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HadronPhysicsQGSC_CHIPS.cc
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25 //
26 // $Id$
27 //
28 //---------------------------------------------------------------------------
29 //
30 // ClassName: HadronPhysicsQGSC_CHIPS
31 //
32 // Author: 2009 M. Kosov
33 //
34 // Modified:
35 //
36 //----------------------------------------------------------------------------
37 // Short description: In fact this is the definition of the Hadronic Inelastic
38 // physics. The definition of the Hadronic Elastic physics one can find in the
39 // G4HadronQElasticPhysics, which is stable (the same for all physics lists).
40 // The only "unstable" part of the physics is the Hadronic Inelastic physics,
41 // which is usually composed of the wixing of the High Energy Inelastic Model
42 // (HEIM) and the Low Energy Inelastic Model (LEIM), which are applied only for
43 // some hadrons (mostly nucleons and pi-mesons), above the LHEP model, which
44 // usually covers all particles (but for Sigma_0 ?) and sometimes covers the
45 // "hole" between the LEIM and HIME at intermediate energies. The name of the
46 // Physics list is usually have a form HEIM_LEIM and the inelastic interactions
47 // are defined in the HadronicPhysicsHEIM_LEIM class. So in this particular
48 // physics list the low energy model is CHIPS (G4QCollision process) and the
49 // high energy model is QGSC (QGS with the Energy Flow interface to CHIPS),
50 // which are in terms of the energy boundary are mixed not on the model level,
51 // but on the process level (G4DiscProcessMixer class). The LHEP is completely
52 // excluded from this physics list, because the MiscLHEP is substituted by the
53 // MiscQGSC class (QGS with the Energy Flow interface to CHIPS), covering all
54 // particles, which are not N, pi, or K, defined by the separate builders.
55 //---------------------------------------------------------------------------
56 #include <iomanip>
57 
59 
60 #include "globals.hh"
61 #include "G4ios.hh"
62 #include "G4SystemOfUnits.hh"
63 #include "G4ParticleDefinition.hh"
64 #include "G4ParticleTable.hh"
65 
66 #include "G4MesonConstructor.hh"
67 #include "G4BaryonConstructor.hh"
69 
71  : G4VPhysicsConstructor("hInelastic QGSC_CHIPS")
72  , theNeut(0)
73  , theQGSCNeut(0)
74  , thePiK(0)
75  , theQGSCPiK(0)
76  , theProt(0)
77  , theQGSCProt(0)
78  , theMiscQGSC(0)
79  , QuasiElastic(true)
80 {}
81 
83  : G4VPhysicsConstructor(name)
84  , theNeut(0)
85  , theQGSCNeut(0)
86  , thePiK(0)
87  , theQGSCPiK(0)
88  , theProt(0)
89  , theQGSCProt(0)
90  , theMiscQGSC(0)
91  , QuasiElastic(quasiElastic)
92 {}
93 
94 void HadronPhysicsQGSC_CHIPS::CreateModels()
95 {
96  theNeut = new G4QNeutronBuilder;
97  theNeut->RegisterMe(theQGSCNeut=new G4QGSC_CHIPSNeutronBuilder(QuasiElastic));
98  //theQGSCNeut = new G4QGSC_CHIPSNeutronBuilder(QuasiElastic));
99 
100  theQGSCNeut->SetMinEnergy(0.0*GeV);
101 
102  theProt = new G4QProtonBuilder;
103  theProt->RegisterMe(theQGSCProt = new G4QGSC_CHIPSProtonBuilder(QuasiElastic));
104  //theQGSCProt = new G4QGSC_CHIPSProtonBuilder(QuasiElastic);
105 
106  theQGSCProt->SetMinEnergy(0.0*GeV);
107 
108  thePiK = new G4PiKBuilder;
109  thePiK->RegisterMe(theQGSCPiK=new G4QGSC_CHIPSPiKBuilder(QuasiElastic));
110 
111  theQGSCPiK->SetMinEnergy(0.0*GeV);
112 
113  theMiscQGSC=new G4MiscQGSCBuilder(0); // No verbose (@@ to be developed)
114 }
115 
117 {
118  delete theQGSCNeut;
119  delete theNeut;
120 
121  delete theQGSCProt;
122  delete theProt;
123 
124  delete theQGSCPiK;
125  delete thePiK;
126 
127  delete theMiscQGSC;
128 }
129 
131 {
132  G4MesonConstructor pMesonConstructor;
133  pMesonConstructor.ConstructParticle();
134 
135  G4BaryonConstructor pBaryonConstructor;
136  pBaryonConstructor.ConstructParticle();
137 
138  G4ShortLivedConstructor pShortLivedConstructor;
139  pShortLivedConstructor.ConstructParticle();
140 }
141 
142 #include "G4ProcessManager.hh"
144 {
145  CreateModels();
146  theNeut->Build();
147  theProt->Build();
148  thePiK->Build();
149  theMiscQGSC->Build();
150 }
151