/livermore/phot/pe-le-cs-" << Z <<".dat"; 702 std::ifstream fin3(ost3.str().c_str()); 570 std::ifstream fin3(ost3.str().c_str()); 703 if (!fin3.is_open()) { << 571 if( !fin3.is_open()) { 704 G4ExceptionDescription ed; 572 G4ExceptionDescription ed; 705 ed << "G4LivermorePhotoElectricModel dat << 573 ed << "G4LivermorePhotoElectricModel data file <" << ost3.str().c_str() 706 << G4endl; << 574 << "> is not opened!" << G4endl; 707 G4Exception("G4LivermorePhotoElectricMod << 575 G4Exception("G4LivermorePhotoElectricModel::ReadData()", 708 "G4LEDATA version should be << 576 "em0003",FatalException, >> 577 ed,"G4LEDATA version should be G4EMLOW6.32 or later."); 709 return; 578 return; >> 579 } else { >> 580 if(verboseLevel > 3) { >> 581 G4cout << "File " << ost3.str().c_str() >> 582 << " is opened by G4LivermorePhotoElectricModel" << G4endl; >> 583 } >> 584 fCrossSectionLE[Z]->Retrieve(fin3, true); >> 585 fCrossSectionLE[Z]->ScaleVector(MeV, barn); >> 586 fin3.close(); 710 } 587 } 711 if (verboseLevel > 3) { << 712 G4cout << "File " << ost3.str().c_str() << 713 << G4endl; << 714 } << 715 pv1->Retrieve(fin3, true); << 716 pv1->ScaleVector(CLHEP::MeV, CLHEP::barn); << 717 pv1->EnableLogBinSearch(number); << 718 fCrossSectionLE->InitialiseForElement(Z, p << 719 fin3.close(); << 720 } << 721 } << 722 << 723 //....oooOO0OOooo........oooOO0OOooo........oo << 724 << 725 G4double G4LivermorePhotoElectricModel::GetBin << 726 { << 727 if (Z < 1 || Z >= ZMAXPE) { << 728 return -1; << 729 } // If Z is out of the supported return 0 << 730 << 731 InitialiseOnFly(Z); << 732 if (fCrossSection->GetElementData(Z) == null << 733 shell < 0 || shell >= fNShellsUsed[Z]) { << 734 return -1; << 735 } << 736 << 737 if (Z > 2) { << 738 return fCrossSection->GetComponentDataByIn << 739 } << 740 else { << 741 return fCrossSection->GetElementData(Z)->E << 742 } 588 } 743 } 589 } 744 590 745 //....oooOO0OOooo........oooOO0OOooo........oo 591 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 746 592 747 void << 593 #include "G4AutoLock.hh" 748 G4LivermorePhotoElectricModel::InitialiseForEl << 594 namespace { G4Mutex LivermorePhotoElectricModelMutex = G4MUTEX_INITIALIZER; } 749 { << 750 if (fCrossSection == nullptr) { << 751 fCrossSection = new G4ElementData(ZMAXPE); << 752 fCrossSection->SetName("PhotoEffXS"); << 753 fCrossSectionLE = new G4ElementData(ZMAXPE << 754 fCrossSectionLE->SetName("PhotoEffLowXS"); << 755 } << 756 ReadData(Z); << 757 } << 758 << 759 //....oooOO0OOooo........oooOO0OOooo........oo << 760 595 761 void G4LivermorePhotoElectricModel::Initialise << 596 void G4LivermorePhotoElectricModel::InitialiseForElement( >> 597 const G4ParticleDefinition*, G4int Z) 762 { 598 { 763 if (fCrossSection->GetElementData(Z) == null << 599 G4AutoLock l(&LivermorePhotoElectricModelMutex); 764 G4AutoLock l(&livPhotoeffMutex); << 600 // G4cout << "G4LivermorePhotoElectricModel::InitialiseForElement Z= " 765 if (fCrossSection->GetElementData(Z) == nu << 601 // << Z << G4endl; 766 ReadData(Z); << 602 if(!fCrossSection[Z]) { ReadData(Z); } 767 } << 603 l.unlock(); 768 l.unlock(); << 769 } << 770 } 604 } 771 605 772 //....oooOO0OOooo........oooOO0OOooo........oo 606 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 773 607