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Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitatio 16 // * for the full disclaimer and the limitation of liability. * 17 // * 17 // * * 18 // * This code implementation is the result 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboratio 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distri 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you ag 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publicati 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Sof 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************* 24 // ******************************************************************** 25 // 25 // >> 26 // >> 27 // $Id: G4TransitionRadiation.hh,v 1.9 2006/06/29 19:55:47 gunter Exp $ >> 28 // GEANT4 tag $Name: geant4-09-03-patch-01 $ >> 29 // >> 30 // G4TransitionRadiation -- header file >> 31 // 26 // Class for description of transition radiat 32 // Class for description of transition radiation generated 27 // by charged particle crossed interface betw 33 // by charged particle crossed interface between material 1 28 // and material 2 (1 -> 2). Transition radiati 34 // and material 2 (1 -> 2). Transition radiation could be of kind: 29 // - optical back 35 // - optical back 30 // - optical forward 36 // - optical forward 31 // - X-ray forward (for relativistic case Tk 37 // - X-ray forward (for relativistic case Tkin/mass >= 10^2) 32 // 38 // 33 // GEANT 4 class header file --- Copyright CER 39 // GEANT 4 class header file --- Copyright CERN 1995 >> 40 // CERB Geneva Switzerland 34 // 41 // >> 42 // for information related to this code, please, contact >> 43 // CERN, CN Division, ASD Group 35 // History: 44 // History: 36 // 18.12.97, V. Grichine (Vladimir.Grichine@ce 45 // 18.12.97, V. Grichine (Vladimir.Grichine@cern.ch) 37 // 02.02.00, V.Grichine, new data fEnergy and 46 // 02.02.00, V.Grichine, new data fEnergy and fVarAngle for double 38 // numerical integration 47 // numerical integration in inherited classes 39 // 03.06.03, V.Ivanchenko fix compilation warn 48 // 03.06.03, V.Ivanchenko fix compilation warnings 40 // 28.07.05, P.Gumplinger add G4ProcessType to 49 // 28.07.05, P.Gumplinger add G4ProcessType to constructor 41 50 42 #ifndef G4TransitionRadiation_h 51 #ifndef G4TransitionRadiation_h 43 #define G4TransitionRadiation_h 52 #define G4TransitionRadiation_h 44 53 45 #include "globals.hh" << 54 46 #include "G4ParticleDefinition.hh" << 47 #include "G4Step.hh" << 48 #include "G4Track.hh" << 49 #include "G4VDiscreteProcess.hh" 55 #include "G4VDiscreteProcess.hh" 50 #include "G4VParticleChange.hh" << 56 #include "G4Material.hh" >> 57 // #include "G4OpBoundaryProcess.hh" 51 58 52 class G4TransitionRadiation : public G4VDiscre << 59 class G4TransitionRadiation : public G4VDiscreteProcess 53 { 60 { 54 public: << 61 public: 55 explicit G4TransitionRadiation(const G4Strin << 62 56 G4ProcessType << 63 // Constructors >> 64 >> 65 >> 66 G4TransitionRadiation( const G4String& processName = "TR", >> 67 G4ProcessType type = fElectromagnetic) ; >> 68 >> 69 >> 70 // G4TransitionRadiation(const G4TransitionRadiation& right) ; >> 71 >> 72 // Destructor >> 73 >> 74 virtual ~G4TransitionRadiation() ; >> 75 >> 76 // Operators >> 77 // G4TransitionRadiation& operator=(const G4TransitionRadiation& right) ; >> 78 // G4int operator==(const G4TransitionRadiation& right)const ; >> 79 // G4int operator!