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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 // 26 // 27 // 27 // 28 // G4PAIySection.cc -- class implementation fi 28 // G4PAIySection.cc -- class implementation file 29 // 29 // 30 // GEANT 4 class implementation file 30 // GEANT 4 class implementation file 31 // 31 // 32 // For information related to this code, pleas 32 // For information related to this code, please, contact 33 // the Geant4 Collaboration. 33 // the Geant4 Collaboration. 34 // 34 // 35 // R&D: Vladimir.Grichine@cern.ch 35 // R&D: Vladimir.Grichine@cern.ch 36 // 36 // 37 // History: 37 // History: 38 // 38 // 39 // 01.10.07, V.Ivanchenko create using V.Grich 39 // 01.10.07, V.Ivanchenko create using V.Grichine G4PAIxSection class 40 // 26.07.09, V.Ivanchenko added protection for 40 // 26.07.09, V.Ivanchenko added protection for mumerical exceptions for 41 // low-density materials 41 // low-density materials 42 // 21.11.10 V. Grichine bug fixed in Initialis 42 // 21.11.10 V. Grichine bug fixed in Initialise for reading sandia table from 43 // material. Warning: the table is 43 // material. Warning: the table is tuned for photo-effect not PAI model. 44 // 23.06.13 V.Grichine arrays->G4DataVectors 44 // 23.06.13 V.Grichine arrays->G4DataVectors 45 // 45 // 46 46 47 #include "G4PAIySection.hh" 47 #include "G4PAIySection.hh" 48 48 49 #include "globals.hh" 49 #include "globals.hh" 50 #include "G4PhysicalConstants.hh" 50 #include "G4PhysicalConstants.hh" 51 #include "G4SystemOfUnits.hh" 51 #include "G4SystemOfUnits.hh" 52 #include "G4ios.hh" 52 #include "G4ios.hh" 53 #include "G4Poisson.hh" 53 #include "G4Poisson.hh" 54 #include "G4Material.hh" 54 #include "G4Material.hh" 55 #include "G4MaterialCutsCouple.hh" 55 #include "G4MaterialCutsCouple.hh" 56 #include "G4SandiaTable.hh" 56 #include "G4SandiaTable.hh" 57 #include "G4Exp.hh" 57 #include "G4Exp.hh" 58 #include "G4Log.hh" 58 #include "G4Log.hh" 59 59 60 using namespace std; 60 using namespace std; 61 61 62 // Local class constants 62 // Local class constants 63 63 64 const G4double G4PAIySection::fDelta = 0.005; 64 const G4double G4PAIySection::fDelta = 0.005; // energy shift from interval border 65 const G4double G4PAIySection::fError = 0.005; 65 const G4double G4PAIySection::fError = 0.005; // error in lin-log approximation 66 66 67 const G4int G4PAIySection::fMaxSplineSize = 50 67 const G4int G4PAIySection::fMaxSplineSize = 500; // Max size of output spline 68 68 // arrays 69 69 70 ////////////////////////////////////////////// 70 ////////////////////////////////////////////////////////////////// 71 // 71 // 72 // Constructor 72 // Constructor 73 // 73 // 74 74 75 G4PAIySection::G4PAIySection() 75 G4PAIySection::G4PAIySection() 76 { 76 { 77 fSandia = nullptr; 77 fSandia = nullptr; 78 fDensity = fElectronDensity = fNormalization 78 fDensity = fElectronDensity = fNormalizationCof = fLowEnergyCof = 0.0; 79 fIntervalNumber = fSplineNumber = 0; 79 fIntervalNumber = fSplineNumber = 0; 80 fVerbose = 0; 80 fVerbose = 0; 81 81 82 betaBohr = fine_structure_const; 82 betaBohr = fine_structure_const; 83 G4double cofBetaBohr = 4.0; 83 G4double cofBetaBohr = 4.0; 84 G4double betaBohr2 = fine_structure_const*fi << 84 G4double betaBohr2 = fine_structure_const*fine_structure_const; 85 betaBohr4 = betaBohr2*betaBohr2*cofBetaBohr; << 85 betaBohr4 = betaBohr2*betaBohr2*cofBetaBohr; 86 86 87 fSplineEnergy = G4DataVector(fMaxSp 87 fSplineEnergy = G4DataVector(fMaxSplineSize,0.0); 88 fRePartDielectricConst = G4DataVector(fMaxSp 88 fRePartDielectricConst = G4DataVector(fMaxSplineSize,0.0); 89 fImPartDielectricConst = G4DataVector(fMaxSp 89 fImPartDielectricConst = G4DataVector(fMaxSplineSize,0.0); 90 fIntegralTerm = G4DataVector(fMaxSp 90 fIntegralTerm = G4DataVector(fMaxSplineSize,0.0); 91 fDifPAIySection = G4DataVector(fMaxSp 91 fDifPAIySection = G4DataVector(fMaxSplineSize,0.0); 92 fdNdxCerenkov = G4DataVector(fMaxSp 92 fdNdxCerenkov = G4DataVector(fMaxSplineSize,0.0); 93 fdNdxPlasmon = G4DataVector(fMaxSp 93 fdNdxPlasmon = G4DataVector(fMaxSplineSize,0.0); 94 fIntegralPAIySection = G4DataVector(fMaxSp 94 fIntegralPAIySection = G4DataVector(fMaxSplineSize,0.0); 95 fIntegralPAIdEdx = G4DataVector(fMaxSp 95 fIntegralPAIdEdx = G4DataVector(fMaxSplineSize,0.0); 96 fIntegralCerenkov = G4DataVector(fMaxSp 96 fIntegralCerenkov = G4DataVector(fMaxSplineSize,0.0); 97 fIntegralPlasmon = G4DataVector(fMaxSp 97 fIntegralPlasmon = G4DataVector(fMaxSplineSize,0.0); 98 98 99 for( G4int i = 0; i < 500; ++i ) 99 for( G4int i = 0; i < 500; ++i ) 100 { 100 { 101 for( G4int j = 0; j < 112; ++j ) { fPAItab 101 for( G4int j = 0; j < 112; ++j ) { fPAItable[i][j] = 0.0; } 102 } 102 } 103 } 103 } 104 104 105 ////////////////////////////////////////////// 105 //////////////////////////////////////////////////////////////////////////// 106 // 106 // 107 // 107 // 108 108 109 G4double G4PAIySection::GetLorentzFactor(G4int 109 G4double G4PAIySection::GetLorentzFactor(G4int j) const 110 { 110 { 111 return fLorentzFactor[j]; 111 return fLorentzFactor[j]; 112 } 112 } 113 113 114 ////////////////////////////////////////////// 114 //////////////////////////////////////////////////////////////////////// 115 // 115 // 116 // Constructor with beta*gamma square value ca 116 // Constructor with beta*gamma square value called from G4PAIModel 117 117 118 void G4PAIySection::Initialize( const G4Materi 118 void G4PAIySection::Initialize( const G4Material* material, 119 G4double maxEn 119 G4double maxEnergyTransfer, 120 G4double betaG 120 G4double betaGammaSq, 121 G4SandiaTable* 121 G4SandiaTable* sandia) 122 { 122 { 123 if(fVerbose > 0) 123 if(fVerbose > 0) 124 { 124 { 125 G4cout<<G4endl; 125 G4cout<<G4endl; 126 G4cout<<"G4PAIySection::Initialize(...,G4S 126 G4cout<<"G4PAIySection::Initialize(...,G4SandiaTable* sandia)"<<G4endl; 127 G4cout<<G4endl; 127 G4cout<<G4endl; 128 } 128 } 129 G4int i, j; 129 G4int i, j; 130 130 131 fSandia = sandia; 131 fSandia = sandia; 132 fIntervalNumber = sandia->GetMaxInterval(); 132 fIntervalNumber = sandia->GetMaxInterval(); 133 fDensity = material->GetDensity(); 133 fDensity = material->GetDensity(); 134 fElectronDensity = material->GetElectronDens 134 fElectronDensity = material->GetElectronDensity(); 135 135 136 // fIntervalNumber--; 136 // fIntervalNumber--; 137 137 138 if( fVerbose > 0 ) 138 if( fVerbose > 0 ) 139 { 139 { 140 G4cout<<"fDensity = "<<fDensity<<"\t"<<fEl 140 G4cout<<"fDensity = "<<fDensity<<"\t"<<fElectronDensity<<"\t fIntervalNumber = " 141 <<fIntervalNumber<< " (beta*gamma)^2 141 <<fIntervalNumber<< " (beta*gamma)^2= " << betaGammaSq << G4endl; 142 } 142 } 143 fEnergyInterval = G4DataVector(fIntervalNumb 143 fEnergyInterval = G4DataVector(fIntervalNumber+2,0.0); 144 fA1 = G4DataVector(fIntervalNumb 144 fA1 = G4DataVector(fIntervalNumber+2,0.0); 145 fA2 = G4DataVector(fIntervalNumb 145 fA2 = G4DataVector(fIntervalNumber+2,0.0); 146 fA3 = G4DataVector(fIntervalNumb 146 fA3 = G4DataVector(fIntervalNumber+2,0.0); 147 fA4 = G4DataVector(fIntervalNumb 147 fA4 = G4DataVector(fIntervalNumber+2,0.0); 148 148 149 for( i = 1; i <= fIntervalNumber; ++i ) 149 for( i = 1; i <= fIntervalNumber; ++i ) 150 { 150 { 151 if ( sandia->GetSandiaMatTablePAI(i-1,0) < 151 if ( sandia->GetSandiaMatTablePAI(i-1,0) < 1.*eV ) 152 { 152 { 153 fIntervalNumber--; 153 fIntervalNumber--; 154 continue; 154 continue; 155 } 155 } 156 if( ( sandia->GetSandiaMatTablePAI(i-1,0) 156 if( ( sandia->GetSandiaMatTablePAI(i-1,0) >= maxEnergyTransfer ) 157 || i >= fIntervalNumber ) 157 || i >= fIntervalNumber ) 158 { 158 { 159 fEnergyInterval[i] = maxEnergyTransfer; 159 fEnergyInterval[i] = maxEnergyTransfer; 160 fIntervalNumber = i; 160 fIntervalNumber = i; 161 break; 161 break; 162 } 162 } 163 fEnergyInterval[i] = sandia->GetSandiaMatT 163 fEnergyInterval[i] = sandia->GetSandiaMatTablePAI(i-1,0); 164 fA1[i] = sandia->GetSandiaMatT 164 fA1[i] = sandia->GetSandiaMatTablePAI(i-1,1); 165 fA2[i] = sandia->GetSandiaMatT 165 fA2[i] = sandia->GetSandiaMatTablePAI(i-1,2); 166 fA3[i] = sandia->GetSandiaMatT 166 fA3[i] = sandia->GetSandiaMatTablePAI(i-1,3); 167 fA4[i] = sandia->GetSandiaMatT 167 fA4[i] = sandia->GetSandiaMatTablePAI(i-1,4); 168 168 169 if( fVerbose > 0 ) { 169 if( fVerbose > 0 ) { 170 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< 170 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t" 171 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4en 171 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; 172 } 172 } 173 } 173 } 174 if( fVerbose > 0 ) { 174 if( fVerbose > 0 ) { 175 G4cout<<"last i = "<<i<<"; "<<"fIntervalNu 175 G4cout<<"last i = "<<i<<"; "<<"fIntervalNumber = " 176 <<fIntervalNumber<<G4endl; 176 <<fIntervalNumber<<G4endl; 177 } 177 } 178 if( fEnergyInterval[fIntervalNumber] != maxE 178 if( fEnergyInterval[fIntervalNumber] != maxEnergyTransfer ) 179 { 179 { 180 fIntervalNumber++; 180 fIntervalNumber++; 181 fEnergyInterval[fIntervalNumber] = maxEn 181 fEnergyInterval[fIntervalNumber] = maxEnergyTransfer; 182 } 182 } 183 if( fVerbose > 0 ) 183 if( fVerbose > 0 ) 184 { 184 { 185 for( i = 1; i <= fIntervalNumber; ++i ) 185 for( i = 1; i <= fIntervalNumber; ++i ) 186 { 186 { 187 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< 187 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t" 188 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; 188 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; 189 } 189 } 190 } 190 } 191 if( fVerbose > 0 ) { 191 if( fVerbose > 0 ) { 192 G4cout<<"Now checking, if two borders are 192 G4cout<<"Now checking, if two borders are too close together"<<G4endl; 193 } 193 } 194 for( i = 1; i < fIntervalNumber; ++i ) 194 for( i = 1; i < fIntervalNumber; ++i ) 195 { 195 { 196 if( fEnergyInterval[i+1]-fEnergyInterval[i 196 if( fEnergyInterval[i+1]-fEnergyInterval[i] > 197 1.5*fDelta*(fEnergyInterval[i+1]+fEne 197 1.5*fDelta*(fEnergyInterval[i+1]+fEnergyInterval[i]) ) continue; 198 else 198 else 199 { 199 { 200 for( j = i; j < fIntervalNumber; j++ ) 200 for( j = i; j < fIntervalNumber; j++ ) 201 { 201 { 202 fEnergyInterval[j] = fEnergyInte 202 fEnergyInterval[j] = fEnergyInterval[j+1]; 203 fA1[j] = fA1[j+1]; 203 fA1[j] = fA1[j+1]; 204 fA2[j] = fA2[j+1]; 204 fA2[j] = fA2[j+1]; 205 fA3[j] = fA3[j+1]; 205 fA3[j] = fA3[j+1]; 206 fA4[j] = fA4[j+1]; 206 fA4[j] = fA4[j+1]; 207 } 207 } 208 fIntervalNumber--; 208 fIntervalNumber--; 209 } 209 } 210 } 210 } 211 if( fVerbose > 0 ) 211 if( fVerbose > 0 ) 212 { 212 { 213 for( i = 1; i <= fIntervalNumber; ++i ) 213 for( i = 1; i <= fIntervalNumber; ++i ) 214 { 214 { 215 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV< 215 G4cout<<i<<"\t"<<fEnergyInterval[i]/keV<<"\t"<<fA1[i]<<"\t"<<fA2[i]<<"\t" 216 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; 216 <<fA3[i]<<"\t"<<fA4[i]<<"\t"<<G4endl; 217 } 217 } 218 } 218 } 219 // Preparation of fSplineEnergy array corres 219 // Preparation of fSplineEnergy array corresponding to min ionisation, G~4 220 220 221 ComputeLowEnergyCof(material); 221 ComputeLowEnergyCof(material); 222 222 223 G4double betaGammaSqRef = 223 G4double betaGammaSqRef = 224 fLorentzFactor[fRefGammaNumber]*fLorentzFa 224 fLorentzFactor[fRefGammaNumber]*fLorentzFactor[fRefGammaNumber] - 1; 225 225 226 NormShift(betaGammaSqRef); 226 NormShift(betaGammaSqRef); 227 SplainPAI(betaGammaSqRef); 227 SplainPAI(betaGammaSqRef); 228 228 229 // Preparation of integral PAI cross section 229 // Preparation of integral PAI cross section for input betaGammaSq 230 230 231 for( i = 1; i <= fSplineNumber; ++i ) 231 for( i = 1; i <= fSplineNumber; ++i ) 232 { 232 { 233 fDifPAIySection[i] = DifPAIySection(i,bet 233 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq); 234 234 235 if( fVerbose > 0 ) G4cout<<i<<"; dNdxPAI 235 if( fVerbose > 0 ) G4cout<<i<<"; dNdxPAI = "<<fDifPAIySection[i]<<G4endl; 236 } 236 } 237 IntegralPAIySection(); 237 IntegralPAIySection(); 238 } 238 } 239 239 240 ////////////////////////////////////////////// 240 ///////////////////////////////////////////////////////////////////////// 241 // 241 // 242 // Compute low energy cof. It reduces PAI xsc 242 // Compute low energy cof. It reduces PAI xsc for Lorentz factors less than 4. 243 // 243 // 244 244 245 void G4PAIySection::ComputeLowEnergyCof(const 245 void G4PAIySection::ComputeLowEnergyCof(const G4Material* material) 246 { 246 { 247 G4int i, numberOfElements = (G4int)material- 247 G4int i, numberOfElements = (G4int)material->GetNumberOfElements(); 248 G4double sumZ = 0., sumCof = 0.; 248 G4double sumZ = 0., sumCof = 0.; 249 249 250 static const G4double p0 = 1.20923e+00; 250 static const G4double p0 = 1.20923e+00; 251 static const G4double p1 = 3.53256e-01; 251 static const G4double p1 = 3.53256e-01; 252 static const G4double p2 = -1.45052e-03; 252 static const G4double p2 = -1.45052e-03; 253 253 254 G4double* thisMaterialZ = new G4double[num 254 G4double* thisMaterialZ = new G4double[numberOfElements]; 255 G4double* thisMaterialCof = new G4double[num 255 G4double* thisMaterialCof = new G4double[numberOfElements]; 256 256 257 for( i = 0; i < numberOfElements; ++i ) 257 for( i = 0; i < numberOfElements; ++i ) 258 { 258 { 259 thisMaterialZ[i] = material->GetElement(i) 259 thisMaterialZ[i] = material->GetElement(i)->GetZ(); 260 sumZ += thisMaterialZ[i]; 260 sumZ += thisMaterialZ[i]; 261 thisMaterialCof[i] = p0+p1*thisMaterialZ[i 261 thisMaterialCof[i] = p0+p1*thisMaterialZ[i]+p2*thisMaterialZ[i]*thisMaterialZ[i]; 262 } 262 } 263 for( i = 0; i < numberOfElements; ++i ) 263 for( i = 0; i < numberOfElements; ++i ) 264 { 264 { 265 sumCof += thisMaterialCof[i]*thisMaterialZ 265 sumCof += thisMaterialCof[i]*thisMaterialZ[i]/sumZ; 266 } 266 } 267 fLowEnergyCof = sumCof; 267 fLowEnergyCof = sumCof; 268 delete [] thisMaterialZ; 268 delete [] thisMaterialZ; 269 delete [] thisMaterialCof; 269 delete [] thisMaterialCof; 270 // G4cout<<"fLowEnergyCof = "<<fLowEnergyCof 270 // G4cout<<"fLowEnergyCof = "<<fLowEnergyCof<<G4endl; 271 } 271 } 272 272 273 ////////////////////////////////////////////// 273 ///////////////////////////////////////////////////////////////////////// 274 // 274 // 275 // General control function for class G4PAIySe 275 // General control function for class G4PAIySection 276 // 276 // 277 277 278 void G4PAIySection::InitPAI() 278 void G4PAIySection::InitPAI() 279 { 279 { 280 G4int i; 280 G4int i; 281 G4double betaGammaSq = fLorentzFactor[fRefG 281 G4double betaGammaSq = fLorentzFactor[fRefGammaNumber]* 282 fLorentzFactor[fRefG 282 fLorentzFactor[fRefGammaNumber] - 1; 283 283 284 // Preparation of integral PAI cross sectio 284 // Preparation of integral PAI cross section for reference gamma 285 285 286 NormShift(betaGammaSq); 286 NormShift(betaGammaSq); 287 SplainPAI(betaGammaSq); 287 SplainPAI(betaGammaSq); 288 288 289 IntegralPAIySection(); 289 IntegralPAIySection(); 290 IntegralCerenkov(); 290 IntegralCerenkov(); 291 IntegralPlasmon(); 291 IntegralPlasmon(); 292 292 293 for( i = 0; i<= fSplineNumber; ++i) 293 for( i = 0; i<= fSplineNumber; ++i) 294 { 294 { 295 fPAItable[i][fRefGammaNumber] = fIntegral 295 fPAItable[i][fRefGammaNumber] = fIntegralPAIySection[i]; 296 296 297 if(i != 0) fPAItable[i][0] = fSplineEner 297 if(i != 0) fPAItable[i][0] = fSplineEnergy[i]; 298 } 298 } 299 fPAItable[0][0] = fSplineNumber; 299 fPAItable[0][0] = fSplineNumber; 300 300 301 for( G4int j = 1; j < 112; ++j) // fo 301 for( G4int j = 1; j < 112; ++j) // for other gammas 302 { 302 { 303 if( j == fRefGammaNumber ) continue; 303 if( j == fRefGammaNumber ) continue; 304 304 305 betaGammaSq = fLorentzFactor[j]*fLorentz 305 betaGammaSq = fLorentzFactor[j]*fLorentzFactor[j] - 1; 306 306 307 for(i = 1; i <= fSplineNumber; ++i) 307 for(i = 1; i <= fSplineNumber; ++i) 308 { 308 { 309 fDifPAIySection[i] = DifPAIySection(i 309 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq); 310 fdNdxCerenkov[i] = PAIdNdxCerenkov( 310 fdNdxCerenkov[i] = PAIdNdxCerenkov(i,betaGammaSq); 311 fdNdxPlasmon[i] = PAIdNdxPlasmon(i 311 fdNdxPlasmon[i] = PAIdNdxPlasmon(i,betaGammaSq); 312 } 312 } 313 IntegralPAIySection(); 313 IntegralPAIySection(); 314 IntegralCerenkov(); 314 IntegralCerenkov(); 315 IntegralPlasmon(); 315 IntegralPlasmon(); 316 316 317 for(i = 0; i <= fSplineNumber; ++i) 317 for(i = 0; i <= fSplineNumber; ++i) 318 { 318 { 319 fPAItable[i][j] = fIntegralPAIySection 319 fPAItable[i][j] = fIntegralPAIySection[i]; 320 } 320 } 321 } 321 } 322 } 322 } 323 323 324 ////////////////////////////////////////////// 324 /////////////////////////////////////////////////////////////////////// 325 // 325 // 326 // Shifting from borders to intervals Creation 326 // Shifting from borders to intervals Creation of first energy points 327 // 327 // 328 328 329 void G4PAIySection::NormShift(G4double betaGam 329 void G4PAIySection::NormShift(G4double betaGammaSq) 330 { 330 { 331 G4int i, j; 331 G4int i, j; 332 332 333 for( i = 1; i <= fIntervalNumber-1; ++i) 333 for( i = 1; i <= fIntervalNumber-1; ++i) 334 { 334 { 335 for( j = 1; j <= 2; ++j) 335 for( j = 1; j <= 2; ++j) 336 { 336 { 337 fSplineNumber = (i-1)*2 + j; 337 fSplineNumber = (i-1)*2 + j; 338 338 339 if( j == 1 ) fSplineEnergy[fSplineNumber 339 if( j == 1 ) fSplineEnergy[fSplineNumber] = fEnergyInterval[i ]*(1+fDelta); 340 else fSplineEnergy[fSplineNumber 340 else fSplineEnergy[fSplineNumber] = fEnergyInterval[i+1]*(1-fDelta); 341 // G4cout<<"cn = "<<fSplineNumber<<"; 341 // G4cout<<"cn = "<<fSplineNumber<<"; "<<"energy = " 342 // <<fSplineEnergy[fSplineNumber]<<G4en 342 // <<fSplineEnergy[fSplineNumber]<<G4endl; 343 } 343 } 344 } 344 } 345 fIntegralTerm[1]=RutherfordIntegral(1,fEnerg 345 fIntegralTerm[1]=RutherfordIntegral(1,fEnergyInterval[1],fSplineEnergy[1]); 346 346 347 j = 1; 347 j = 1; 348 348 349 for(i=2;i<=fSplineNumber;++i) 349 for(i=2;i<=fSplineNumber;++i) 350 { 350 { 351 if(fSplineEnergy[i]<fEnergyInterval[j+1]) 351 if(fSplineEnergy[i]<fEnergyInterval[j+1]) 352 { 352 { 353 fIntegralTerm[i] = fIntegralTerm[i-1] 353 fIntegralTerm[i] = fIntegralTerm[i-1] + 354 RutherfordIntegral 354 RutherfordIntegral(j,fSplineEnergy[i-1], 355 355 fSplineEnergy[i] ); 356 } 356 } 357 else 357 else 358 { 358 { 359 G4double x = RutherfordIntegral(j,fSpli 359 G4double x = RutherfordIntegral(j,fSplineEnergy[i-1], 360 fEn 360 fEnergyInterval[j+1] ); 361 j++; 361 j++; 362 fIntegralTerm[i] = fIntegralTerm[i-1] 362 fIntegralTerm[i] = fIntegralTerm[i-1] + x + 363 RutherfordIntegral 363 RutherfordIntegral(j,fEnergyInterval[j], 364 364 fSplineEnergy[i] ); 365 } 365 } 366 // G4cout<<i<<"\t"<<fSplineEnergy[i]<<"\t" 366 // G4cout<<i<<"\t"<<fSplineEnergy[i]<<"\t"<<fIntegralTerm[i]<<"\n"<<G4endl; 367 } 367 } 368 static const G4double nfactor = 368 static const G4double nfactor = 369 2*pi*pi*hbarc*hbarc*fine_structure_const/e 369 2*pi*pi*hbarc*hbarc*fine_structure_const/electron_mass_c2; 370 fNormalizationCof = nfactor*fElectronDensity 370 fNormalizationCof = nfactor*fElectronDensity/fIntegralTerm[fSplineNumber]; 371 371 372 // G4cout<<"fNormalizationCof = "<<fNormaliz 372 // G4cout<<"fNormalizationCof = "<<fNormalizationCof<<G4endl; 373 373 374 // Calculation of PAI differrential cross-se << 374 // Calculation of PAI differrential cross-section (1/(keV*cm)) 375 // in the energy points near borders of ener << 375 // in the energy points near borders of energy intervals 376 376 377 for(G4int k=1; k<=fIntervalNumber-1; ++k) << 377 for(G4int k=1; k<=fIntervalNumber-1; ++k) 378 { 378 { 379 for(j=1; j<=2; ++j) << 379 for(j=1; j<=2; ++j) 380 { 380 { 381 i = (k-1)*2 + j; 381 i = (k-1)*2 + j; 382 fImPartDielectricConst[i] = fNormaliz 382 fImPartDielectricConst[i] = fNormalizationCof* 383 ImPartDie 383 ImPartDielectricConst(k,fSplineEnergy[i]); 384 fRePartDielectricConst[i] = fNormaliz 384 fRePartDielectricConst[i] = fNormalizationCof* 385 RePartDie 385 RePartDielectricConst(fSplineEnergy[i]); 386 fIntegralTerm[i] *= fNormalizationCof 386 fIntegralTerm[i] *= fNormalizationCof; 387 387 388 fDifPAIySection[i] = DifPAIySection(i 388 fDifPAIySection[i] = DifPAIySection(i,betaGammaSq); 389 fdNdxCerenkov[i] = PAIdNdxCerenkov( 389 fdNdxCerenkov[i] = PAIdNdxCerenkov(i,betaGammaSq); 390 fdNdxPlasmon[i] = PAIdNdxPlasmon(i 390 fdNdxPlasmon[i] = PAIdNdxPlasmon(i,betaGammaSq); 391 } 391 } 392 } 392 } 393 393 394 } // end of NormShift 394 } // end of NormShift 395 395 396 ////////////////////////////////////////////// 396 ///////////////////////////////////////////////////////////////////////// 397 // 397 // 398 // Creation of new energy points as geometrica 398 // Creation of new energy points as geometrical mean of existing 399 // one, calculation PAI_cs for them, while the 399 // one, calculation PAI_cs for them, while the error of logarithmic 400 // linear approximation would be smaller than 400 // linear approximation would be smaller than 'fError' 401 401 402 void G4PAIySection::SplainPAI(G4double betaGam 402 void G4PAIySection::SplainPAI(G4double betaGammaSq) 403 { 403 { 404 G4int k = 1; 404 G4int k = 1; 405 G4int i = 1; 405 G4int i = 1; 406 406 407 while ( (i < fSplineNumber) && (fSplineNumb 407 while ( (i < fSplineNumber) && (fSplineNumber < fMaxSplineSize-1) ) 408 { 408 { 409 if(fSplineEnergy[i+1] > fEnergyInterval[ 409 if(fSplineEnergy[i+1] > fEnergyInterval[k+1]) 410 { 410 { 411 k++; // Here next energy point is 411 k++; // Here next energy point is in next energy interval 412 ++i; 412 ++i; 413 continue; 413 continue; 414 } 414 } 415 // Shifting of arrayes for inserting the << 415 // Shifting of arrayes for inserting the geometrical 416 // average of 'i' and 'i+1' energy point << 416 // average of 'i' and 'i+1' energy points to 'i+1' place 417 fSplineNumber++; 417 fSplineNumber++; 418 418 419 for(G4int j = fSplineNumber; j >= i+2; j 419 for(G4int j = fSplineNumber; j >= i+2; j-- ) 420 { 420 { 421 fSplineEnergy[j] = fSplineEn 421 fSplineEnergy[j] = fSplineEnergy[j-1]; 422 fImPartDielectricConst[j] = fImPartDi 422 fImPartDielectricConst[j] = fImPartDielectricConst[j-1]; 423 fRePartDielectricConst[j] = fRePartDi 423 fRePartDielectricConst[j] = fRePartDielectricConst[j-1]; 424 fIntegralTerm[j] = fIntegral 424 fIntegralTerm[j] = fIntegralTerm[j-1]; 425 425 426 fDifPAIySection[j] = fDifPAIySection[ 426 fDifPAIySection[j] = fDifPAIySection[j-1]; 427 fdNdxCerenkov[j] = fdNdxCerenkov[j- 427 fdNdxCerenkov[j] = fdNdxCerenkov[j-1]; 428 fdNdxPlasmon[j] = fdNdxPlasmon[j-1 428 fdNdxPlasmon[j] = fdNdxPlasmon[j-1]; 429 } 429 } 430 G4double x1 = fSplineEnergy[i]; 430 G4double x1 = fSplineEnergy[i]; 431 G4double x2 = fSplineEnergy[i+1]; 431 G4double x2 = fSplineEnergy[i+1]; 432 G4double yy1 = fDifPAIySection[i]; 432 G4double yy1 = fDifPAIySection[i]; 433 G4double y2 = fDifPAIySection[i+1]; 433 G4double y2 = fDifPAIySection[i+1]; 434 434 435 G4double en1 = sqrt(x1*x2); 435 G4double en1 = sqrt(x1*x2); 436 fSplineEnergy[i+1] = en1; 436 fSplineEnergy[i+1] = en1; 437 437 438 // Calculation of logarithmic linear app << 438 // Calculation of logarithmic linear approximation 439 // in this (enr) energy point, which num << 439 // in this (enr) energy point, which number is 'i+1' now 440 440 441 G4double a = log10(y2/yy1)/log10(x2/x1); 441 G4double a = log10(y2/yy1)/log10(x2/x1); 442 G4double b = log10(yy1) - a*log10(x1); 442 G4double b = log10(yy1) - a*log10(x1); 443 G4double y = a*log10(en1) + b; 443 G4double y = a*log10(en1) + b; 444 y = pow(10.,y); 444 y = pow(10.,y); 445 445 446 // Calculation of the PAI dif. cross-sec << 446 // Calculation of the PAI dif. cross-section at this point 447 447 448 fImPartDielectricConst[i+1] = fNormaliza 448 fImPartDielectricConst[i+1] = fNormalizationCof* 449 ImPartDiel 449 ImPartDielectricConst(k,fSplineEnergy[i+1]); 450 fRePartDielectricConst[i+1] = fNormaliza 450 fRePartDielectricConst[i+1] = fNormalizationCof* 451 RePartDiel 451 RePartDielectricConst(fSplineEnergy[i+1]); 452 fIntegralTerm[i+1] = fIntegralTerm[i] + 452 fIntegralTerm[i+1] = fIntegralTerm[i] + fNormalizationCof* 453 RutherfordIntegral( 453 RutherfordIntegral(k,fSplineEnergy[i], 454 454 fSplineEnergy[i+1]); 455 455 456 fDifPAIySection[i+1] = DifPAIySection(i+ 456 fDifPAIySection[i+1] = DifPAIySection(i+1,betaGammaSq); 457 fdNdxCerenkov[i+1] = PAIdNdxCerenkov(i 457 fdNdxCerenkov[i+1] = PAIdNdxCerenkov(i+1,betaGammaSq); 458 fdNdxPlasmon[i+1] = PAIdNdxPlasmon(i+ 458 fdNdxPlasmon[i+1] = PAIdNdxPlasmon(i+1,betaGammaSq); 459 459 460 // Condition for next divisi 460 // Condition for next division of this segment or to pass 461 // to higher energies 461 // to higher energies 462 462 463 G4double x = 2*(fDifPAIySection[i+1] - y 463 G4double x = 2*(fDifPAIySection[i+1] - y)/(fDifPAIySection[i+1] + y); 464 464 465 G4double delta = 2.*(fSplineEnergy[i+1]- 465 G4double delta = 2.*(fSplineEnergy[i+1]-fSplineEnergy[i]) 466 /(fSplineEnergy[i+1]+fSplineEnergy[i]) 466 /(fSplineEnergy[i+1]+fSplineEnergy[i]); 467 467 468 if( x < 0 ) 468 if( x < 0 ) 469 { 469 { 470 x = -x; 470 x = -x; 471 } 471 } 472 if( x > fError && fSplineNumber < fMaxSp 472 if( x > fError && fSplineNumber < fMaxSplineSize-1 && delta > 2.*fDelta ) 473 { 473 { 474 continue; // next division 474 continue; // next division 475 } 475 } 476 i += 2; // pass to next segment 476 i += 2; // pass to next segment 477 477 478 // Loop checking, 03-Aug-2015, Vladimir 478 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko 479 } // close 'while' 479 } // close 'while' 480 480 481 } // end of SplainPAI 481 } // end of SplainPAI 482 482 483 483 484 ////////////////////////////////////////////// 484 //////////////////////////////////////////////////////////////////// 485 // 485 // 486 // Integration over electrons that could be co 486 // Integration over electrons that could be considered 487 // quasi-free at energy transfer of interest 487 // quasi-free at energy transfer of interest 488 488 489 G4double G4PAIySection::RutherfordIntegral( G4 489 G4double G4PAIySection::RutherfordIntegral( G4int k, 490 G4 490 G4double x1, 491 491 G4double x2 ) 492 { 492 { 493 G4double c1, c2, c3; 493 G4double c1, c2, c3; 494 // G4cout<<"RI: x1 = "<<x1<<"; "<<"x2 = "<< 494 // G4cout<<"RI: x1 = "<<x1<<"; "<<"x2 = "<<x2<<G4endl; 495 G4double x12 = x1*x2; 495 G4double x12 = x1*x2; 496 c1 = (x2 - x1)/x12; 496 c1 = (x2 - x1)/x12; 497 c2 = (x2 - x1)*(x2 + x1)/(x12*x12); 497 c2 = (x2 - x1)*(x2 + x1)/(x12*x12); 498 c3 = (x2 - x1)*(x1*x1 + x1*x2 + x2*x2)/(x12 498 c3 = (x2 - x1)*(x1*x1 + x1*x2 + x2*x2)/(x12*x12*x12); 499 // G4cout<<" RI: c1 = "<<c1<<"; "<<"c2 = "< 499 // G4cout<<" RI: c1 = "<<c1<<"; "<<"c2 = "<<c2<<"; "<<"c3 = "<<c3<<G4endl; 500 500 501 return fA1[k]*log(x2/x1) + fA2[k]*c1 + fA3 501 return fA1[k]*log(x2/x1) + fA2[k]*c1 + fA3[k]*c2/2 + fA4[k]*c3/3; 502 502 503 } // end of RutherfordIntegral 503 } // end of RutherfordIntegral 504 504 505 505 506 ////////////////////////////////////////////// 506 ///////////////////////////////////////////////////////////////// 507 // 507 // 508 // Imaginary part of dielectric constant 508 // Imaginary part of dielectric constant 509 // (G4int k - interval number, G4double en1 - 509 // (G4int k - interval number, G4double en1 - energy point) 510 510 511 G4double G4PAIySection::ImPartDielectricConst( << 511 G4double G4PAIySection::ImPartDielectricConst( G4int k , >> 512 G4double energy1 ) 512 { 513 { 513 G4double energy2,energy3,energy4,result; 514 G4double energy2,energy3,energy4,result; 514 515 515 energy2 = energy1*energy1; 516 energy2 = energy1*energy1; 516 energy3 = energy2*energy1; 517 energy3 = energy2*energy1; 517 energy4 = energy3*energy1; 518 energy4 = energy3*energy1; 518 519 519 result = fA1[k]/energy1+fA2[k]/energy2+fA3[ 520 result = fA1[k]/energy1+fA2[k]/energy2+fA3[k]/energy3+fA4[k]/energy4; 520 result *=hbarc/energy1; 521 result *=hbarc/energy1; 521 522 522 return result; 523 return result; 523 524 524 } // end of ImPartDielectricConst 525 } // end of ImPartDielectricConst 525 526 526 527 527 ////////////////////////////////////////////// 528 ////////////////////////////////////////////////////////////////////////////// 528 // 529 // 529 // Real part of dielectric constant minus unit 530 // Real part of dielectric constant minus unit: epsilon_1 - 1 530 // (G4double enb - energy point) 531 // (G4double enb - energy point) 531 // 532 // 532 533 533 G4double G4PAIySection::RePartDielectricConst( 534 G4double G4PAIySection::RePartDielectricConst(G4double enb) 534 { 535 { 535 G4double x0, x02, x03, x04, x05, x1, x2, xx 536 G4double x0, x02, x03, x04, x05, x1, x2, xx1 ,xx2 , xx12, 536 c1, c2, c3, cof1, cof2, xln1, xln2 537 c1, c2, c3, cof1, cof2, xln1, xln2, xln3, result; 537 538 538 x0 = enb; 539 x0 = enb; 539 result = 0; 540 result = 0; 540 541 541 for(G4int i=1;i<=fIntervalNumber-1;++i) 542 for(G4int i=1;i<=fIntervalNumber-1;++i) 542 { 543 { 543 x1 = fEnergyInterval[i]; 544 x1 = fEnergyInterval[i]; 544 x2 = fEnergyInterval[i+1]; 545 x2 = fEnergyInterval[i+1]; 545 xx1 = x1 - x0; 546 xx1 = x1 - x0; 546 xx2 = x2 - x0; 547 xx2 = x2 - x0; 547 xx12 = xx2/xx1; 548 xx12 = xx2/xx1; 548 549 549 if(xx12<0.) << 550 if(xx12<0) 550 { 551 { 551 xx12 = -xx12; 552 xx12 = -xx12; 552 } 553 } 553 xln1 = log(x2/x1); 554 xln1 = log(x2/x1); 554 xln2 = log(xx12); 555 xln2 = log(xx12); 555 xln3 = log((x2 + x0)/(x1 + x0)); 556 xln3 = log((x2 + x0)/(x1 + x0)); 556 x02 = x0*x0; 557 x02 = x0*x0; 557 x03 = x02*x0; 558 x03 = x02*x0; 558 x04 = x03*x0; 559 x04 = x03*x0; 559 x05 = x04*x0; 560 x05 = x04*x0; 560 G4double x12 = x1*x2; 561 G4double x12 = x1*x2; 561 c1 = (x2 - x1)/x12; 562 c1 = (x2 - x1)/x12; 562 c2 = (x2 - x1)*(x2 +x1)/(x12*x12); 563 c2 = (x2 - x1)*(x2 +x1)/(x12*x12); 563 c3 = (x2 -x1)*(x1*x1 + x1*x2 + x2*x2)/( 564 c3 = (x2 -x1)*(x1*x1 + x1*x2 + x2*x2)/(x12*x12*x12); 564 565 565 result -= (fA1[i]/x02 + fA3[i]/x04)*xln1 566 result -= (fA1[i]/x02 + fA3[i]/x04)*xln1; 566 result -= (fA2[i]/x02 + fA4[i]/x04)*c1; 567 result -= (fA2[i]/x02 + fA4[i]/x04)*c1; 567 result -= fA3[i]*c2/2/x02; 568 result -= fA3[i]*c2/2/x02; 568 result -= fA4[i]*c3/3/x02; 569 result -= fA4[i]*c3/3/x02; 569 570 570 cof1 = fA1[i]/x02 + fA3[i]/x04; 571 cof1 = fA1[i]/x02 + fA3[i]/x04; 571 cof2 = fA2[i]/x03 + fA4[i]/x05; 572 cof2 = fA2[i]/x03 + fA4[i]/x05; 572 573 573 result += 0.5*(cof1 +cof2)*xln2; 574 result += 0.5*(cof1 +cof2)*xln2; 574 result += 0.5*(cof1 - cof2)*xln3; 575 result += 0.5*(cof1 - cof2)*xln3; 575 } 576 } 576 result *= 2*hbarc/pi; 577 result *= 2*hbarc/pi; 577 578 578 return result; 579 return result; 579 580 580 } // end of RePartDielectricConst 581 } // end of RePartDielectricConst 581 582 582 ////////////////////////////////////////////// 583 ////////////////////////////////////////////////////////////////////// 583 // 584 // 584 // PAI differential cross-section in terms of 585 // PAI differential cross-section in terms of 585 // simplified Allison's equation 586 // simplified Allison's equation 586 // 587 // 587 588 588 G4double G4PAIySection::DifPAIySection( G4int 589 G4double G4PAIySection::DifPAIySection( G4int i , 589 G4doub 590 G4double betaGammaSq ) 590 { 591 { 591 G4double beta, be2,cof,x1,x2,x3,x4,x5,x6,x7 << 592 G4double beta, be2,cof,x1,x2,x3,x4,x5,x6,x7,x8,result; >> 593 //G4double beta, be4; >> 594 //G4double be4; >> 595 // G4double betaBohr2 = fine_structure_const*fine_structure_const; >> 596 // G4double betaBohr4 = betaBohr2*betaBohr2*4.0; 592 be2 = betaGammaSq/(1 + betaGammaSq); 597 be2 = betaGammaSq/(1 + betaGammaSq); 593 beta = std::sqrt(be2); << 598 //be4 = be2*be2; >> 599 beta = sqrt(be2); 594 cof = 1; 600 cof = 1; 595 x1 = log(2*electron_mass_c2/fSplineEnergy[i 601 x1 = log(2*electron_mass_c2/fSplineEnergy[i]); 596 602 597 if( betaGammaSq < 0.01 ) x2 = log(be2); 603 if( betaGammaSq < 0.01 ) x2 = log(be2); 598 else 604 else 599 { 605 { 600 x2 = -log( (1/betaGammaSq - fRePartDielec 606 x2 = -log( (1/betaGammaSq - fRePartDielectricConst[i])* 601 (1/betaGammaSq - fRePartDielec 607 (1/betaGammaSq - fRePartDielectricConst[i]) + 602 fImPartDielectricConst[i]*fImP 608 fImPartDielectricConst[i]*fImPartDielectricConst[i] )/2; 603 } 609 } 604 if( fImPartDielectricConst[i] == 0.0 ||beta 610 if( fImPartDielectricConst[i] == 0.0 ||betaGammaSq < 0.01 ) 605 { 611 { 606 x6=0; 612 x6=0; 607 } 613 } 608 else 614 else 609 { 615 { 610 x3 = -fRePartDielectricConst[i] + 1/betaG 616 x3 = -fRePartDielectricConst[i] + 1/betaGammaSq; 611 x5 = -1 - fRePartDielectricConst[i] + 617 x5 = -1 - fRePartDielectricConst[i] + 612 be2*((1 +fRePartDielectricConst[i])* 618 be2*((1 +fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) + 613 fImPartDielectricConst[i]*fImPartDie 619 fImPartDielectricConst[i]*fImPartDielectricConst[i]); 614 620 615 x7 = std::atan2(fImPartDielectricConst[i] << 621 x7 = atan2(fImPartDielectricConst[i],x3); 616 x6 = x5 * x7; 622 x6 = x5 * x7; 617 } 623 } >> 624 // if(fImPartDielectricConst[i] == 0) x6 = 0; >> 625 618 x4 = ((x1 + x2)*fImPartDielectricConst[i] + 626 x4 = ((x1 + x2)*fImPartDielectricConst[i] + x6)/hbarc; >> 627 // if( x4 < 0.0 ) x4 = 0.0; 619 x8 = (1 + fRePartDielectricConst[i])*(1 + f 628 x8 = (1 + fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) + 620 fImPartDielectricConst[i]*fImPartDiele 629 fImPartDielectricConst[i]*fImPartDielectricConst[i]; 621 630 622 result = (x4 + cof*fIntegralTerm[i]/fSpline 631 result = (x4 + cof*fIntegralTerm[i]/fSplineEnergy[i]/fSplineEnergy[i]); 623 result = std::max(result, 1.0e-8); 632 result = std::max(result, 1.0e-8); 624 result *= fine_structure_const/(be2*pi); << 633 result *= fine_structure_const/be2/pi; 625 // low energy correction 634 // low energy correction 626 635 627 G4double lowCof = fLowEnergyCof; // 6.0 ; / 636 G4double lowCof = fLowEnergyCof; // 6.0 ; // Ar ~ 4.; -> fLowCof as f(Z1,Z2)? 628 637 629 result *= (1 - std::exp(-beta/(betaBohr*low << 638 result *= (1 - exp(-beta/betaBohr/lowCof)); >> 639 >> 640 // result *= (1-exp(-beta/betaBohr))*(1-exp(-beta/betaBohr)); >> 641 // result *= (1-exp(-be2/betaBohr2)); >> 642 // result *= (1-exp(-be4/betaBohr4)); >> 643 // if(fDensity >= 0.1) 630 if(x8 > 0.) 644 if(x8 > 0.) 631 { 645 { 632 result /= x8; << 646 result /= x8; 633 } 647 } 634 return result; 648 return result; 635 649 636 } // end of DifPAIySection 650 } // end of DifPAIySection 637 651 638 ////////////////////////////////////////////// 652 ////////////////////////////////////////////////////////////////////////// 639 // 653 // 640 // Calculation od dN/dx of collisions with cre 654 // Calculation od dN/dx of collisions with creation of Cerenkov pseudo-photons 641 655 642 G4double G4PAIySection::PAIdNdxCerenkov( G4int << 656 G4double G4PAIySection::PAIdNdxCerenkov( G4int i , >> 657 G4double betaGammaSq ) 643 { 658 { 644 G4double logarithm, x3, x5, argument, modul 659 G4double logarithm, x3, x5, argument, modul2, dNdxC; 645 G4double be2, be4; 660 G4double be2, be4; 646 661 >> 662 //G4double cof = 1.0; >> 663 647 be2 = betaGammaSq/(1 + betaGammaSq); 664 be2 = betaGammaSq/(1 + betaGammaSq); 648 be4 = be2*be2; 665 be4 = be2*be2; 649 666 650 if( betaGammaSq < 0.01 ) logarithm = log(1. 667 if( betaGammaSq < 0.01 ) logarithm = log(1.0+betaGammaSq); // 0.0; 651 else 668 else 652 { 669 { 653 logarithm = -std::log( (1/betaGammaSq - f << 670 logarithm = -log( (1/betaGammaSq - fRePartDielectricConst[i])* 654 (1/betaGammaSq - fRePa 671 (1/betaGammaSq - fRePartDielectricConst[i]) + 655 fImPartDielectricConst 672 fImPartDielectricConst[i]*fImPartDielectricConst[i] )*0.5; 656 logarithm += std::log(1+1.0/betaGammaSq); << 673 logarithm += log(1+1.0/betaGammaSq); 657 } 674 } 658 675 659 if( fImPartDielectricConst[i] == 0.0 || bet 676 if( fImPartDielectricConst[i] == 0.0 || betaGammaSq < 0.01 ) 660 { 677 { 661 argument = 0.0; 678 argument = 0.0; 662 } 679 } 663 else 680 else 664 { 681 { 665 x3 = -fRePartDielectricConst[i] + 1.0/bet 682 x3 = -fRePartDielectricConst[i] + 1.0/betaGammaSq; 666 x5 = -1.0 - fRePartDielectricConst[i] + 683 x5 = -1.0 - fRePartDielectricConst[i] + 667 be2*((1.0 +fRePartDielectricConst[i] 684 be2*((1.0 +fRePartDielectricConst[i])*(1.0 + fRePartDielectricConst[i]) + 668 fImPartDielectricConst[i]*fImPartDie 685 fImPartDielectricConst[i]*fImPartDielectricConst[i]); 669 if( x3 == 0.0 ) argument = 0.5*pi; 686 if( x3 == 0.0 ) argument = 0.5*pi; 670 else argument = std::atan2(fIm << 687 else argument = atan2(fImPartDielectricConst[i],x3); 671 argument *= x5 ; 688 argument *= x5 ; 672 } 689 } 673 dNdxC = ( logarithm*fImPartDielectricConst[ 690 dNdxC = ( logarithm*fImPartDielectricConst[i] + argument )/hbarc; 674 691 675 if(dNdxC < 1.0e-8) dNdxC = 1.0e-8; 692 if(dNdxC < 1.0e-8) dNdxC = 1.0e-8; 676 693 677 dNdxC *= fine_structure_const/be2/pi; 694 dNdxC *= fine_structure_const/be2/pi; 678 695 679 dNdxC *= (1 - std::exp(-be4/betaBohr4)); << 696 dNdxC *= (1-exp(-be4/betaBohr4)); 680 697 >> 698 // if(fDensity >= 0.1) >> 699 // { 681 modul2 = (1.0 + fRePartDielectricConst[i])* 700 modul2 = (1.0 + fRePartDielectricConst[i])*(1.0 + fRePartDielectricConst[i]) + 682 fImPartDielectricConst[i]* 701 fImPartDielectricConst[i]*fImPartDielectricConst[i]; 683 if(modul2 > 0.) 