source: trunk/source/physics_lists/lists/include/HadronPhysicsQGSC_CHIPS.hh @ 1315

Last change on this file since 1315 was 1315, checked in by garnier, 14 years ago

update geant4-09-04-beta-cand-01 interfaces-V09-03-09 vis-V09-03-08

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25//
26// $Id: HadronPhysicsQGSC_CHIPS.hh,v 1.7 2010/06/03 10:42:44 gunter Exp $
27// GEANT4 tag $Name: geant4-09-04-beta-cand-01 $
28//
29//---------------------------------------------------------------------------
30//
31// ClassName:   HadronPhysicsQGSC_CHIPS
32//
33// Author: 2009  M. Kosov
34//
35// Modified:
36//
37//----------------------------------------------------------------------------
38// Short description: In fact this is the definition of the Hadronic Inelastic
39// physics. The definition of the Hadronic Elastic physics one can find in the
40// G4HadronQElasticPhysics, which is stable (the same for all physics lists).
41// The only "unstable" part of the physics is the Hadronic Inelastic physics,
42// which is usually composed of the wixing of the High Energy Inelastic Model
43// (HEIM) and the Low Energy Inelastic Model (LEIM), which are applied only for
44// some hadrons (mostly nucleons and pi-mesons), above the LHEP model, which
45// usually covers all particles (but for Sigma_0 ?) and sometimes covers the
46// "hole" between the LEIM and HIME at intermediate energies. The name of the
47// Physics list is usually have a form HEIM_LEIM and the inelastic interactions
48// are defined in the HadronicPhysicsHEIM_LEIM class. So in this particular
49// physics list the low energy model is CHIPS (G4QCollision process) and the
50// high energy model is QGSC (QGS with the Energy Flow interface to CHIPS),
51// which are in terms of the energy boundary are mixed not on the model level,
52// but on the process level (G4DiscProcessMixer class). The LHEP is completely
53// excluded from this physics list, because the MiscLHEP is substituted by the
54// MiscQGSC class (QGS with the Energy Flow interface to CHIPS), covering all
55// particles, which are not N, pi, or K, defined by the separate builders.
56//---------------------------------------------------------------------------
57
58#ifndef HadronPhysicsQGSC_CHIPS_h
59#define HadronPhysicsQGSC_CHIPS_h 1
60
61#include "globals.hh"
62#include "G4ios.hh"
63
64#include "G4VPhysicsConstructor.hh"
65#include "G4MiscQGSCBuilder.hh"
66
67#include "G4PiKBuilder.hh"
68#include "G4QGSC_CHIPSPiKBuilder.hh"
69
70#include "G4QProtonBuilder.hh"
71#include "G4QGSC_CHIPSProtonBuilder.hh"
72
73#include "G4QNeutronBuilder.hh"
74#include "G4QGSC_CHIPSNeutronBuilder.hh"
75
76class HadronPhysicsQGSC_CHIPS : public G4VPhysicsConstructor
77{
78public: 
79  HadronPhysicsQGSC_CHIPS(G4int verbose =1);
80  HadronPhysicsQGSC_CHIPS(const G4String& name, G4bool quasiElastic=true);
81  virtual ~HadronPhysicsQGSC_CHIPS();
82
83public: 
84  virtual void ConstructParticle();
85  virtual void ConstructProcess();
86
87private:
88  void CreateModels();
89
90  G4QNeutronBuilder* theNeut;
91  G4QGSC_CHIPSNeutronBuilder* theQGSCNeut;
92   
93  G4PiKBuilder* thePiK;
94  G4QGSC_CHIPSPiKBuilder* theQGSCPiK;
95   
96  G4QProtonBuilder* theProt;
97  G4QGSC_CHIPSProtonBuilder * theQGSCProt;   
98   
99  G4MiscQGSCBuilder* theMiscQGSC;
100   
101  G4bool QuasiElastic;
102};
103
104#endif
105
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