// This code implementation is the intellectual property of // the GEANT4 collaboration. // // By copying, distributing or modifying the Program (or any work // based on the Program) you indicate your acceptance of this statement, // and all its terms. // // $Id: G4PAIxSection.hh,v 1.4 1999/12/15 14:51:47 gunter Exp $ // GEANT4 tag $Name: geant4-03-01 $ // // // G4PAIxSection.hh -- header file // // GEANT 4 class header file --- Copyright CERN 1995 // CERB Geneva Switzerland // // for information related to this code, please, contact // CERN, CN Division, ASD Group // // Preparation of ionizing collision cross section according to Photo Absorption // Ionization (PAI) model for simulation of ionization energy losses in very thin // absorbers // // History: // 1st version 11.06.97, V. Grichine // 2nd version 30.11.97, V. Grichine // 27.10.99, V.Grichine: Bug fixed in constructors, 3rd constructor and // GetStepEnergyLoss(step) were added, fDelta = 0.005 #ifndef G4PAIXSECTION_HH #define G4PAIXSECTION_HH #include "G4ios.hh" #include "globals.hh" #include "Randomize.hh" #include"G4SandiaTable.hh" class G4PAIxSection { public: // Constructors G4PAIxSection( G4int materialIndex, G4double maxEnergyTransfer ) ; G4PAIxSection( G4int materialIndex, // for proton loss table G4double maxEnergyTransfer, G4double betaGammaSq , G4double** photoAbsCof, G4int intNumber ) ; G4PAIxSection( G4int materialIndex, // test constructor G4double maxEnergyTransfer, G4double betaGammaSq ) ; // G4PAIxSection(const G4PAIxSection& right) ; // Destructor ~G4PAIxSection() ; // Operators // G4PAIxSection& operator=(const G4PAIxSection& right) ; // G4int operator==(const G4PAIxSection& right)const ; // G4int operator!=(const G4PAIxSection& right)const ; // Methods // General control functions void InitPAI() ; void NormShift( G4double betaGammaSq ) ; void SplainPAI( G4double betaGammaSq ) ; // Physical methods void IntegralPAIxSection() ; G4double RutherfordIntegral( G4int intervalNumber, G4double limitLow, G4double limitHigh ) ; G4double ImPartDielectricConst( G4int intervalNumber, G4double energy ) ; G4double RePartDielectricConst(G4double energy) ; G4double DifPAIxSection( G4int intervalNumber, G4double betaGammaSq ) ; G4double SumOverInterval(G4int intervalNumber) ; G4double SumOverBorder( G4int intervalNumber, G4double energy ) ; G4double GetStepEnergyLoss( G4double step ) ; // Inline access functions G4int GetNumberOfGammas() const { return fNumberOfGammas ; } G4int GetSplineSize() const { return fSplineNumber ; } G4int GetIntervalNumber() const { return fIntervalNumber ; } G4double GetEnergyInterval(G4int i){ return fEnergyInterval[i] ; } G4double GetMeanEnergyLoss() const {return fIntegralPAIxSection[0] ; } G4double GetNormalizationCof() const { return fNormalizationCof ; } inline G4double GetPAItable(G4int i,G4int j) const ; inline G4double GetLorentzFactor(G4int i) const ; inline G4double GetSplineEnergy(G4int i) const ; inline G4double GetIntegralPAIxSection(G4int i) const ; protected : private : // Local class constants static const G4double fDelta ; // energy shift from interval border = 0.001 static const G4double fError ; // error in lin-log approximation = 0.005 static G4int fNumberOfGammas ; // = 111 ; static const G4double fLorentzFactor[112] ; // static gamma array static const G4int fRefGammaNumber ; // The number of gamma for creation of spline (15) G4int fIntervalNumber ; // The number of energy intervals G4double fNormalizationCof ; // Normalization cof for PhotoAbsorptionXsection // G4double fBetaGammaSq ; // (beta*gamma)^2 G4double fDensity ; // Current density G4double fElectronDensity ; // Current electron (number) density G4int fSplineNumber ; // Current size of spline // Arrays of Sandia coefficients G4double* fEnergyInterval ; G4double* fA1 ; G4double* fA2 ; G4double* fA3 ; G4double* fA4 ; static const G4int fMaxSplineSize ; // Max size of output splain arrays = 500 /* ****************** G4double* fSplineEnergy ; // energy points of splain G4double* fRePartDielectricConst ; // Real part of dielectric const G4double* fImPartDielectricConst ; // Imaginary part of dielectric const G4double* fIntegralTerm ; // Integral term in PAI cross section G4double* fDifPAIxSection ; // Differential PAI cross section G4double* fIntegralPAIxSection ; // Integral PAI cross section ? */ /////////////// G4double fSplineEnergy[500] ; // energy points of splain G4double fRePartDielectricConst[500] ; // Real part of dielectric const G4double fImPartDielectricConst[500] ; // Imaginary part of dielectric const G4double fIntegralTerm[500] ; // Integral term in PAI cross section G4double fDifPAIxSection[500] ; // Differential PAI cross section G4double fIntegralPAIxSection[500] ; // Integral PAI cross section ? G4double fPAItable[500][112] ; // Output array } ; //////////////// Inline methods ////////////////////////////////// // inline G4double G4PAIxSection::GetPAItable(G4int i, G4int j) const { return fPAItable[i][j] ; } inline G4double G4PAIxSection::GetLorentzFactor(G4int j) const { return fLorentzFactor[j] ; } inline G4double G4PAIxSection::GetSplineEnergy(G4int i) const { if(i < 1 || i > fSplineNumber) { G4Exception("Invalid argument in G4PAIxSection::GetSplineEnergy"); } return fSplineEnergy[i] ; } inline G4double G4PAIxSection::GetIntegralPAIxSection(G4int i) const { if(i < 1 || i > fSplineNumber) { G4Exception("Invalid argument in G4PAIxSection::GetIntegralPAIxSection"); } return fIntegralPAIxSection[i] ; } #endif // ----------------- end of G4PAIxSection header file -------------------