702 if(modul2 > 0.) 684 { 703 { 685 dNdxC /= modul2; 704 dNdxC /= modul2; 686 } 705 } 687 return dNdxC; 706 return dNdxC; 688 707 689 } // end of PAIdNdxCerenkov 708 } // end of PAIdNdxCerenkov 690 709 691 ////////////////////////////////////////////// 710 ////////////////////////////////////////////////////////////////////////// 692 // 711 // 693 // Calculation od dN/dx of collisions with cre 712 // Calculation od dN/dx of collisions with creation of longitudinal EM 694 // excitations (plasmons, delta-electrons) 713 // excitations (plasmons, delta-electrons) 695 714 696 G4double G4PAIySection::PAIdNdxPlasmon( G4int << 715 G4double G4PAIySection::PAIdNdxPlasmon( G4int i , >> 716 G4double betaGammaSq ) 697 { 717 { 698 G4double cof, resonance, modul2, dNdxP; 718 G4double cof, resonance, modul2, dNdxP; 699 G4double be2, be4; 719 G4double be2, be4; 700 720 701 cof = 1; 721 cof = 1; 702 722 703 be2 = betaGammaSq/(1 + betaGammaSq); 723 be2 = betaGammaSq/(1 + betaGammaSq); 704 be4 = be2*be2; 724 be4 = be2*be2; 705 725 706 resonance = std::log(2*electron_mass_c2*be2 << 726 resonance = log(2*electron_mass_c2*be2/fSplineEnergy[i]); 707 resonance *= fImPartDielectricConst[i]/hbar 727 resonance *= fImPartDielectricConst[i]/hbarc; 708 728 709 dNdxP = ( resonance + cof*fIntegralTerm[i]/ 729 dNdxP = ( resonance + cof*fIntegralTerm[i]/fSplineEnergy[i]/fSplineEnergy[i] ); 710 730 711 dNdxP = std::max(dNdxP, 1.0e-8); 731 dNdxP = std::max(dNdxP, 1.0e-8); 712 732 713 dNdxP *= fine_structure_const/be2/pi; 733 dNdxP *= fine_structure_const/be2/pi; 714 dNdxP *= (1 - std::exp(-be4/betaBohr4)); << 734 dNdxP *= (1-exp(-be4/betaBohr4)); 715 735 >> 736 // if( fDensity >= 0.1 ) >> 737 // { 716 modul2 = (1 + fRePartDielectricConst[i])*(1 738 modul2 = (1 + fRePartDielectricConst[i])*(1 + fRePartDielectricConst[i]) + 717 fImPartDielectricConst[i]*fImPartDielectr 739 fImPartDielectricConst[i]*fImPartDielectricConst[i]; 718 if(modul2 > 0.) 740 if(modul2 > 0.) 719 { 741 { 720 dNdxP /= modul2; 742 dNdxP /= modul2; 721 } 743 } 722 return dNdxP; 744 return dNdxP; 723 745 724 } // end of PAIdNdxPlasmon 746 } // end of PAIdNdxPlasmon 725 747 726 ////////////////////////////////////////////// 748 //////////////////////////////////////////////////////////////////////// 727 // 749 // 728 // Calculation of the PAI integral cross-secti 750 // Calculation of the PAI integral cross-section 729 // fIntegralPAIySection[1] = specific primary 751 // fIntegralPAIySection[1] = specific primary ionisation, 1/cm 730 // and fIntegralPAIySection[0] = mean energy l 752 // and fIntegralPAIySection[0] = mean energy loss per cm in keV/cm 731 753 732 void G4PAIySection::IntegralPAIySection() 754 void G4PAIySection::IntegralPAIySection() 733 { 755 { 734 fIntegralPAIySection[fSplineNumber] = 0; 756 fIntegralPAIySection[fSplineNumber] = 0; 735 fIntegralPAIdEdx[fSplineNumber] = 0; 757 fIntegralPAIdEdx[fSplineNumber] = 0; 736 fIntegralPAIySection[0] = 0; 758 fIntegralPAIySection[0] = 0; 737 G4int k = fIntervalNumber -1; 759 G4int k = fIntervalNumber -1; 738 760 739 for(G4int i = fSplineNumber-1; i >= 1; i--) 761 for(G4int i = fSplineNumber-1; i >= 1; i--) 740 { 762 { 741 if(fSplineEnergy[i] >= fEnergyInterval[k]) 763 if(fSplineEnergy[i] >= fEnergyInterval[k]) 742 { 764 { 743 fIntegralPAIySection[i] = fIntegralPAIyS 765 fIntegralPAIySection[i] = fIntegralPAIySection[i+1] + SumOverInterval(i); 744 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i 766 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i+1] + SumOverIntervaldEdx(i); 745 } 767 } 746 else 768 else 747 { 769 { 748 fIntegralPAIySection[i] = fIntegralPAIyS 770 fIntegralPAIySection[i] = fIntegralPAIySection[i+1] + 749 SumOverBord 771 SumOverBorder(i+1,fEnergyInterval[k]); 750 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i 772 fIntegralPAIdEdx[i] = fIntegralPAIdEdx[i+1] + 751 SumOverBord 773 SumOverBorderdEdx(i+1,fEnergyInterval[k]); 752 k--; 774 k--; 753 } 775 } 754 } 776 } 755 } // end of IntegralPAIySection 777 } // end of IntegralPAIySection 756 778 757 ////////////////////////////////////////////// 779 //////////////////////////////////////////////////////////////////////// 758 // 780 // 759 // Calculation of the PAI Cerenkov integral cr 781 // Calculation of the PAI Cerenkov integral cross-section 760 // fIntegralCrenkov[1] = specific Crenkov ioni 782 // fIntegralCrenkov[1] = specific Crenkov ionisation, 1/cm 761 // and fIntegralCerenkov[0] = mean Cerenkov lo 783 // and fIntegralCerenkov[0] = mean Cerenkov loss per cm in keV/cm 762 784 763 void G4PAIySection::IntegralCerenkov() 785 void G4PAIySection::IntegralCerenkov() 764 { 786 { 765 G4int i, k; 787 G4int i, k; 766 fIntegralCerenkov[fSplineNumber] = 0; 788 fIntegralCerenkov[fSplineNumber] = 0; 767 fIntegralCerenkov[0] = 0; 789 fIntegralCerenkov[0] = 0; 768 k = fIntervalNumber -1; 790 k = fIntervalNumber -1; 769 791 770 for( i = fSplineNumber-1; i >= 1; i-- ) 792 for( i = fSplineNumber-1; i >= 1; i-- ) 771 { 793 { 772 if(fSplineEnergy[i] >= fEnergyInterval[k 794 if(fSplineEnergy[i] >= fEnergyInterval[k]) 773 { 795 { 774 fIntegralCerenkov[i] = fIntegralCerenk 796 fIntegralCerenkov[i] = fIntegralCerenkov[i+1] + SumOverInterCerenkov(i); 775 // G4cout<<"int: i = "<<i<<"; sumC = " 797 // G4cout<<"int: i = "<<i<<"; sumC = "<<fIntegralCerenkov[i]<<G4endl; 776 } 798 } 777 else 799 else 778 { 800 { 779 fIntegralCerenkov[i] = fIntegralCerenk 801 fIntegralCerenkov[i] = fIntegralCerenkov[i+1] + 780 SumOverBord 802 SumOverBordCerenkov(i+1,fEnergyInterval[k]); 781 k--; 803 k--; 782 // G4cout<<"bord: i = "<<i<<"; sumC = 804 // G4cout<<"bord: i = "<<i<<"; sumC = "<<fIntegralCerenkov[i]<<G4endl; 783 } 805 } 784 } 806 } 785 807 786 } // end of IntegralCerenkov 808 } // end of IntegralCerenkov 787 809 788 ////////////////////////////////////////////// 810 //////////////////////////////////////////////////////////////////////// 789 // 811 // 790 // Calculation of the PAI Plasmon integral cro 812 // Calculation of the PAI Plasmon integral cross-section 791 // fIntegralPlasmon[1] = splasmon primary ioni 813 // fIntegralPlasmon[1] = splasmon primary ionisation, 1/cm 792 // and fIntegralPlasmon[0] = mean plasmon loss 814 // and fIntegralPlasmon[0] = mean plasmon loss per cm in keV/cm 793 815 794 void G4PAIySection::IntegralPlasmon() 816 void G4PAIySection::IntegralPlasmon() 795 { 817 { 796 fIntegralPlasmon[fSplineNumber] = 0; 818 fIntegralPlasmon[fSplineNumber] = 0; 797 fIntegralPlasmon[0] = 0; 819 fIntegralPlasmon[0] = 0; 798 G4int k = fIntervalNumber -1; 820 G4int k = fIntervalNumber -1; 799 for(G4int i=fSplineNumber-1;i>=1;i--) 821 for(G4int i=fSplineNumber-1;i>=1;i--) 800 { 822 { 801 if(fSplineEnergy[i] >= fEnergyInterval[k 823 if(fSplineEnergy[i] >= fEnergyInterval[k]) 802 { 824 { 803 fIntegralPlasmon[i] = fIntegralPlasmon 825 fIntegralPlasmon[i] = fIntegralPlasmon[i+1] + SumOverInterPlasmon(i); 804 } 826 } 805 else 827 else 806 { 828 { 807 fIntegralPlasmon[i] = fIntegralPlasmon 829 fIntegralPlasmon[i] = fIntegralPlasmon[i+1] + 808 SumOverBord 830 SumOverBordPlasmon(i+1,fEnergyInterval[k]); 809 k--; 831 k--; 810 } 832 } 811 } 833 } >> 834 812 } // end of IntegralPlasmon 835 } // end of IntegralPlasmon 813 836 814 ////////////////////////////////////////////// 837 ////////////////////////////////////////////////////////////////////// 815 // 838 // 816 // Calculation the PAI integral cross-section 839 // Calculation the PAI integral cross-section inside 817 // of interval of continuous values of photo-i 840 // of interval of continuous values of photo-ionisation 818 // cross-section. Parameter 'i' is the number 841 // cross-section. Parameter 'i' is the number of interval. 819 842 820 G4double G4PAIySection::SumOverInterval( G4int 843 G4double G4PAIySection::SumOverInterval( G4int i ) 821 { 844 { 822 G4double x0,x1,y0,yy1,a,b,c,result; 845 G4double x0,x1,y0,yy1,a,b,c,result; 823 846 824 x0 = fSplineEnergy[i]; 847 x0 = fSplineEnergy[i]; 825 x1 = fSplineEnergy[i+1]; 848 x1 = fSplineEnergy[i+1]; 826 849 827 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) 850 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) return 0.; 828 851 829 y0 = fDifPAIySection[i]; 852 y0 = fDifPAIySection[i]; 830 yy1 = fDifPAIySection[i+1]; 853 yy1 = fDifPAIySection[i+1]; 831 //G4cout << "## x0= " << x0 << " x1= " << x 854 //G4cout << "## x0= " << x0 << " x1= " << x1 << G4endl; 832 c = x1/x0; 855 c = x1/x0; 833 //G4cout << "c= " << c << " y0= " << y0 << 856 //G4cout << "c= " << c << " y0= " << y0 << " yy1= " << yy1 << G4endl; 834 a = log10(yy1/y0)/log10(c); 857 a = log10(yy1/y0)/log10(c); 835 //G4cout << "a= " << a << G4endl; 858 //G4cout << "a= " << a << G4endl; 836 << 859 // b = log10(y0) - a*log10(x0); 837 b = 0.0; << 860 b = y0/pow(x0,a); 838 if(a < 20.) b = y0/pow(x0,a); << 839 << 840 a += 1; 861 a += 1; 841 if(a == 0) 862 if(a == 0) 842 { 863 { 843 result = b*log(x1/x0); 864 result = b*log(x1/x0); 844 } 865 } 845 else 866 else 846 { 867 { 847 result = y0*(x1*pow(c,a-1) - x0)/a; 868 result = y0*(x1*pow(c,a-1) - x0)/a; 848 } 869 } 849 a++; 870 a++; 850 if(a == 