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geant4/source/processes/electromagnetic/xrays/include/G4SynchrotronRadiation.hh
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//
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// $Id: G4SynchrotronRadiation.hh,v 1.4 2006/06/29 19:55:43 gunter Exp $
// GEANT4 tag $Name: geant4-09-01 $
//
// ------------------------------------------------------------
// GEANT 4 class header file
// CERN Geneva Switzerland
//
//
// History:
// 21-5-98 1 version , V. Grichine
// 28-05-01, V.Ivanchenko minor changes to provide ANSI -wall compilation
// 23-05-06, H. Burkhardt: Energy spectrum from function rather than table
//
//
// ------------------------------------------------------------
#ifndef G4SynchrotronRadiation_h
#define G4SynchrotronRadiation_h 1
#include "G4ios.hh"
#include "globals.hh"
#include "Randomize.hh"
#include "G4VDiscreteProcess.hh"
#include "G4TransportationManager.hh"
#include "G4FieldManager.hh"
#include "G4Field.hh"
#include "G4ThreeVector.hh"
#include "G4PropagatorInField.hh"
#include "G4Track.hh"
#include "G4Step.hh"
#include "G4Gamma.hh"
#include "G4Electron.hh"
#include "G4Positron.hh"
class G4SynchrotronRadiation : public G4VDiscreteProcess
{
public:
G4SynchrotronRadiation(const G4String& pName = "SynRad",
G4ProcessType type = fElectromagnetic);
virtual ~G4SynchrotronRadiation();
G4double GetMeanFreePath( const G4Track& track,
G4double previousStepSize,
G4ForceCondition* condition );
G4VParticleChange *PostStepDoIt( const G4Track& track,
const G4Step& Step );
G4double GetPhotonEnergy( const G4Track& trackData,
const G4Step& stepData );
G4double GetRandomEnergySR( G4double, G4double );
G4double InvSynFracInt(G4double x);
G4double Chebyshev(G4double a,G4double b,const G4double c[],G4int m,G4double x);
G4bool IsApplicable(const G4ParticleDefinition&);
void BuildPhysicsTable(const G4ParticleDefinition& );
void PrintInfoDefinition();
private:
G4SynchrotronRadiation & operator=(const G4SynchrotronRadiation &right);
G4SynchrotronRadiation(const G4SynchrotronRadiation&);
G4ParticleDefinition* theGamma;
const G4ParticleDefinition* theElectron;
const G4ParticleDefinition* thePositron;
G4double fLambdaConst;
G4double fEnergyConst;
G4PropagatorInField* fFieldPropagator;
};
////////////////////////// INLINE METHODS /////////////////////////////
inline G4bool
G4SynchrotronRadiation::IsApplicable( const G4ParticleDefinition& particle )
{
return ( ( &particle == (const G4ParticleDefinition *)theElectron ) ||
( &particle == (const G4ParticleDefinition *)thePositron ) );
// return ( particle.GetPDGCharge() != 0.0 );
}
inline G4double G4SynchrotronRadiation::Chebyshev(G4double a,G4double b,const G4double c[],G4int m,G4double x)
{
G4double y;
G4double y2=2.0*(y=(2.0*x-a-b)/(b-a)); // Change of variable.
G4double d=0,dd=0;
for (G4int j=m-1;j>=1;j--) // Clenshaw's recurrence.
{ G4double sv=d;
d=y2*d-dd+c[j];
dd=sv;
}
return y*d-dd+0.5*c[0];
}
#endif // end of G4SynchrotronRadiation.hh