// 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: G4LowEnergyIonisation.hh,v 1.16 2000/11/03 10:29:51 pia Exp $ // GEANT4 tag $Name: geant4-03-00 $ // // // ------------------------------------------------------------ // GEANT 4 class header file // // For information related to this code contact: // CERN, IT Division, ASD group // --- G4LowEnergyIonisation physics process for electrons // by Alessandra Forti July 1999 // ************************************************************ // // 07.04.2000 Veronique Lefebure + Laszlo Urban // - First implemention of continuous energy loss // 14/07/99: corrections , L.Urban // 20/09/00 update fluctuations V.Ivanchenko // // Class description: // Low Energy Electromagnetic process, electron Ionisation // Further documentation available from http://www.ge.infn.it/geant4/lowE // ------------------------------------------------------------ #ifndef G4LowEnergyIonisation_h #define G4LowEnergyIonisation_h 1 // Base Class Headers #include "G4eLowEnergyLoss.hh" // Contained Variables Headers #include "G4LowEnergyUtilities.hh" #include "G4Electron.hh" #include "G4Positron.hh" typedef G4FirstLevel oneShellTable; typedef G4SecondLevel oneAtomTable; typedef G4ThirdLevel allAtomTable; class G4LowEnergyIonisation : public G4eLowEnergyLoss{ public: G4LowEnergyIonisation(const G4String& processName = "LowEnergyIoni"); ~G4LowEnergyIonisation(); G4bool IsApplicable(const G4ParticleDefinition&); void SetCutForLowEnSecPhotons(G4double); void SetCutForLowEnSecElectrons(G4double); void BuildPhysicsTable(const G4ParticleDefinition& aParticleType); G4double GetMeanFreePath(const G4Track& track, G4double previousStepSize, G4ForceCondition* condition ) ; inline G4double GetTransitionShell(G4int k){return(thePrimShVec(k));}; G4VParticleChange *PostStepDoIt(const G4Track& track, const G4Step& Step ) ; void PrintInfoDefinition(); G4double GetShellCrossSection(const G4double AtomicNumber, const G4int subshellindex, const G4double KineticEnergy) ; G4double GetShellCrossSectionwithCut(const G4double AtomicNumber, const G4int subshellindex, const G4double KineticEnergy, const G4double Tcut) ; G4double GetShellEnergyLosswithCut(const G4double AtomicNumber, const G4int subshellindex, const G4double KineticEnergy, const G4double Tcut) ; private: virtual G4double ComputeCrossSection(const G4double AtomicNumber, const G4double IncEnergy); G4double ComputeCrossSectionWithCut(const G4double AtomIndex, const G4double IncEnergy, const G4double CutEnergy); void BuildLossTable(const G4ParticleDefinition& aParticleType); void BuildShellCrossSectionTable(); void BuildBindingEnergyTable(); void BuildFluorTransitionTable(); void BuildSamplingCoeffTable(); void BuildZVec(); void BuildLambdaTable(const G4ParticleDefinition& aParticleType); private: // hide assignment operator G4LowEnergyIonisation & operator=(const G4LowEnergyIonisation &right); G4LowEnergyIonisation(const G4LowEnergyIonisation&); private: G4int SelectRandomShell(const G4int AtomIndex , const G4double IncEnergy , const G4double CutEnergy); G4Element* SelectRandomAtom(const G4DynamicParticle* aDynamicPhoton, G4Material* aMaterial); G4bool SelectRandomTransition(G4int, G4double*, const oneAtomTable*); G4double EnergySampling(const G4int AtomicNumber , const G4int ShellIndex , const G4double KinEn , const G4double deltaRayMinE = 0.1*eV); allAtomTable* allAtomShellCrossSec; allAtomTable* theFluorTransitionTable; allAtomTable* theSamplingCoeffTable; G4SecondLevel* theBindingEnergyTable; G4DataVector thePrimShVec; G4Data* ZNumVec; G4Data* ZNumVecFluor; G4LowEnergyUtilities util; G4double LowestKineticEnergy; G4double HighestKineticEnergy; G4int TotBin; G4double CutForLowEnergySecondaryPhotons; G4double CutForLowEnergySecondaryElectrons; G4double MeanFreePath; G4PhysicsTable* theMeanFreePathTable; }; #include "G4LowEnergyIonisation.icc" #endif