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Warning, file /include/Geant4/G4eDPWACoulombScatteringModel.hh was not indexed or was modified since last indexation (in which case cross-reference links may be missing, inaccurate or erroneous).
0001 // 0002 // ******************************************************************** 0003 // * License and Disclaimer * 0004 // * * 0005 // * The Geant4 software is copyright of the Copyright Holders of * 0006 // * the Geant4 Collaboration. It is provided under the terms and * 0007 // * conditions of the Geant4 Software License, included in the file * 0008 // * LICENSE and available at http://cern.ch/geant4/license . These * 0009 // * include a list of copyright holders. * 0010 // * * 0011 // * Neither the authors of this software system, nor their employing * 0012 // * institutes,nor the agencies providing financial support for this * 0013 // * work make any representation or warranty, express or implied, * 0014 // * regarding this software system or assume any liability for its * 0015 // * use. Please see the license in the file LICENSE and URL above * 0016 // * for the full disclaimer and the limitation of liability. * 0017 // * * 0018 // * This code implementation is the result of the scientific and * 0019 // * technical work of the GEANT4 collaboration. * 0020 // * By using, copying, modifying or distributing the software (or * 0021 // * any work based on the software) you agree to acknowledge its * 0022 // * use in resulting scientific publications, and indicate your * 0023 // * acceptance of all terms of the Geant4 Software license. * 0024 // ******************************************************************** 0025 // 0026 // 0027 // ------------------------------------------------------------------- 0028 // 0029 // GEANT4 Class header file 0030 // 0031 // 0032 // File name: G4eDPWACoulombScatteringModel 0033 // 0034 // Author: Mihaly Novak 0035 // 0036 // Creation date: 02.07.2020 0037 // 0038 // Modifications: 0039 // 0040 // Class Description: 0041 // 0042 // e-/e+ Coulomb scattering model based on numerical Differential Cross Sections 0043 // (DCS) obtained by Dirac Partial Wave Analysis (DPWA) and supplied by the 0044 // G4eDPWAElasticDCS class. 0045 // The model contains the possibility to incorporate the effects of angular 0046 // deflections of sub-threshold ionisation intercations when it's described by 0047 // the condensed history model. Note, this must be inactivated (by setting the 0048 // `isscpcor` input argument of the CTR to false) when ionisation is described 0049 // with a classical, event by event based simulation model instead of usign the 0050 // condensed history approach (otherwise, the corresponding angular defelctions 0051 // will be "double counted"). 0052 // 0053 // ------------------------------------------------------------------- 0054 0055 0056 0057 #ifndef G4eDPWACoulombScatteringModel_h 0058 #define G4eDPWACoulombScatteringModel_h 1 0059 0060 #include "G4VEmModel.hh" 0061 #include "globals.hh" 0062 0063 class G4eDPWAElasticDCS; 0064 class G4ParticleChangeForGamma; 0065 class G4ParticleDefinition; 0066 class G4DataVector; 0067 0068 class G4eDPWACoulombScatteringModel : public G4VEmModel { 0069 0070 public: 0071 0072 /** 0073 * Constructor. 0074 * 0075 * @param[in] ismixed Indicates if the model is for mixed or for pure single 0076 * Coulomb scattering. Different type of tables are pre- 0077 * pared for sampling polar angle of Coulomb scattering 0078 * for mixed and for pure single scattering models: cosine 0079 * of the polar scattering angle can be sampled in a 0080 * restriced inteval (see fMuMin parameter). 0081 * @param[in] isscpcor Indicates if scattering power correction should be used. 0082 * Note, scattering power correction accounts the effects 0083 * angular deflections due to sub-threshold ionisations 0084 * when ionisation is described by using condensed history 0085 * model (should be active only in this case). 0086 */ 0087 G4eDPWACoulombScatteringModel(G4bool ismixed=false, G4bool isscpcor=true); 0088 0089 ~G4eDPWACoulombScatteringModel() override; 0090 0091 // 0092 // Interface methods: 0093 0094 void Initialise(const G4ParticleDefinition*, const G4DataVector&) override; 0095 0096 void InitialiseLocal(const G4ParticleDefinition*, G4VEmModel*) override; 0097 0098 G4double ComputeCrossSectionPerAtom(const G4ParticleDefinition*, G4double ekin, 0099 G4double Z, G4double A, G4double prodcut, 0100 G4double emax) override; 0101 0102 void SampleSecondaries(std::vector<G4DynamicParticle*>*, 0103 const G4MaterialCutsCouple*, 0104 const G4DynamicParticle*, 0105 G4double tmin, 0106 G4double maxEnergy) override; 0107 0108 G4double MinPrimaryEnergy(const G4Material*, const G4ParticleDefinition*, 0109 G4double) override; 0110 0111 void SetTheDCS(G4eDPWAElasticDCS* theDCS) { fTheDCS = theDCS; } 0112 0113 G4eDPWAElasticDCS* GetTheDCS() { return fTheDCS; } 0114 0115 0116 private: 0117 0118 // Indicates if the model is mixed: MSC for soft (theta<theta_c), Singe 0119 // Scattering(SS) for hard scatterings(theta>theta_c). SS otherwise. 0120 // Note, that while the model provides restricted (elastic and transport) 0121 // cross sections, it's responsible to handle, i.e. provide final state, 0122 // only for the Singe Scattering part in case of a mixed model. 0123 G4bool fIsMixedModel; 0124 // indicates if scattering power correction should be applied: correction due 0125 // to deflection in case of sub-threshold, inelastic interactions -> only in 0126 // case of condensed history simulation of inonisation! 0127 G4bool fIsScpCorrection; 0128 // mu(theta)=0.5[1-cos(theta)]: the model porvides final states \in [fMuMin,1] 0129 // NOTE: `theta` for this limit can be set in `G4EmParameters::SetMscThetaLimit` 0130 G4double fMuMin; 0131 // the object that provides cross sections and polar angle of scattering 0132 G4eDPWAElasticDCS* fTheDCS; 0133 // particle change 0134 G4ParticleChangeForGamma* fParticleChange; 0135 0136 }; 0137 0138 #endif
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