// // ******************************************************************** // * DISCLAIMER * // * * // * The following disclaimer summarizes all the specific disclaimers * // * of contributors to this software. The specific disclaimers,which * // * govern, are listed with their locations in: * // * http://cern.ch/geant4/license * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. * // * * // * 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 1.20.2.2 2001/06/28 20:19:23 gunter Exp $ // GEANT4 tag $Name: $ // // // ------------------------------------------------------------ // GEANT 4 class header file // // --- 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) ; void SetLowEnergyLimit(G4double val) {if(val > 0.0) lEnergyLimit = val;}; private: virtual G4double ComputeCrossSection(const G4double AtomicNumber, const G4double IncEnergy); G4double ComputeCrossSectionWithCut(const G4double AtomIndex, const G4double IncEnergy, const G4double CutEnergy); G4double ComputeMicroscopicCrossSection(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* ZNumVec; G4DataVector* ZNumVecFluor; G4PhysicsTable* theMeanFreePathTable; G4double CutForLowEnergySecondaryPhotons; G4double CutForLowEnergySecondaryElectrons; G4double MeanFreePath; G4double lowestKineticEnergy; G4double highestKineticEnergy; G4int TotBin; G4LowEnergyUtilities util; G4DataVector thePrimShVec; G4double lEnergyLimit; }; #include "G4LowEnergyIonisation.icc" #endif