G4HEAntiNeutronInelastic.hh

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00025 //
00026 // $Id$
00027 //
00028 //
00029 // G4 Gheisha High Energy model class -- header file
00030 // H. Fesefeldt, RWTH Aachen 23-October-1996
00031 // A prototype of the Gheisha High Energy collision model.
00032 
00033 #ifndef G4HEAntiNeutronInelastic_h
00034 #define G4HEAntiNeutronInelastic_h 1
00035 
00036 // Class description:
00037 // High energy parameterized model for anti-neutron inelastic scattering.  This
00038 // class is responsible for producing the final state of the interaction and
00039 // is typically valid for incident anti-neutron energies above 20 GeV.  This
00040 // physics may be invoked by registering an instance of the class with
00041 // G4AntiNeutronInelasticProcess in the user's physics list.
00042 //
00043 // This class is derived from G4HEInelastic which in turn is derived from
00044 // G4HadronicInteraction.
00045 
00046 // Class Description - End
00047 
00048 #include "G4HEInelastic.hh"
00049 
00050 class G4HEAntiNeutronInelastic : public G4HEInelastic  
00051 {
00052   public:  // with description 
00053     G4HEAntiNeutronInelastic(const G4String& name = "G4HEAntiNeutronInelastic");
00054     ~G4HEAntiNeutronInelastic(){};
00055 
00056     virtual void ModelDescription(std::ostream&) const;
00057         
00058     G4int vecLength;
00059         
00060     G4HadFinalState* ApplyYourself(const G4HadProjectile &aTrack,
00061                                    G4Nucleus &targetNucleus);
00062 
00063     G4int GetNumberOfSecondaries() {return vecLength;}         
00064 
00065     void FirstIntInCasAntiNeutron(G4bool &inElastic,
00066                                   const G4double availableEnergy,
00067                                   G4HEVector pv[],
00068                                   G4int &vecLen, 
00069                                   const G4HEVector& incidentParticle,
00070                                   const G4HEVector& targetParticle,
00071                                   const G4double atomicWeight);
00072 };
00073 #endif

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