Gabriele Cosmo
284 lines
8.9 KiB
C++
284 lines
8.9 KiB
C++
//
|
|
// ********************************************************************
|
|
// * 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: G4Scintillation.hh,v 1.11 2002/11/25 18:48:51 gum Exp $
|
|
// GEANT4 tag $Name: geant4-05-02-patch-01 $
|
|
//
|
|
//
|
|
////////////////////////////////////////////////////////////////////////
|
|
// Scintillation Light Class Definition
|
|
////////////////////////////////////////////////////////////////////////
|
|
//
|
|
// File: G4Scintillation.hh
|
|
// Description: Discrete Process - Generation of Scintillation Photons
|
|
// Version: 1.0
|
|
// Created: 1998-11-07
|
|
// Author: Peter Gumplinger
|
|
// Updated: 2002-11-21 change to user G4Poisson for small MeanNumPotons
|
|
// 2002-11-07 allow for fast and slow scintillation
|
|
// 2002-11-05 make use of constant material properties
|
|
// 2002-05-16 changed to inherit from VRestDiscreteProcess
|
|
// 2002-05-09 changed IsApplicable method
|
|
// 1999-10-29 add method and class descriptors
|
|
//
|
|
// mail: gum@triumf.ca
|
|
//
|
|
////////////////////////////////////////////////////////////////////////
|
|
|
|
#ifndef G4Scintillation_h
|
|
#define G4Scintillation_h 1
|
|
|
|
/////////////
|
|
// Includes
|
|
/////////////
|
|
|
|
#include "globals.hh"
|
|
#include "templates.hh"
|
|
#include "Randomize.hh"
|
|
#include "G4Poisson.hh"
|
|
#include "G4ThreeVector.hh"
|
|
#include "G4ParticleMomentum.hh"
|
|
#include "G4Step.hh"
|
|
#include "G4VRestDiscreteProcess.hh"
|
|
#include "G4OpticalPhoton.hh"
|
|
#include "G4DynamicParticle.hh"
|
|
#include "G4Material.hh"
|
|
#include "G4PhysicsTable.hh"
|
|
#include "G4MaterialPropertiesTable.hh"
|
|
#include "G4PhysicsOrderedFreeVector.hh"
|
|
|
|
// Class Description:
|
|
// RestDiscrete Process - Generation of Scintillation Photons.
|
|
// Class inherits publicly from G4VRestDiscreteProcess.
|
|
// Class Description - End:
|
|
|
|
/////////////////////
|
|
// Class Definition
|
|
/////////////////////
|
|
|
|
class G4Scintillation : public G4VRestDiscreteProcess
|
|
{
|
|
|
|
private:
|
|
|
|
//////////////
|
|
// Operators
|
|
//////////////
|
|
|
|
// G4Scintillation& operator=(const G4Scintillation &right);
|
|
|
|
public: // Without description
|
|
|
|
////////////////////////////////
|
|
// Constructors and Destructor
|
|
////////////////////////////////
|
|
|
|
G4Scintillation(const G4String& processName = "Scintillation");
|
|
|
|
// G4Scintillation(const G4Scintillation &right);
|
|
|
|
~G4Scintillation();
|
|
|
|
////////////
|
|
// Methods
|
|
////////////
|
|
|
|
public: // With description
|
|
|
|
// G4Scintillation Process has both PostStepDoIt (for energy
|
|
// deposition of particles in flight) and AtRestDoIt (for energy
|
|
// given to the medium by particles at rest)
|
|
|
|
G4bool IsApplicable(const G4ParticleDefinition& aParticleType);
|
|
// Returns true -> 'is applicable', for any particle type except
|
|
// for an 'opticalphoton'
|
|
|
|
G4double GetMeanFreePath(const G4Track& aTrack,
|
|
G4double ,
|
|
G4ForceCondition* );
|
|
// Returns infinity; i. e. the process does not limit the step,
|
|
// but sets the 'StronglyForced' condition for the DoIt to be
|
|
// invoked at every step.
|
|
|
|
G4double GetMeanLifeTime(const G4Track& aTrack,
|
|
G4ForceCondition* );
|
|
// Returns infinity; i. e. the process does not limit the time,
|
|
// but sets the 'StronglyForced' condition for the DoIt to be
|
|
// invoked at every step.
|
|
|
|
G4VParticleChange* PostStepDoIt(const G4Track& aTrack,
|
|
const G4Step& aStep);
|
|
G4VParticleChange* AtRestDoIt (const G4Track& aTrack,
|
|
const G4Step& aStep);
|
|
|
|
// These are the methods implementing the scintillation process.
|
|
|
|
void SetTrackSecondariesFirst(const G4bool state);
|
|
// If set, the primary particle tracking is interrupted and any
|
|
// produced scintillation photons are tracked next. When all
|
|
// have been tracked, the tracking of the primary resumes.
|
|
|
|
G4bool GetTrackSecondariesFirst() const;
|
|
// Returns the boolean flag for tracking secondaries first.