=(const G4TransitionRadiation& right)const ; >> 80 >> 81 // Methods >> 82 >> 83 G4bool IsApplicable(const G4ParticleDefinition& aParticleType) >> 84 { >> 85 return ( aParticleType.GetPDGCharge() != 0.0 ); >> 86 } >> 87 >> 88 G4double GetMeanFreePath(const G4Track&, >> 89 G4double, >> 90 G4ForceCondition* condition) >> 91 { >> 92 *condition = Forced; >> 93 return DBL_MAX; // so TR doesn't limit mean free path >> 94 } >> 95 >> 96 G4VParticleChange* PostStepDoIt(const G4Track&, >> 97 const G4Step&) >> 98 { >> 99 ClearNumberOfInteractionLengthLeft(); >> 100 return &aParticleChange; >> 101 } >> 102 >> 103 >> 104 >> 105 >> 106 virtual >> 107 G4double SpectralAngleTRdensity( G4double energy, >> 108 G4double varAngle ) const = 0 ; 57 109 58 virtual ~G4TransitionRadiation(); << 110 G4double IntegralOverEnergy( G4double energy1, >> 111 G4double energy2, >> 112 G4double varAngle ) const ; 59 113 60 G4TransitionRadiation(const G4TransitionRadi << 114 G4double IntegralOverAngle( G4double energy, 61 G4TransitionRadiation& operator=(const G4Tra << 115 G4double varAngle1, >> 116 G4double varAngle2 ) const ; 62 117 63 // Methods << 118 G4double AngleIntegralDistribution( G4double varAngle1, >> 119 G4double varAngle2 ) const ; 64 120 65 G4bool IsApplicable(const G4ParticleDefiniti << 121 G4double EnergyIntegralDistribution( G4double energy1, >> 122 G4double energy2 ) const ; 66 123 67 virtual G4double GetMeanFreePath(const G4Tra << 68 G4ForceCond << 69 124 70 virtual G4VParticleChange* PostStepDoIt(cons << 71 cons << 72 125 73 virtual void ProcessDescription(std::ostream << 126 // Access functions 74 virtual void DumpInfo() const override { Pro << 75 127 76 virtual G4double SpectralAngleTRdensity(G4do << 77 G4do << 78 128 79 G4double IntegralOverEnergy(G4double energy1 << 129 protected : 80 G4double varAngl << 81 130 82 G4double IntegralOverAngle(G4double energy, << 131 G4int fMatIndex1 ; // index of the 1st material 83 G4double varAngle << 132 G4int fMatIndex2 ; // index of the 2nd material 84 133 85 G4double AngleIntegralDistribution(G4double << 134 // private : 86 G4double << 87 135 88 G4double EnergyIntegralDistribution(G4double << 136 G4double fGamma ; >> 137 G4double fEnergy ; >> 138 G4double fVarAngle ; 89 139 90 protected: << 140 // Local constants 91 // Local constants << 141 static const G4int fSympsonNumber ; // Accuracy of Sympson integration 10 92 // Accuracy of Sympson integration << 142 static const G4int fGammaNumber ; // = 15 93 static constexpr G4int fSympsonNumber = 100; << 143 static const G4int fPointNumber ; // = 100 94 static constexpr G4int fGammaNumber = 15; << 95 static constexpr G4int fPointNumber = 100; << 96 144 97 G4double fGamma; << 145 G4double fMinEnergy ; // min TR energy 98 G4double fEnergy; << 146 G4double fMaxEnergy ; // max TR energy 99 G4double fVarAngle; << 147 G4double fMaxTheta ; // max theta of TR quanta 100 148 101 G4double fMinEnergy; // min TR energy << 149 G4double fSigma1 ; // plasma energy Sq of matter1 102 G4double fMaxEnergy; // max TR energy << 150 G4double fSigma2 ; // plasma energy Sq of matter2 103 G4double fMaxTheta; // max theta of TR qu << 104 151 105 G4double fSigma1; // plasma energy Sq of ma << 106 G4double fSigma2; // plasma energy Sq of ma << 107 152 108 G4int fMatIndex1; // index of the 1st mater << 153 } ; 109 G4int fMatIndex2; // index of the 2nd mater << 110 }; << 111 154 112 #endif // G4TransitionRadiation_h << 155 #endif // G4TransitionRadiation_h 113 156