0) 871 if(a == 0) 851 { 872 { 852 fIntegralPAIySection[0] += b*log(x1/x0); 873 fIntegralPAIySection[0] += b*log(x1/x0); 853 } 874 } 854 else 875 else 855 { 876 { 856 fIntegralPAIySection[0] += y0*(x1*x1*pow 877 fIntegralPAIySection[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a; 857 } 878 } 858 return result; 879 return result; 859 880 860 } // end of SumOverInterval 881 } // end of SumOverInterval 861 882 862 ///////////////////////////////// 883 ///////////////////////////////// 863 884 864 G4double G4PAIySection::SumOverIntervaldEdx( G 885 G4double G4PAIySection::SumOverIntervaldEdx( G4int i ) 865 { 886 { 866 G4double x0,x1,y0,yy1,a,b,c,result; 887 G4double x0,x1,y0,yy1,a,b,c,result; 867 888 868 x0 = fSplineEnergy[i]; 889 x0 = fSplineEnergy[i]; 869 x1 = fSplineEnergy[i+1]; 890 x1 = fSplineEnergy[i+1]; 870 891 871 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) 892 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) return 0.; 872 893 873 y0 = fDifPAIySection[i]; 894 y0 = fDifPAIySection[i]; 874 yy1 = fDifPAIySection[i+1]; 895 yy1 = fDifPAIySection[i+1]; 875 c = x1/x0; 896 c = x1/x0; 876 a = log10(yy1/y0)/log10(c); 897 a = log10(yy1/y0)/log10(c); 877 << 898 // b = log10(y0) - a*log10(x0); 878 b = 0.0; << 899 b = y0/pow(x0,a); 879 if(a < 20.) b = y0/pow(x0,a); << 880 << 881 a += 2; 900 a += 2; 882 if(a == 0) 901 if(a == 0) 883 { 902 { 884 result = b*log(x1/x0); 903 result = b*log(x1/x0); 885 } 904 } 886 else 905 else 887 { 906 { 888 result = y0*(x1*x1*pow(c,a-2) - x0*x0)/a; 907 result = y0*(x1*x1*pow(c,a-2) - x0*x0)/a; 889 } 908 } 890 return result; 909 return result; 891 910 892 } // end of SumOverInterval 911 } // end of SumOverInterval 893 912 894 ////////////////////////////////////////////// 913 ////////////////////////////////////////////////////////////////////// 895 // 914 // 896 // Calculation the PAI Cerenkov integral cross 915 // Calculation the PAI Cerenkov integral cross-section inside 897 // of interval of continuous values of photo-i 916 // of interval of continuous values of photo-ionisation Cerenkov 898 // cross-section. Parameter 'i' is the number 917 // cross-section. Parameter 'i' is the number of interval. 899 918 900 G4double G4PAIySection::SumOverInterCerenkov( 919 G4double G4PAIySection::SumOverInterCerenkov( G4int i ) 901 { 920 { 902 G4double x0,x1,y0,yy1,a,c,result; 921 G4double x0,x1,y0,yy1,a,c,result; 903 922 904 x0 = fSplineEnergy[i]; 923 x0 = fSplineEnergy[i]; 905 x1 = fSplineEnergy[i+1]; 924 x1 = fSplineEnergy[i+1]; 906 925 907 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) 926 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) return 0.; 908 927 909 y0 = fdNdxCerenkov[i]; 928 y0 = fdNdxCerenkov[i]; 910 yy1 = fdNdxCerenkov[i+1]; 929 yy1 = fdNdxCerenkov[i+1]; 911 // G4cout<<"SumC, i = "<<i<<"; x0 ="<<x0<<" 930 // G4cout<<"SumC, i = "<<i<<"; x0 ="<<x0<<"; x1 = "<<x1 912 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4en 931 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl; 913 932 914 c = x1/x0; 933 c = x1/x0; 915 a = log10(yy1/y0)/log10(c); 934 a = log10(yy1/y0)/log10(c); 916 G4double b = 0.0; 935 G4double b = 0.0; 917 if(a < 20.) b = y0/pow(x0,a); 936 if(a < 20.) b = y0/pow(x0,a); 918 937 919 a += 1.0; 938 a += 1.0; 920 if(a == 0) result = b*log(c); 939 if(a == 0) result = b*log(c); 921 else result = y0*(x1*pow(c,a-1) - x0) 940 else result = y0*(x1*pow(c,a-1) - x0)/a; 922 a += 1.0; 941 a += 1.0; 923 942 924 if( a == 0 ) fIntegralCerenkov[0] += b*log( 943 if( a == 0 ) fIntegralCerenkov[0] += b*log(x1/x0); 925 else fIntegralCerenkov[0] += y0*(x1 944 else fIntegralCerenkov[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a; 926 // G4cout<<"a = "<<a<<"; b = "<<b<<"; resu 945 // G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl; 927 return result; 946 return result; 928 947 929 } // end of SumOverInterCerenkov 948 } // end of SumOverInterCerenkov 930 949 931 ////////////////////////////////////////////// 950 ////////////////////////////////////////////////////////////////////// 932 // 951 // 933 // Calculation the PAI Plasmon integral cross- 952 // Calculation the PAI Plasmon integral cross-section inside 934 // of interval of continuous values of photo-i 953 // of interval of continuous values of photo-ionisation Plasmon 935 // cross-section. Parameter 'i' is the number 954 // cross-section. Parameter 'i' is the number of interval. 936 955 937 G4double G4PAIySection::SumOverInterPlasmon( G 956 G4double G4PAIySection::SumOverInterPlasmon( G4int i ) 938 { 957 { 939 G4double x0,x1,y0,yy1,a,c,result; 958 G4double x0,x1,y0,yy1,a,c,result; 940 959 941 x0 = fSplineEnergy[i]; 960 x0 = fSplineEnergy[i]; 942 x1 = fSplineEnergy[i+1]; 961 x1 = fSplineEnergy[i+1]; 943 962 944 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) 963 if( std::abs( 2.*(x1-x0)/(x1+x0) ) < 1.e-6) return 0.; 945 964 946 y0 = fdNdxPlasmon[i]; 965 y0 = fdNdxPlasmon[i]; 947 yy1 = fdNdxPlasmon[i+1]; 966 yy1 = fdNdxPlasmon[i+1]; 948 c = x1/x0; 967 c = x1/x0; 949 a = log10(yy1/y0)/log10(c); 968 a = log10(yy1/y0)/log10(c); 950 969 951 G4double b = 0.0; 970 G4double b = 0.0; 952 if(a < 20.) b = y0/pow(x0,a); 971 if(a < 20.) b = y0/pow(x0,a); 953 972 954 a += 1.0; 973 a += 1.0; 955 if(a == 0) result = b*log(x1/x0); 974 if(a == 0) result = b*log(x1/x0); 956 else result = y0*(x1*pow(c,a-1) - x0) 975 else result = y0*(x1*pow(c,a-1) - x0)/a; 957 a += 1.0; 976 a += 1.0; 958 977 959 if( a == 0 ) fIntegralPlasmon[0] += b*log(x 978 if( a == 0 ) fIntegralPlasmon[0] += b*log(x1/x0); 960 else fIntegralPlasmon[0] += y0*(x1* 979 else fIntegralPlasmon[0] += y0*(x1*x1*pow(c,a-2) - x0*x0)/a; 961 980 962 return result; 981 return result; 963 982 964 } // end of SumOverInterPlasmon 983 } // end of SumOverInterPlasmon 965 984 966 ////////////////////////////////////////////// 985 /////////////////////////////////////////////////////////////////////////////// 967 // 986 // 968 // Integration of PAI cross-section for the ca 987 // Integration of PAI cross-section for the case of 969 // passing across border between intervals 988 // passing across border between intervals 970 989 971 G4double G4PAIySection::SumOverBorder( G4int 990 G4double G4PAIySection::SumOverBorder( G4int i , 972 G4doubl 991 G4double en0 ) 973 { 992 { 974 G4double x0,x1,y0,yy1,a,d,e0,result; << 993 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result; 975 994 976 e0 = en0; 995 e0 = en0; 977 x0 = fSplineEnergy[i]; 996 x0 = fSplineEnergy[i]; 978 x1 = fSplineEnergy[i+1]; 997 x1 = fSplineEnergy[i+1]; 979 y0 = fDifPAIySection[i]; 998 y0 = fDifPAIySection[i]; 980 yy1 = fDifPAIySection[i+1]; 999 yy1 = fDifPAIySection[i+1]; 981 1000 >> 1001 //c = x1/x0; 982 d = e0/x0; 1002 d = e0/x0; 983 a = log10(yy1/y0)/log10(x1/x0); 1003 a = log10(yy1/y0)/log10(x1/x0); 984 1004 985 G4double b = 0.0; 1005 G4double b = 0.0; 986 if(a < 20.) b = y0/pow(x0,a); 1006 if(a < 20.) b = y0/pow(x0,a); 987 1007 988 a += 1; 1008 a += 1; 989 if(a == 0) 1009 if(a == 0) 990 { 1010 { 991 result = b*log(x0/e0); 1011 result = b*log(x0/e0); 992 } 1012 } 993 else 1013 else 994 { 1014 { 995 result = y0*(x0 - e0*pow(d,a-1))/a; 1015 result = y0*(x0 - e0*pow(d,a-1))/a; 996 } 1016 } 997 a++; 1017 a++; 998 if(a == 0) 1018 if(a == 0) 999 { 1019 { 1000 fIntegralPAIySection[0] += b*log(x0/e0) 1020 fIntegralPAIySection[0] += b*log(x0/e0); 1001 } 1021 } 1002 else 1022 else 1003 { 1023 { 1004 fIntegralPAIySection[0] += y0*(x0*x0 - 1024 fIntegralPAIySection[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a; 1005 } 1025 } 1006 x0 = fSplineEnergy[i - 1]; 1026 x0 = fSplineEnergy[i - 1]; 1007 x1 = fSplineEnergy[i - 2]; 1027 x1 = fSplineEnergy[i - 2]; 1008 y0 = fDifPAIySection[i - 1]; 1028 y0 = fDifPAIySection[i - 1]; 1009 yy1 = fDifPAIySection[i - 2]; 1029 yy1 = fDifPAIySection[i - 2]; 1010 1030 1011 //c = x1/x0; 1031 //c = x1/x0; 1012 d = e0/x0; 1032 d = e0/x0; 1013 a = log10(yy1/y0)/log10(x1/x0); 1033 a = log10(yy1/y0)/log10(x1/x0); 1014 << 1034 // b0 = log10(y0) - a*log10(x0); 1015 b = 0.0; << 1035 b = y0/pow(x0,a); 1016 if(a < 20.) b = y0/pow(x0,a); << 1017 << 1018 a += 1; 1036 a += 1; 1019 if(a == 0) 1037 if(a == 0) 1020 { 1038 { 1021 result += b*log(e0/x0); 1039 result += b*log(e0/x0); 1022 } 1040 } 1023 else 1041 else 1024 { 1042 { 1025 result += y0*(e0*pow(d,a-1) - x0)/a; 1043 result += y0*(e0*pow(d,a-1) - x0)/a; 1026 } 1044 } 1027 a++; 1045 a++; 1028 if(a == 0) 1046 if(a == 0) 1029 { 1047 { 1030 fIntegralPAIySection[0] += b*log(e0/x0) 1048 fIntegralPAIySection[0] += b*log(e0/x0); 1031 } 1049 } 1032 else 1050 else 1033 { 1051 { 1034 fIntegralPAIySection[0] += y0*(e0*e0*po 1052 fIntegralPAIySection[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a; 1035 } 1053 } 1036 return result; 1054 return result; 1037 1055 1038 } 1056 } 1039 1057 1040 ///////////////////////////////////////////// 1058 /////////////////////////////////////////////////////////////////////// 1041 1059 1042 G4double G4PAIySection::SumOverBorderdEdx( G4 1060 G4double G4PAIySection::SumOverBorderdEdx( G4int i , 1043 G4doub 1061 G4double en0 ) 1044 { 1062 { 1045 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result; 1063 G4double x0,x1,y0,yy1,a,/*c,*/d,e0,result; 1046 1064 1047 e0 = en0; 1065 e0 = en0; 