|
|
|
|
void SetScintillationYieldFactor(const G4double yieldfactor);
|
|
// Called to set the scintillation photon yield factor, needed when
|
|
// the yield is different for different types of particles. This
|
|
// scales the yield obtained from the G4MaterialPropertiesTable.
|
|
|
|
G4double GetScintillationYieldFactor() const;
|
|
// Returns the photon yield factor.
|
|
|
|
void SetScintillationExcitationRatio(const G4double excitationratio);
|
|
// Called to set the scintillation exciation ratio, needed when
|
|
// the scintillation level excitation is different for different
|
|
// types of particles. This overwrites the YieldRatio obtained
|
|
// from the G4MaterialPropertiesTable.
|
|
|
|
G4double GetScintillationExcitationRatio() const;
|
|
// Returns the scintillation level excitation ratio.
|
|
|
|
G4PhysicsTable* GetFastIntegralTable() const;
|
|
// Returns the address of the fast scintillation integral table.
|
|
|
|
G4PhysicsTable* GetSlowIntegralTable() const;
|
|
// Returns the address of the slow scintillation integral table.
|
|
|
|
void DumpPhysicsTable() const;
|
|
// Prints the fast and slow scintillation integral tables.
|
|
|
|
private:
|
|
|
|
void BuildThePhysicsTable();
|
|
// It builds either the fast or slow scintillation integral table;
|
|
// or both.
|
|
|
|
///////////////////////
|
|
// Class Data Members
|
|
///////////////////////
|
|
|
|
protected:
|
|
|
|
G4PhysicsTable* theSlowIntegralTable;
|
|
G4PhysicsTable* theFastIntegralTable;
|
|
|
|
private:
|
|
|
|
G4bool fTrackSecondariesFirst;
|
|
|
|
G4double YieldFactor;
|
|
|
|
G4double ExcitationRatio;
|
|
|
|
};
|
|
|
|
////////////////////
|
|
// Inline methods
|
|
////////////////////
|
|
|
|
inline
|
|
G4bool G4Scintillation::IsApplicable(const G4ParticleDefinition& aParticleType)
|
|
{
|
|
if (aParticleType.GetParticleName() == "opticalphoton"){
|
|
return false;
|
|
} else {
|
|
return true;
|
|
}
|
|
}
|
|
|
|
inline
|
|
void G4Scintillation::SetTrackSecondariesFirst(const G4bool state)
|
|
{
|
|
fTrackSecondariesFirst = state;
|
|
}
|
|
|
|
inline
|
|
G4bool G4Scintillation::GetTrackSecondariesFirst() const
|
|
{
|
|
return fTrackSecondariesFirst;
|
|
}
|
|
|
|
inline
|
|
void G4Scintillation::SetScintillationYieldFactor(const G4double yieldfactor)
|
|
{
|
|
YieldFactor = yieldfactor;
|
|
}
|
|
|
|
inline
|
|
G4double G4Scintillation::GetScintillationYieldFactor() const
|
|
{
|
|
return YieldFactor;
|
|
}
|
|
|
|
inline
|
|
void G4Scintillation::SetScintillationExcitationRatio(const G4double excitationratio)
|
|
{
|
|
ExcitationRatio = excitationratio;
|
|
}
|
|
|
|
inline
|
|
G4double G4Scintillation::GetScintillationExcitationRatio() const
|
|
{
|
|
return ExcitationRatio;
|
|
}
|
|
|
|
inline
|
|
G4PhysicsTable* G4Scintillation::GetSlowIntegralTable() const
|
|
{
|
|
return theSlowIntegralTable;
|
|
}
|
|
|
|
inline
|
|
G4PhysicsTable* G4Scintillation::GetFastIntegralTable() const
|
|
{
|
|
return theFastIntegralTable;
|
|
}
|
|
|
|
inline
|
|
void G4Scintillation::DumpPhysicsTable() const
|
|
{
|
|
if (theFastIntegralTable) {
|
|
G4int PhysicsTableSize = theFastIntegralTable->entries();
|
|
G4PhysicsOrderedFreeVector *v;
|
|
|
|
for (G4int i = 0 ; i < PhysicsTableSize ; i++ )
|
|
{
|
|
v = (G4PhysicsOrderedFreeVector*)(*theFastIntegralTable)[i];
|
|
v->DumpValues();
|
|
}
|
|
}
|
|
|
|
if (theSlowIntegralTable) {
|
|
G4int PhysicsTableSize = theSlowIntegralTable->entries();
|
|
G4PhysicsOrderedFreeVector *v;
|
|
|
|
for (G4int i = 0 ; i < PhysicsTableSize ; i++ )
|
|
{
|
|
v = (G4PhysicsOrderedFreeVector*)(*theSlowIntegralTable)[i];
|
|
v->DumpValues();
|
|
}
|
|
}
|
|
}
|
|
|
|
#endif /* G4Scintillation_h */
|