// 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: G4IeIonisation.hh,v 1.2.8.1 1999/12/07 20:50:49 gunter Exp $ // GEANT4 tag $Name: geant4-01-00 $ // // $Id: // ------------------------------------------------------------ // GEANT 4 class header file // // For information related to this code contact: // CERN, IT Division, ASD group // History: based on object model of // 2nd December 1995, G.Cosmo // ---------- G4IeIonisation physics process ----------- // by Laszlo Urban, 23 June 1998 // ************************************************************ // It is the first implementation of the IONISATION // PROCESS. ( delta rays + continuous energy loss) // using an INTEGRAL APPROACH instead of the differential // one used in the standard implementation . // ************************************************************ // 27/10/98 : minor changes+cleanup , L.Urban // ------------------------------------------------------------ #ifndef G4IeIonisation_h #define G4IeIonisation_h 1 #include "G4ios.hh" #include #include "globals.hh" #include "Randomize.hh" #include "G4IeEnergyLoss.hh" #include "G4EnergyLossTables.hh" #include "globals.hh" #include "G4Track.hh" #include "G4Step.hh" #include "G4Electron.hh" #include "G4Positron.hh" #include "G4Gamma.hh" #include "G4PhysicsLogVector.hh" #include "G4PhysicsLinearVector.hh" class G4IeIonisation : public G4IeEnergyLoss { public: G4IeIonisation(const G4String& processName = "IeIoni"); ~G4IeIonisation(); G4bool IsApplicable(const G4ParticleDefinition&); void SetPhysicsTableBining(G4double lowE, G4double highE, G4int nBins); void BuildPhysicsTable(const G4ParticleDefinition& aParticleType); void BuildLossTable(const G4ParticleDefinition& aParticleType); void BuildLambdaTable(const G4ParticleDefinition& aParticleType); void PrintInfoDefinition(); G4double PostStepGetPhysicalInteractionLength( const G4Track& track, G4double previousStepSize, G4ForceCondition* condition); G4VParticleChange *PostStepDoIt(const G4Track& track, const G4Step& Step ) ; G4double GetNlambda( G4double KineticEnergy,G4Material* material); protected: virtual G4double ComputeMicroscopicCrossSection( const G4ParticleDefinition& aParticleType, G4double KineticEnergy, G4double AtomicNumber); private: // hide assignment operator G4IeIonisation & operator=(const G4IeIonisation &right); G4IeIonisation(const G4IeIonisation&); void BuildNlambdaTable(const G4ParticleDefinition& aParticleType) ; void BuildNlambdaVector(const G4ParticleDefinition& aParticleType, G4int materialIndex, G4PhysicsLogVector* nlambdaVector) ; void BuildInverseNlambdaTable( const G4ParticleDefinition& aParticleType) ; void InvertNlambdaVector(const G4ParticleDefinition& aParticleType, G4int materialIndex, G4PhysicsLogVector* nlambdaVector) ; void BuildCoeffATable(const G4ParticleDefinition& aParticleType) ; void BuildCoeffBTable(const G4ParticleDefinition& aParticleType) ; void BuildCoeffCTable(const G4ParticleDefinition& aParticleType) ; void TestOfInversion(const G4ParticleDefinition& aParticleType, G4int printflag) ; private: // private data members ............................... G4PhysicsTable* theMeanFreePathTable; G4PhysicsTable* theNlambdaTable; G4PhysicsTable* theInverseNlambdaTable; G4PhysicsTable* theCoeffATable; G4PhysicsTable* theCoeffBTable; G4PhysicsTable* theCoeffCTable; G4double LowestKineticEnergy; G4double HighestKineticEnergy; G4int TotBin; G4double RTable ; // cut in range G4double CutInRange ; // particles , cuts in kinetic energy ........ const G4Electron* theElectron; const G4Positron* thePositron; const G4double* ParticleCutInKineticEnergy; const G4double* DeltaCutInKineticEnergy ; G4double ParticleCutInKineticEnergyNow ; G4double DeltaKineticEnergyCutNow ; G4int NumberOfBuildPhysicsTableCalls ; }; #include "G4IeIonisation.icc" #endif