1048 x0 = fSplineEnergy[i]; 1066 x0 = fSplineEnergy[i]; 1049 x1 = fSplineEnergy[i+1]; 1067 x1 = fSplineEnergy[i+1]; 1050 y0 = fDifPAIySection[i]; 1068 y0 = fDifPAIySection[i]; 1051 yy1 = fDifPAIySection[i+1]; 1069 yy1 = fDifPAIySection[i+1]; 1052 1070 >> 1071 //c = x1/x0; 1053 d = e0/x0; 1072 d = e0/x0; 1054 a = log10(yy1/y0)/log10(x1/x0); 1073 a = log10(yy1/y0)/log10(x1/x0); 1055 1074 1056 G4double b = 0.0; 1075 G4double b = 0.0; 1057 if(a < 20.) b = y0/pow(x0,a); 1076 if(a < 20.) b = y0/pow(x0,a); 1058 1077 1059 a += 2; 1078 a += 2; 1060 if(a == 0) 1079 if(a == 0) 1061 { 1080 { 1062 result = b*log(x0/e0); 1081 result = b*log(x0/e0); 1063 } 1082 } 1064 else 1083 else 1065 { 1084 { 1066 result = y0*(x0*x0 - e0*e0*pow(d,a-2))/ 1085 result = y0*(x0*x0 - e0*e0*pow(d,a-2))/a; 1067 } 1086 } 1068 x0 = fSplineEnergy[i - 1]; 1087 x0 = fSplineEnergy[i - 1]; 1069 x1 = fSplineEnergy[i - 2]; 1088 x1 = fSplineEnergy[i - 2]; 1070 y0 = fDifPAIySection[i - 1]; 1089 y0 = fDifPAIySection[i - 1]; 1071 yy1 = fDifPAIySection[i - 2]; 1090 yy1 = fDifPAIySection[i - 2]; 1072 1091 >> 1092 //c = x1/x0; 1073 d = e0/x0; 1093 d = e0/x0; 1074 a = log10(yy1/y0)/log10(x1/x0); 1094 a = log10(yy1/y0)/log10(x1/x0); 1075 1095 1076 b = 0.0; << 1077 if(a < 20.) b = y0/pow(x0,a); 1096 if(a < 20.) b = y0/pow(x0,a); 1078 1097 1079 a += 2; 1098 a += 2; 1080 if(a == 0) 1099 if(a == 0) 1081 { 1100 { 1082 result += b*log(e0/x0); 1101 result += b*log(e0/x0); 1083 } 1102 } 1084 else 1103 else 1085 { 1104 { 1086 result += y0*(e0*e0*pow(d,a-2) - x0*x0) 1105 result += y0*(e0*e0*pow(d,a-2) - x0*x0)/a; 1087 } 1106 } 1088 return result; 1107 return result; >> 1108 1089 } 1109 } 1090 1110 1091 ///////////////////////////////////////////// 1111 /////////////////////////////////////////////////////////////////////////////// 1092 // 1112 // 1093 // Integration of Cerenkov cross-section for 1113 // Integration of Cerenkov cross-section for the case of 1094 // passing across border between intervals 1114 // passing across border between intervals 1095 1115 1096 G4double G4PAIySection::SumOverBordCerenkov( 1116 G4double G4PAIySection::SumOverBordCerenkov( G4int i , 1097 1117 G4double en0 ) 1098 { 1118 { 1099 G4double x0,x1,y0,yy1,a,e0,c,d,result; 1119 G4double x0,x1,y0,yy1,a,e0,c,d,result; 1100 1120 1101 e0 = en0; 1121 e0 = en0; 1102 x0 = fSplineEnergy[i]; 1122 x0 = fSplineEnergy[i]; 1103 x1 = fSplineEnergy[i+1]; 1123 x1 = fSplineEnergy[i+1]; 1104 y0 = fdNdxCerenkov[i]; 1124 y0 = fdNdxCerenkov[i]; 1105 yy1 = fdNdxCerenkov[i+1]; 1125 yy1 = fdNdxCerenkov[i+1]; 1106 1126 1107 // G4cout<<G4endl; 1127 // G4cout<<G4endl; 1108 //G4cout<<"SumBordC, i = "<<i<<"; en0 = "< 1128 //G4cout<<"SumBordC, i = "<<i<<"; en0 = "<<en0<<"; x0 ="<<x0<<"; x1 = "<<x1 1109 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G 1129 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl; 1110 c = x1/x0; 1130 c = x1/x0; 1111 d = e0/x0; 1131 d = e0/x0; 1112 a = log10(yy1/y0)/log10(c); 1132 a = log10(yy1/y0)/log10(c); 1113 1133 1114 G4double b = 0.0; 1134 G4double b = 0.0; 1115 if(a < 20.) b = y0/pow(x0,a); 1135 if(a < 20.) b = y0/pow(x0,a); 1116 1136 1117 a += 1.0; 1137 a += 1.0; 1118 if( a == 0 ) result = b*log(x0/e0); 1138 if( a == 0 ) result = b*log(x0/e0); 1119 else result = y0*(x0 - e0*pow(d,a- 1139 else result = y0*(x0 - e0*pow(d,a-1))/a; 1120 a += 1.0; 1140 a += 1.0; 1121 1141 1122 if( a == 0 ) fIntegralCerenkov[0] += b*log 1142 if( a == 0 ) fIntegralCerenkov[0] += b*log(x0/e0); 1123 else fIntegralCerenkov[0] += y0*(x 1143 else fIntegralCerenkov[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a; 1124 1144 1125 //G4cout<<"a = "<<a<<"; b = "<<b<<"; resul 1145 //G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl; 1126 1146 1127 x0 = fSplineEnergy[i - 1]; 1147 x0 = fSplineEnergy[i - 1]; 1128 x1 = fSplineEnergy[i - 2]; 1148 x1 = fSplineEnergy[i - 2]; 1129 y0 = fdNdxCerenkov[i - 1]; 1149 y0 = fdNdxCerenkov[i - 1]; 1130 yy1 = fdNdxCerenkov[i - 2]; 1150 yy1 = fdNdxCerenkov[i - 2]; 1131 1151 1132 //G4cout<<"x0 ="<<x0<<"; x1 = "<<x1 1152 //G4cout<<"x0 ="<<x0<<"; x1 = "<<x1 1133 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4 1153 // <<"; y0 = "<<y0<<"; yy1 = "<<yy1<<G4endl; 1134 1154 1135 c = x1/x0; 1155 c = x1/x0; 1136 d = e0/x0; 1156 d = e0/x0; 1137 a = log10(yy1/y0)/log10(x1/x0); 1157 a = log10(yy1/y0)/log10(x1/x0); 1138 1158 1139 // G4cout << "a= " << a << G4endl; 1159 // G4cout << "a= " << a << G4endl; 1140 if(a > 20.0) b = 0.0; 1160 if(a > 20.0) b = 0.0; 1141 else b = y0/pow(x0,a); 1161 else b = y0/pow(x0,a); 1142 1162 1143 //G4cout << "b= " << b << G4endl; 1163 //G4cout << "b= " << b << G4endl; 1144 1164 1145 a += 1.0; 1165 a += 1.0; 1146 if( a == 0 ) result += b*log(e0/x0); 1166 if( a == 0 ) result += b*log(e0/x0); 1147 else result += y0*(e0*pow(d,a-1) - 1167 else result += y0*(e0*pow(d,a-1) - x0 )/a; 1148 a += 1.0; 1168 a += 1.0; 1149 //G4cout << "result= " << result << G4endl 1169 //G4cout << "result= " << result << G4endl; 1150 1170 1151 if( a == 0 ) fIntegralCerenkov[0] += b*l 1171 if( a == 0 ) fIntegralCerenkov[0] += b*log(e0/x0); 1152 else fIntegralCerenkov[0] += y0* 1172 else fIntegralCerenkov[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a; 1153 1173 1154 //G4cout<<"a = "<<a<<"; b = "<<b<<"; resul 1174 //G4cout<<"a = "<<a<<"; b = "<<b<<"; result = "<<result<<G4endl; 1155 1175 1156 return result; 1176 return result; >> 1177 1157 } 1178 } 1158 1179 1159 ///////////////////////////////////////////// 1180 /////////////////////////////////////////////////////////////////////////////// 1160 // 1181 // 1161 // Integration of Plasmon cross-section for t 1182 // Integration of Plasmon cross-section for the case of 1162 // passing across border between intervals 1183 // passing across border between intervals 1163 1184 1164 G4double G4PAIySection::SumOverBordPlasmon( G 1185 G4double G4PAIySection::SumOverBordPlasmon( G4int i , 1165 1186 G4double en0 ) 1166 { 1187 { 1167 G4double x0,x1,y0,yy1,a,c,d,e0,result; 1188 G4double x0,x1,y0,yy1,a,c,d,e0,result; 1168 1189 1169 e0 = en0; 1190 e0 = en0; 1170 x0 = fSplineEnergy[i]; 1191 x0 = fSplineEnergy[i]; 1171 x1 = fSplineEnergy[i+1]; 1192 x1 = fSplineEnergy[i+1]; 1172 y0 = fdNdxPlasmon[i]; 1193 y0 = fdNdxPlasmon[i]; 1173 yy1 = fdNdxPlasmon[i+1]; 1194 yy1 = fdNdxPlasmon[i+1]; 1174 1195 1175 c = x1/x0; 1196 c = x1/x0; 1176 d = e0/x0; 1197 d = e0/x0; 1177 a = log10(yy1/y0)/log10(c); 1198 a = log10(yy1/y0)/log10(c); 1178 1199 1179 G4double b = 0.0; 1200 G4double b = 0.0; 1180 if(a < 20.) b = y0/pow(x0,a); 1201 if(a < 20.) b = y0/pow(x0,a); 1181 1202 1182 a += 1.0; 1203 a += 1.0; 1183 if( a == 0 ) result = b*log(x0/e0); 1204 if( a == 0 ) result = b*log(x0/e0); 1184 else result = y0*(x0 - e0*pow(d,a- 1205 else result = y0*(x0 - e0*pow(d,a-1))/a; 1185 a += 1.0; 1206 a += 1.0; 1186 1207 1187 if( a == 0 ) fIntegralPlasmon[0] += b*log( 1208 if( a == 0 ) fIntegralPlasmon[0] += b*log(x0/e0); 1188 else fIntegralPlasmon[0] += y0*(x0 1209 else fIntegralPlasmon[0] += y0*(x0*x0 - e0*e0*pow(d,a-2))/a; 1189 1210 1190 x0 = fSplineEnergy[i - 1]; 1211 x0 = fSplineEnergy[i - 1]; 1191 x1 = fSplineEnergy[i - 2]; 1212 x1 = fSplineEnergy[i - 2]; 1192 y0 = fdNdxPlasmon[i - 1]; 1213 y0 = fdNdxPlasmon[i - 1]; 1193 yy1 = fdNdxPlasmon[i - 2]; 1214 yy1 = fdNdxPlasmon[i - 2]; 1194 1215 1195 c = x1/x0; 1216 c = x1/x0; 1196 d = e0/x0; 1217 d = e0/x0; 1197 a = log10(yy1/y0)/log10(c); 1218 a = log10(yy1/y0)/log10(c); 1198 1219 1199 if(a < 20.) b = y0/pow(x0,a); 1220 if(a < 20.) b = y0/pow(x0,a); 1200 1221 1201 a += 1.0; 1222 a += 1.0; 1202 if( a == 0 ) result += b*log(e0/x0); 1223 if( a == 0 ) result += b*log(e0/x0); 1203 else result += y0*(e0*pow(d,a-1) - 1224 else result += y0*(e0*pow(d,a-1) - x0)/a; 1204 a += 1.0; 1225 a += 1.0; 1205 1226 1206 if( a == 0 ) fIntegralPlasmon[0] += b*lo 1227 if( a == 0 ) fIntegralPlasmon[0] += b*log(e0/x0); 1207 else fIntegralPlasmon[0] += y0*( 1228 else fIntegralPlasmon[0] += y0*(e0*e0*pow(d,a-2) - x0*x0)/a; 1208 1229 1209 return result; 1230 return result; 1210 1231 1211 } 1232 } 1212 1233 1213 ///////////////////////////////////////////// 1234 ///////////////////////////////////////////////////////////////////////// 1214 // 1235 // 1215 // 1236 // 1216 1237 1217 G4double G4PAIySection::GetStepEnergyLoss( G4 1238 G4double G4PAIySection::GetStepEnergyLoss( G4double step ) 1218 { 1239 { 1219 G4int iTransfer ; 1240 G4int iTransfer ; 1220 G4long numOfCollisions; 1241 G4long numOfCollisions; 1221 G4double loss = 0.0; 1242 G4double loss = 0.0; 1222 G4double meanNumber, position; 1243 G4double meanNumber, position; 1223 1244 1224 // G4cout<<" G4PAIySection::GetStepEnergyLo 1245 // G4cout<<" G4PAIySection::GetStepEnergyLoss "<<G4endl; 1225 1246 1226 1247 1227 1248 1228 meanNumber = fIntegralPAIySection[1]*step; 1249 meanNumber = fIntegralPAIySection[1]*step; 1229 numOfCollisions = G4Poisson(meanNumber); 1250 numOfCollisions = G4Poisson(meanNumber); 1230 1251 1231 // G4cout<<"numOfCollisions = "<<numOfCol 1252 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl; 1232 1253 1233 while(numOfCollisions) 1254 while(numOfCollisions) 1234 { 1255 { 1235 position = fIntegralPAIySection[1]*G4Unif 1256 position = fIntegralPAIySection[1]*G4UniformRand(); 1236 1257 