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geant4/source/processes/electromagnetic/standard/include/G4IhIonisation.hh
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// 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: G4IhIonisation.hh,v 1.4 2000/04/25 14:33:01 maire Exp $
// GEANT4 tag $Name: geant4-03-00 $
//
//
// ------------------------------------------------------------
// 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
// ---------- G4IhIonisation physics process -----------
// by Laszlo Urban, 30 May 1997
// ************************************************************
// It is the first implementation of the NEW IONISATION
// PROCESS. ( delta rays + continuous energy loss)
// It calculates the ionisation for charged hadrons.
// ************************************************************
// corrected by L.Urban on 24/09/97
// corrected by L.Urban on 13/01/98
// 28/10/98: some cleanup , L.Urban
// ------------------------------------------------------------
#ifndef G4IhIonisation_h
#define G4IhIonisation_h 1
#include "G4ios.hh"
#include "globals.hh"
#include "Randomize.hh"
#include "G4VIhEnergyLoss.hh"
#include "G4EnergyLossTables.hh"
#include "globals.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4Electron.hh"
#include "G4Proton.hh"
#include "G4AntiProton.hh"
#include "G4PhysicsLogVector.hh"
#include "G4PhysicsLinearVector.hh"
class G4IhIonisation : public G4VIhEnergyLoss
{
public:
G4IhIonisation(const G4String& processName = "IhIoni");
~G4IhIonisation();
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 ) ;
protected:
virtual G4double ComputeMicroscopicCrossSection(
const G4ParticleDefinition& aParticleType,
G4double KineticEnergy,
G4double AtomicNumber);
private:
// hide assignment operator
G4IhIonisation & operator=(const G4IhIonisation &right);
G4IhIonisation(const G4IhIonisation&);
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;
const G4Electron* theElectron;
const G4Proton* theProton;
const G4AntiProton* theAntiProton;
const G4double* ParticleCutInKineticEnergy;
const G4double* DeltaCutInKineticEnergy ;
G4double ParticleCutInKineticEnergyNow ;
G4double DeltaCutInKineticEnergyNow ;
G4int NumberOfBuildPhysicsTableCalls ;
};
#include "G4IhIonisation.icc"
#endif