// // ******************************************************************** // * 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. * // ******************************************************************** // // ------------------------------------------------------------ // GEANT 4 class header file // // History: // 21-5-98 1 version , V. Grichine // 28-05-01, V.Ivanchenko minor changes to provide ANSI -wall compilation // 19-05-06, V.Ivanchenko rename from G4SynchrotronRadiation // // ------------------------------------------------------------ #ifndef G4SynchrotronRadiationInMat_h #define G4SynchrotronRadiationInMat_h 1 #include "globals.hh" #include "G4Electron.hh" #include "G4Gamma.hh" #include "G4PhysicsLogVector.hh" #include "G4PhysicsTable.hh" #include "G4Positron.hh" #include "G4Step.hh" #include "G4ThreeVector.hh" #include "G4Track.hh" #include "G4TransportationManager.hh" #include "G4VDiscreteProcess.hh" #include "G4VParticleChange.hh" class G4ParticleDefinition; class G4PropagatorInField; class G4SynchrotronRadiationInMat : public G4VDiscreteProcess { public: explicit G4SynchrotronRadiationInMat( const G4String& processName = "SynchrotronRadiation", G4ProcessType type = fElectromagnetic); ~G4SynchrotronRadiationInMat(); G4SynchrotronRadiationInMat& operator=( const G4SynchrotronRadiationInMat& right) = delete; G4SynchrotronRadiationInMat(const G4SynchrotronRadiationInMat&) = delete; G4double GetMeanFreePath(const G4Track& track, G4double previousStepSize, G4ForceCondition* condition) override; G4VParticleChange* PostStepDoIt(const G4Track& track, const G4Step& Step) override; G4double GetPhotonEnergy(const G4Track& trackData, const G4Step& stepData); G4double GetRandomEnergySR(G4double, G4double); G4double GetProbSpectrumSRforInt(G4double); G4double GetIntProbSR(G4double); G4double GetProbSpectrumSRforEnergy(G4double); G4double GetEnergyProbSR(G4double); G4double GetIntegrandForAngleK(G4double); G4double GetAngleK(G4double); G4double GetAngleNumberAtGammaKsi(G4double); G4bool IsApplicable(const G4ParticleDefinition&) override; static G4double GetLambdaConst(); static G4double GetEnergyConst(); void SetRootNumber(G4int rn) { fRootNumber = rn; }; void SetVerboseLevel(G4int v) { fVerboseLevel = v; }; void SetKsi(G4double ksi) { fKsi = ksi; }; void SetEta(G4double eta) { fEta = eta; }; void SetPsiGamma(G4double psg) { fPsiGamma = psg; }; void SetOrderAngleK(G4double ord) { fOrderAngleK = ord; }; // should be 1/3 or 2/3 private: // Constant for calculation of mean free path // sqrt(3.) = 1.73... static constexpr G4double fLambdaConst = 1.73205080756887729352 * CLHEP::electron_mass_c2 / (2.5 * CLHEP::fine_structure_const * CLHEP::eplus * ::CLHEP::c_light); // Constant for calculation of characterictic energy static constexpr G4double fEnergyConst = 1.5 * CLHEP::c_light * CLHEP::c_light * CLHEP::eplus * CLHEP::hbar_Planck / CLHEP::electron_mass_c2; // Array of integral probability of synchrotron photons: // the corresponding energy = 0.0001*i*i*(characteristic energy) static const G4double fIntegralProbabilityOfSR[200]; const G4ParticleDefinition* theGamma; const G4ParticleDefinition* theElectron; const G4ParticleDefinition* thePositron; G4PropagatorInField* fFieldPropagator; const G4double LowestKineticEnergy; // low energy limit of the cross-section formula G4double CutInRange; G4double GammaCutInKineticEnergyNow; G4double ElectronCutInKineticEnergyNow; G4double PositronCutInKineticEnergyNow; G4double ParticleCutInKineticEnergyNow; G4double fAlpha; G4double fKsi; // omega/omega_c G4double fPsiGamma; // Psi-angle*gamma G4double fEta; // G4double fOrderAngleK; // 1/3 or 2/3 G4int fRootNumber; G4int fVerboseLevel; G4int secID = -1; // creator modelID }; #endif // end of G4SynchrotronRadiationInMat.hh