1237 for( iTransfer=1; iTransfer<=fSplineNumbe 1258 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ ) 1238 { 1259 { 1239 if( position >= fIntegralPAIySection[ 1260 if( position >= fIntegralPAIySection[iTransfer] ) break; 1240 } 1261 } 1241 loss += fSplineEnergy[iTransfer] ; 1262 loss += fSplineEnergy[iTransfer] ; 1242 numOfCollisions--; 1263 numOfCollisions--; 1243 // Loop checking, 03-Aug-2015, Vladimir I 1264 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko 1244 } 1265 } 1245 // G4cout<<"PAI energy loss = "<<loss/keV<< 1266 // G4cout<<"PAI energy loss = "<<loss/keV<<" keV"<<G4endl; 1246 1267 1247 return loss; 1268 return loss; 1248 } 1269 } 1249 1270 1250 ///////////////////////////////////////////// 1271 ///////////////////////////////////////////////////////////////////////// 1251 // 1272 // 1252 // 1273 // 1253 1274 1254 G4double G4PAIySection::GetStepCerenkovLoss( 1275 G4double G4PAIySection::GetStepCerenkovLoss( G4double step ) 1255 { 1276 { 1256 G4int iTransfer ; 1277 G4int iTransfer ; 1257 G4long numOfCollisions; 1278 G4long numOfCollisions; 1258 G4double loss = 0.0; 1279 G4double loss = 0.0; 1259 G4double meanNumber, position; 1280 G4double meanNumber, position; 1260 1281 1261 // G4cout<<" G4PAIySection::GetStepCreLosnk 1282 // G4cout<<" G4PAIySection::GetStepCreLosnkovs "<<G4endl; 1262 1283 1263 1284 1264 1285 1265 meanNumber = fIntegralCerenkov[1]*step; 1286 meanNumber = fIntegralCerenkov[1]*step; 1266 numOfCollisions = G4Poisson(meanNumber); 1287 numOfCollisions = G4Poisson(meanNumber); 1267 1288 1268 // G4cout<<"numOfCollisions = "<<numOfCol 1289 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl; 1269 1290 1270 while(numOfCollisions) 1291 while(numOfCollisions) 1271 { 1292 { 1272 position = fIntegralCerenkov[1]*G4Uniform 1293 position = fIntegralCerenkov[1]*G4UniformRand(); 1273 1294 1274 for( iTransfer=1; iTransfer<=fSplineNumbe 1295 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ ) 1275 { 1296 { 1276 if( position >= fIntegralCerenkov[iTr 1297 if( position >= fIntegralCerenkov[iTransfer] ) break; 1277 } 1298 } 1278 loss += fSplineEnergy[iTransfer] ; 1299 loss += fSplineEnergy[iTransfer] ; 1279 numOfCollisions--; 1300 numOfCollisions--; 1280 // Loop checking, 03-Aug-2015, Vladimir I 1301 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko 1281 } 1302 } 1282 // G4cout<<"PAI Cerenkov loss = "<<loss/keV 1303 // G4cout<<"PAI Cerenkov loss = "<<loss/keV<<" keV"<<G4endl; 1283 1304 1284 return loss; 1305 return loss; 1285 } 1306 } 1286 1307 1287 ///////////////////////////////////////////// 1308 ///////////////////////////////////////////////////////////////////////// 1288 // 1309 // 1289 // 1310 // 1290 1311 1291 G4double G4PAIySection::GetStepPlasmonLoss( G 1312 G4double G4PAIySection::GetStepPlasmonLoss( G4double step ) 1292 { 1313 { 1293 G4int iTransfer ; 1314 G4int iTransfer ; 1294 G4long numOfCollisions; 1315 G4long numOfCollisions; 1295 G4double loss = 0.0; 1316 G4double loss = 0.0; 1296 G4double meanNumber, position; 1317 G4double meanNumber, position; 1297 1318 1298 // G4cout<<" G4PAIySection::GetStepCreLosnk 1319 // G4cout<<" G4PAIySection::GetStepCreLosnkovs "<<G4endl; 1299 1320 1300 1321 1301 1322 1302 meanNumber = fIntegralPlasmon[1]*step; 1323 meanNumber = fIntegralPlasmon[1]*step; 1303 numOfCollisions = G4Poisson(meanNumber); 1324 numOfCollisions = G4Poisson(meanNumber); 1304 1325 1305 // G4cout<<"numOfCollisions = "<<numOfCol 1326 // G4cout<<"numOfCollisions = "<<numOfCollisions<<G4endl; 1306 1327 1307 while(numOfCollisions) 1328 while(numOfCollisions) 1308 { 1329 { 1309 position = fIntegralPlasmon[1]*G4UniformR 1330 position = fIntegralPlasmon[1]*G4UniformRand(); 1310 1331 1311 for( iTransfer=1; iTransfer<=fSplineNumbe 1332 for( iTransfer=1; iTransfer<=fSplineNumber; iTransfer++ ) 1312 { 1333 { 1313 if( position >= fIntegralPlasmon[iTra 1334 if( position >= fIntegralPlasmon[iTransfer] ) break; 1314 } 1335 } 1315 loss += fSplineEnergy[iTransfer] ; 1336 loss += fSplineEnergy[iTransfer] ; 1316 numOfCollisions--; 1337 numOfCollisions--; 1317 // Loop checking, 03-Aug-2015, Vladimir I 1338 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko 1318 } 1339 } 1319 // G4cout<<"PAI Plasmon loss = "<<loss/keV< 1340 // G4cout<<"PAI Plasmon loss = "<<loss/keV<<" keV"<<G4endl; 1320 1341 1321 return loss; 1342 return loss; 1322 } 1343 } 1323 1344 1324 ///////////////////////////////////////////// 1345 ///////////////////////////////////////////////////////////////////////////// 1325 // 1346 // 1326 1347 1327 void G4PAIySection::CallError(G4int i, const 1348 void G4PAIySection::CallError(G4int i, const G4String& methodName) const 1328 { 1349 { 1329 G4String head = "G4PAIySection::" + methodN 1350 G4String head = "G4PAIySection::" + methodName + "()"; 1330 G4ExceptionDescription ed; 1351 G4ExceptionDescription ed; 1331 ed << "Wrong index " << i << " fSplineNumbe 1352 ed << "Wrong index " << i << " fSplineNumber= " << fSplineNumber; 1332 G4Exception(head,"pai001",FatalException,ed 1353 G4Exception(head,"pai001",FatalException,ed); 1333 } 1354 } 1334 1355 1335 ///////////////////////////////////////////// 1356 ///////////////////////////////////////////////////////////////////////////// 1336 // 1357 // 1337 // Init array of Lorentz factors 1358 // Init array of Lorentz factors 1338 // 1359 // 1339 1360 1340 G4int G4PAIySection::fNumberOfGammas = 111; 1361 G4int G4PAIySection::fNumberOfGammas = 111; 1341 1362 1342 const G4double G4PAIySection::fLorentzFactor[ 1363 const G4double G4PAIySection::fLorentzFactor[112] = // fNumberOfGammas+1 1343 { 1364 { 1344 0.0, 1365 0.0, 1345 1.094989e+00, 1.107813e+00, 1.122369e+00, 1.1 1366 1.094989e+00, 1.107813e+00, 1.122369e+00, 1.138890e+00, 1.157642e+00, 1346 1.178925e+00, 1.203082e+00, 1.230500e+00, 1.2 1367 1.178925e+00, 1.203082e+00, 1.230500e+00, 1.261620e+00, 1.296942e+00, // 10 1347 1.337032e+00, 1.382535e+00, 1.434181e+00, 1.4 1368 1.337032e+00, 1.382535e+00, 1.434181e+00, 1.492800e+00, 1.559334e+00, 1348 1.634850e+00, 1.720562e+00, 1.817845e+00, 1.9 1369 1.634850e+00, 1.720562e+00, 1.817845e+00, 1.928263e+00, 2.053589e+00, // 20 1349 2.195835e+00, 2.357285e+00, 2.540533e+00, 2.7 1370 2.195835e+00, 2.357285e+00, 2.540533e+00, 2.748522e+00, 2.984591e+00, 1350 3.252533e+00, 3.556649e+00, 3.901824e+00, 4.2 1371 3.252533e+00, 3.556649e+00, 3.901824e+00, 4.293602e+00, 4.738274e+00, // 30 1351 5.242981e+00, 5.815829e+00, 6.466019e+00, 7.2 1372 5.242981e+00, 5.815829e+00, 6.466019e+00, 7.203990e+00, 8.041596e+00, 1352 8.992288e+00, 1.007133e+01, 1.129606e+01, 1.2 1373 8.992288e+00, 1.007133e+01, 1.129606e+01, 1.268614e+01, 1.426390e+01, // 40 1353 1.605467e+01, 1.808721e+01, 2.039417e+01, 2.3 1374 1.605467e+01, 1.808721e+01, 2.039417e+01, 2.301259e+01, 2.598453e+01, 1354 2.935771e+01, 3.318630e+01, 3.753180e+01, 4.2 1375 2.935771e+01, 3.318630e+01, 3.753180e+01, 4.246399e+01, 4.806208e+01, // 50 1355 5.441597e+01, 6.162770e+01, 6.981310e+01, 7.9 1376 5.441597e+01, 6.162770e+01, 6.981310e+01, 7.910361e+01, 8.964844e+01, 1356 1.016169e+02, 1.152013e+02, 1.306197e+02, 1.4 1377 1.016169e+02, 1.152013e+02, 1.306197e+02, 1.481198e+02, 1.679826e+02, // 60 1357 1.905270e+02, 2.161152e+02, 2.451581e+02, 2.7 1378 1.905270e+02, 2.161152e+02, 2.451581e+02, 2.781221e+02, 3.155365e+02, 1358 3.580024e+02, 4.062016e+02, 4.609081e+02, 5.2 1379 3.580024e+02, 4.062016e+02, 4.609081e+02, 5.230007e+02, 5.934765e+02, // 70 1359 6.734672e+02, 7.642575e+02, 8.673056e+02, 9.8 1380 6.734672e+02, 7.642575e+02, 8.673056e+02, 9.842662e+02, 1.117018e+03, 1360 1.267692e+03, 1.438709e+03, 1.632816e+03, 1.8 1381 1.267692e+03, 1.438709e+03, 1.632816e+03, 1.853128e+03, 2.103186e+03, // 80 1361 2.387004e+03, 2.709140e+03, 3.074768e+03, 3.4 1382 2.387004e+03, 2.709140e+03, 3.074768e+03, 3.489760e+03, 3.960780e+03, 1362 4.495394e+03, 5.102185e+03, 5.790900e+03, 6.5 1383 4.495394e+03, 5.102185e+03, 5.790900e+03, 6.572600e+03, 7.459837e+03, // 90 1363 8.466860e+03, 9.609843e+03, 1.090714e+04, 1.2 1384 8.466860e+03, 9.609843e+03, 1.090714e+04, 1.237959e+04, 1.405083e+04, 1364 1.594771e+04, 1.810069e+04, 2.054434e+04, 2.3 1385 1.594771e+04, 1.810069e+04, 2.054434e+04, 2.331792e+04, 2.646595e+04, // 100 1365 3.003901e+04, 3.409446e+04, 3.869745e+04, 4.3 1386 3.003901e+04, 3.409446e+04, 3.869745e+04, 4.392189e+04, 4.985168e+04, 1366 5.658206e+04, 6.422112e+04, 7.289153e+04, 8.2 1387 5.658206e+04, 6.422112e+04, 7.289153e+04, 8.273254e+04, 9.390219e+04, // 110 1367 1.065799e+05 1388 1.065799e+05 1368 }; 1389 }; 1369 1390 1370 ///////////////////////////////////////////// 1391 /////////////////////////////////////////////////////////////////////// 1371 // 1392 // 1372 // The number of gamma for creation of splin 1393 // The number of gamma for creation of spline (near ion-min , G ~ 4 ) 1373 // 1394 // 1374 1395 1375 const G4int G4PAIySection::fRefGammaNumber = 1396 const G4int G4PAIySection::fRefGammaNumber = 29; 1376 1397 1377 // 1398 // 1378 // end of G4PAIySection implementation file 1399 // end of G4PAIySection implementation file 1379 // 1400 // 1380 ///////////////////////////////////////////// 1401 //////////////////////////////////////////////////////////////////////////// 1381 1402 1382 1403