// This code implementation is the intellectual property of // the RD44 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: G4MuNuclearInteraction.hh,v 1.1 1998/11/23 18:14:51 hpw Exp $ // GEANT4 tag $Name: geant4-00 $ // // $Id: // ------------------------------------------------------------ // GEANT 4 class header file // // For information related to this code contact: // CERN, CN Division, ASD group // History: first implementation, based on object model of // 2nd December 1995, G.Cosmo // -------- G4MuNuclearInteraction physics process --------- // by Laszlo Urban, May 1998 // ************************************************************ #ifndef G4MuNuclearInteraction_h #define G4MuNuclearInteraction_h 1 #include "G4ios.hh" #include "globals.hh" #include "Randomize.hh" #include "G4VDiscreteProcess.hh" #include "G4Track.hh" #include "G4Step.hh" #include "G4MuonMinus.hh" #include "G4MuonPlus.hh" #include "G4PionZero.hh" #include "G4OrderedTable.hh" #include "G4PhysicsTable.hh" #include "G4ElementTable.hh" #include "G4PhysicsLogVector.hh" #include "G4ParametrizedHadronicVertex.hh" class G4MuNuclearInteraction : public G4VDiscreteProcess { public: G4MuNuclearInteraction(const G4String& processName = "MuNucl"); ~G4MuNuclearInteraction(); G4bool IsApplicable(const G4ParticleDefinition&); void SetPhysicsTableBining(G4double lowE, G4double highE, G4int nBins); void BuildPhysicsTable(const G4ParticleDefinition& ParticleType); void PrintInfoDefinition() ; G4double GetMeanFreePath(const G4Track& track, G4double previousStepSize, G4ForceCondition* condition ) ; G4VParticleChange *PostStepDoIt(const G4Track& track, const G4Step& Step ) ; protected: G4double ComputeMeanFreePath( const G4ParticleDefinition* ParticleType, G4double KineticEnergy, const G4Material* aMaterial); void ComputePartialSumSigma( const G4ParticleDefinition* ParticleType, G4double KineticEnergy, const G4Material* aMaterial); virtual G4double ComputeMicroscopicCrossSection( const G4ParticleDefinition* ParticleType, G4double KineticEnergy, G4double AtomicNumber, G4double AtomicMass); virtual G4double ComputeDMicroscopicCrossSection( const G4ParticleDefinition* ParticleType, G4double KineticEnergy, G4double AtomicNumber, G4double AtomicMass, G4double epsilon); private: G4MuNuclearInteraction & operator=(const G4MuNuclearInteraction &right); G4MuNuclearInteraction(const G4MuNuclearInteraction&); G4Element* SelectRandomAtom(G4Material* aMaterial) const; void MakeSamplingTables( const G4ParticleDefinition* ParticleType ); private: G4PhysicsTable* theMeanFreePathTable; G4PhysicsTable* theCrossSectionTable ; G4OrderedTable PartialSumSigma; G4double LowestKineticEnergy; G4double HighestKineticEnergy; G4int TotBin; //cut from R.P. Kokoulin const G4double CutFixed ; // for the atomic weight conversion G4double GramPerMole ; const G4MuonMinus* theMuonMinus; const G4MuonPlus* theMuonPlus; const G4PionZero* thePionZero; // tables for sampling .............. static G4int nzdat,ntdat,NBIN ; static G4double zdat[5],adat[5],tdat[8] ; static G4double ya[1000],proba[5][8][1000] ; // for the hadronic final state; use base cass * in next release G4ParametrizedHadronicVertex theHadronicVertex; }; #include "G4MuNuclearInteraction.icc" #endif