|
||||
File indexing completed on 2025-01-31 09:22:04
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 // 0030 // Author: A. Forti 0031 // Maria Grazia Pia (Maria.Grazia.Pia@cern.ch) 0032 // 0033 // History: 0034 // ----------- 0035 // 02 Mar 1999 A. Forti 1st implementation 0036 // 11 Aug 2001 MGP Major revision according to a design iteration 0037 // 0038 // ------------------------------------------------------------------- 0039 0040 // Class description: 0041 // Low Energy Electromagnetic process, Rayleigh effect 0042 // Further documentation available from http://www.ge.infn.it/geant4/lowE 0043 0044 // ------------------------------------------------------------------- 0045 0046 #ifndef G4RDLOWENERGYRAYLEIGH_HH 0047 #define G4RDLOWENERGYRAYLEIGH_HH 1 0048 0049 #include "globals.hh" 0050 #include "G4VDiscreteProcess.hh" 0051 class G4Track; 0052 class G4Step; 0053 class G4ParticleDefinition; 0054 class G4VParticleChange; 0055 class G4RDVEMDataSet; 0056 class G4RDVCrossSectionHandler; 0057 0058 class G4LowEnergyRayleigh : public G4VDiscreteProcess { 0059 0060 public: 0061 0062 G4LowEnergyRayleigh(const G4String& processName ="LowEnRayleigh"); 0063 0064 ~G4LowEnergyRayleigh(); 0065 0066 G4bool IsApplicable(const G4ParticleDefinition&); 0067 0068 void BuildPhysicsTable(const G4ParticleDefinition& photon); 0069 0070 G4VParticleChange* PostStepDoIt(const G4Track& aTrack, const G4Step& aStep); 0071 0072 // For testing purpose only 0073 G4double DumpMeanFreePath(const G4Track& aTrack, 0074 G4double previousStepSize, 0075 G4ForceCondition* condition) 0076 { return GetMeanFreePath(aTrack, previousStepSize, condition); } 0077 0078 protected: 0079 0080 G4double GetMeanFreePath(const G4Track& aTrack, 0081 G4double previousStepSize, 0082 G4ForceCondition* condition); 0083 0084 private: 0085 0086 // Hide copy constructor and assignment operator as private 0087 G4LowEnergyRayleigh& operator=(const G4LowEnergyRayleigh &right); 0088 G4LowEnergyRayleigh(const G4LowEnergyRayleigh& ); 0089 0090 G4double lowEnergyLimit; // low energy limit applied to the process 0091 G4double highEnergyLimit; // high energy limit applied to the process 0092 0093 G4RDVEMDataSet* meanFreePathTable; 0094 G4RDVEMDataSet* formFactorData; 0095 0096 G4RDVCrossSectionHandler* crossSectionHandler; 0097 0098 const G4double intrinsicLowEnergyLimit; // intrinsic validity range 0099 const G4double intrinsicHighEnergyLimit; 0100 0101 }; 0102 0103 #endif 0104 0105 0106 0107 0108 0109 0110 0111 0112 0113 0114 0115 0116 0117
[ Source navigation ] | [ Diff markup ] | [ Identifier search ] | [ general search ] |
This page was automatically generated by the 2.3.7 LXR engine. The LXR team |