source: trunk/source/processes/hadronic/models/high_energy/include/G4HEOmegaMinusInelastic.hh @ 1340

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27// $Id: G4HEOmegaMinusInelastic.hh,v 1.14 2007/04/11 18:11:30 dennis Exp $
28// GEANT4 tag $Name: geant4-09-03-ref-09 $
29//
30//
31// G4 Gheisha High Energy model class -- header file
32// H. Fesefeldt, RWTH Aachen 23-October-1996
33// Last modified: 10-December-1996
34
35// A prototype of the Gheisha High Energy collision model.
36
37#ifndef G4HEOmegaMinusInelastic_h
38#define G4HEOmegaMinusInelastic_h 1
39
40// Class description:
41// High energy parameterized model for Omega- inelastic scattering.  This
42// class is responsible for producing the final state of the interaction and
43// is typically valid for incident Omega- energies above 20 GeV.  This
44// physics may be invoked by registering an instance of the class with
45// G4OmegaMinusInelasticProcess in the user's physics list.
46//
47// This class is derived from G4HEInelastic which in turn is derived from
48// G4HadronicInteraction.
49
50// Class Description - End
51
52#include "G4HEInelastic.hh"
53
54class G4HEOmegaMinusInelastic : public G4HEInelastic 
55{
56 public:  // with description
57   G4HEOmegaMinusInelastic() : G4HEInelastic("G4HEOmegaMinusInelastic")
58   {
59     theMinEnergy =  20*GeV;
60     theMaxEnergy = 10*TeV;
61     MAXPART      = 2048;
62     verboseLevel = 0; 
63   }
64
65   ~G4HEOmegaMinusInelastic(){ };
66         
67   G4int vecLength;
68       
69   G4HadFinalState* ApplyYourself(const G4HadProjectile &aTrack, G4Nucleus &targetNucleus);
70
71   G4int GetNumberOfSecondaries()
72        { return vecLength; }         
73
74   void FirstIntInCasOmegaMinus(G4bool &inElastic, const G4double availableEnergy,
75                                G4HEVector pv[],
76                                G4int &vecLen, 
77                                G4HEVector incidentParticle,
78                                G4HEVector targetParticle,
79                                const G4double atomicWeight);
80};
81#endif                     
82                                         
83
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