Geant4  10.01.p03
G4SynchrotronRadiationInMat.hh
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27 // $Id: G4SynchrotronRadiationInMat.hh 68037 2013-03-13 14:15:08Z gcosmo $
28 //
29 // ------------------------------------------------------------
30 // GEANT 4 class header file
31 // CERN Geneva Switzerland
32 //
33 //
34 // History:
35 // 21-5-98 1 version , V. Grichine
36 // 28-05-01, V.Ivanchenko minor changes to provide ANSI -wall compilation
37 // 19-05-06, V.Ivanchenko rename from G4SynchrotronRadiation
38 //
39 //
40 // ------------------------------------------------------------
41 
42 #ifndef G4SynchrotronRadiationInMat_h
43 #define G4SynchrotronRadiationInMat_h 1
44 
45 #include "G4ios.hh"
46 #include "globals.hh"
47 #include "Randomize.hh"
48 #include "G4VDiscreteProcess.hh"
50 #include "G4FieldManager.hh"
51 #include "G4Field.hh"
52 #include "G4ThreeVector.hh"
53 #include "G4PropagatorInField.hh"
54 
55 #include "G4Track.hh"
56 #include "G4Step.hh"
57 
58 
59 #include "G4Gamma.hh"
60 #include "G4Electron.hh"
61 #include "G4Positron.hh"
62 
63 
64 #include "G4PhysicsTable.hh"
65 #include "G4PhysicsLogVector.hh"
66 
67 
69 {
70 public:
71 
72  G4SynchrotronRadiationInMat(const G4String& processName =
73  "SynchrotronRadiation",
75 
77 
78 private:
79 
82 
83 public:
84 
85  G4double GetMeanFreePath( const G4Track& track,
86  G4double previousStepSize,
88 
89  G4VParticleChange *PostStepDoIt( const G4Track& track,
90  const G4Step& Step );
91 
92  G4double GetPhotonEnergy( const G4Track& trackData,
93  const G4Step& stepData );
94 
96 
99 
102 
106 
108 
109  static G4double GetLambdaConst(){ return fLambdaConst; };
110  static G4double GetEnergyConst(){ return fEnergyConst; };
111 
112  void SetRootNumber(G4int rn){ fRootNumber = rn; };
114  void SetKsi(G4double ksi){ fKsi = ksi; };
115  void SetEta(G4double eta){ fEta = eta; };
116  void SetPsiGamma(G4double psg){ fPsiGamma = psg; };
117  void SetOrderAngleK(G4double ord){ fOrderAngleK = ord; }; // should be 1/3 or 2/3
118 
119 private:
120 
121  static const G4double fLambdaConst;
122 
123  static const G4double fEnergyConst;
124 
126 
127  const G4double
128  LowestKineticEnergy; // low energy limit of the cross-section formula
129 
130  const G4double
131  HighestKineticEnergy; // high energy limit of the cross-section formula
132 
133  G4int TotBin; // number of bins in the tables
134 
136 
140 
145 
146 
151 
154  G4double fKsi; // omega/omega_c
155  G4double fPsiGamma; // Psi-angle*gamma
157  G4double fOrderAngleK; // 1/3 or 2/3
158 
159 
162 
163 };
164 
165 #endif // end of G4SynchrotronRadiationInMat.hh
166 
G4double condition(const G4ErrorSymMatrix &m)
G4double GetMeanFreePath(const G4Track &track, G4double previousStepSize, G4ForceCondition *condition)
const G4ParticleDefinition * theGamma
int G4int
Definition: G4Types.hh:78
const G4ParticleDefinition * theElectron
static const G4double fIntegralProbabilityOfSR[200]
G4SynchrotronRadiationInMat(const G4String &processName="SynchrotronRadiation", G4ProcessType type=fElectromagnetic)
G4double GetPhotonEnergy(const G4Track &trackData, const G4Step &stepData)
G4SynchrotronRadiationInMat & operator=(const G4SynchrotronRadiationInMat &right)
bool G4bool
Definition: G4Types.hh:79
Definition: G4Step.hh:76
const G4ParticleDefinition * thePositron
G4VParticleChange * PostStepDoIt(const G4Track &track, const G4Step &Step)
Definition: Step.hh:41
double G4double
Definition: G4Types.hh:76
G4bool IsApplicable(const G4ParticleDefinition &)
G4ForceCondition
G4double GetRandomEnergySR(G4double, G4double)
G4ProcessType