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G4QIonIonElastic.hh
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26 // $Id$
27 //
28 // ---------------- G4QIonIonElastic header ----------------
29 // by Mikhail Kossov, December 2006.
30 // Header of G4QIonIonElastic class (A+A) of the CHIPS Simulation Branch in GEANT4
31 // -------------------------------------------------------------------------------
32 // This is a unique CHIPS class for the Ion-Ion Elastic Scattering Prosesses
33 // -------------------------------------------------------------------------------
34 // @@ This class is on the testing level @@
35 // -------------------------------------------------------------------------------
36 // Short description: a simple process for the Ion-Ion elastic scattering.
37 // For heavy by heavy ions it can reach 50% of the total cross-section.
38 // -----------------------------------------------------------------------
39 
40 #ifndef G4QIonIonElastic_hh
41 #define G4QIonIonElastic_hh
42 
43 // GEANT4 Headers
44 #include "globals.hh"
45 #include "G4ios.hh"
46 #include "Randomize.hh"
47 #include "G4VDiscreteProcess.hh"
48 #include "G4Track.hh"
49 #include "G4Step.hh"
50 #include "G4ParticleTypes.hh"
51 #include "G4VParticleChange.hh"
52 #include "G4ParticleDefinition.hh"
53 #include "G4DynamicParticle.hh"
54 #include "G4ThreeVector.hh"
55 #include "G4LorentzVector.hh"
56 
57 // CHIPS Headers
58 #include "G4QIonIonCrossSection.hh"
61 #include "G4QIsotope.hh"
62 #include "G4QCHIPSWorld.hh"
63 #include "G4QHadron.hh"
64 #include <vector>
65 
67 {
68 public:
69 
70  // Constructor
71  G4QIonIonElastic(const G4String& processName ="CHIPS_IonIonElasticScattering");
72 
73  // Destructor
75 
76  G4bool IsApplicable(const G4ParticleDefinition& particle);
77 
78  G4double GetMeanFreePath(const G4Track& aTrack, G4double previousStepSize,
80  // It returns the MeanFreePath of the process for the current track :
81  // (energy, material)
82  // The previousStepSize and G4ForceCondition* are not used.
83  // This function overloads a virtual function of the base class.
84  // It is invoked by the ProcessManager of the Particle.
85 
86 
87  G4VParticleChange* PostStepDoIt(const G4Track& aTrack, const G4Step& aStep);
88  // It computes the final state of the process (at end of step),
89  // returned as a ParticleChange object.
90  // This function overloads a virtual function of the base class.
91  // It is invoked by the ProcessManager of the Particle.
92 
93 
94  G4LorentzVector GetEnegryMomentumConservation(){return EnMomConservation;}
95 
96  G4int GetNumberOfNeutronsInTarget(){return nOfNeutrons;}
97 
98 private:
99 
100  // Hide assignment operator as private
101  G4QIonIonElastic& operator=(const G4QIonIonElastic &right);
102 
103  // Copy constructor
105 
106  // BODY
107  // Static Parameters --------------------------------------------------------------------
108  static G4int nPartCWorld; // The#of particles for hadronization (limit of A of fragm.)
109  //--------------------------------- End of static parameters ---------------------------
110  // Working parameters
111  G4VQCrossSection* theCS;
112  G4LorentzVector EnMomConservation; // Residual of Energy/Momentum Cons.
113  G4int nOfNeutrons; // #of neutrons in the target nucleus
114 
115  // Modifires for the reaction
116  G4double Time; // Time shift of the capture reaction
117  G4double EnergyDeposition; // Energy deposited in the reaction
118  static std::vector <G4int> ElementZ; // Z of the element(i) in theLastCalc
119  static std::vector <G4double> ElProbInMat; // SumProbabilityElements in Material
120  static std::vector <std::vector<G4int>*> ElIsoN; // N of isotope(j) of Element(i)
121  static std::vector <std::vector<G4double>*> IsoProbInEl;// SumProbabIsotopes in Element i
122 };
123 #endif
124