// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * 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. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // // $Id: G4SynchrotronRadiation.hh,v 1.4 2006-06-29 19:55:43 gunter Exp $ // GEANT4 tag $Name: not supported by cvs2svn $ // // ------------------------------------------------------------ // 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