source: trunk/source/processes/hadronic/models/neutron_hp/src/G4NeutronHPorLFission.cc@ 1036

Last change on this file since 1036 was 819, checked in by garnier, 17 years ago

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1//
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18// * This code implementation is the result of the scientific and *
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24// ********************************************************************
25//
26//
27// 05-11-21 NeutronHP or Low Energy Parameterization Models
28// Implemented by T. Koi (SLAC/SCCS)
29// If NeutronHP data do not available for an element, then Low Energy
30// Parameterization models handle the interactions of the element.
31// 080319 Compilation warnings - gcc-4.3.0 fix by T. Koi
32//
33
34// neutron_hp -- source file
35// J.P. Wellisch, Nov-1996
36// A prototype of the low energy neutron transport model.
37//
38#include "G4NeutronHPorLFission.hh"
39#include "G4NeutronHPFissionFS.hh"
40
41G4NeutronHPorLFission::G4NeutronHPorLFission()
42 :G4HadronicInteraction("NeutronHPorLFission")
43{
44 SetMinEnergy(0.*eV);
45 SetMaxEnergy(20.*MeV);
46
47 if( !getenv("G4NEUTRONHPDATA") )
48 throw G4HadronicException(__FILE__, __LINE__, "Please setenv G4NEUTRONHPDATA to point to the neutron cross-section files.");
49
50 dirName = getenv("G4NEUTRONHPDATA");
51 G4String tString = "/Fission/";
52 dirName = dirName + tString;
53// G4cout <<"G4NeutronHPorLFission::G4NeutronHPorLFission testit "<<dirName<<G4endl;
54 unavailable_elements.clear();
55
56 numEle = G4Element::GetNumberOfElements();
57 theFission = new G4NeutronHPChannel[numEle];
58
59 for ( G4int i = 0; i < numEle ; i++)
60 {
61 if ( (*(G4Element::GetElementTable()))[i]-> GetZ() > 89 )
62 {
63 theFission[i].Init((*(G4Element::GetElementTable()))[i], dirName);
64 try { while(!theFission[i].Register(&theFS)) ; }
65 catch ( G4HadronicException )
66 {
67 unavailable_elements.insert ( (*(G4Element::GetElementTable()))[i]->GetName() );
68 }
69 }
70 }
71
72 if ( unavailable_elements.size() > 0 )
73 {
74 std::set< G4String>::iterator it;
75 G4cout << "HP Fission data are not available for thess elements "<< G4endl;
76 for ( it = unavailable_elements.begin() ; it != unavailable_elements.end() ; it++ )
77 {
78 G4cout << *it << G4endl;
79 }
80 G4cout << "Low Energy Parameterization Models will be used."<< G4endl;
81 }
82
83 createXSectionDataSet();
84}
85
86G4NeutronHPorLFission::~G4NeutronHPorLFission()
87{
88 delete [] theFission;
89 delete theDataSet;
90}
91
92#include "G4NeutronHPThermalBoost.hh"
93
94G4HadFinalState * G4NeutronHPorLFission::ApplyYourself(const G4HadProjectile& aTrack, G4Nucleus& )
95{
96 const G4Material * theMaterial = aTrack.GetMaterial();
97 G4int n = theMaterial->GetNumberOfElements();
98 G4int index = theMaterial->GetElement(0)->GetIndex();
99 if(n!=1)
100 {
101 G4int i;
102 xSec = new G4double[n];
103 G4double sum=0;
104 const G4double * NumAtomsPerVolume = theMaterial->GetVecNbOfAtomsPerVolume();
105 G4double rWeight;
106 G4NeutronHPThermalBoost aThermalE;
107 for (i=0; i<n; i++)
108 {
109 index = theMaterial->GetElement(i)->GetIndex();
110 rWeight = NumAtomsPerVolume[i];
111 G4double x = aThermalE.GetThermalEnergy(aTrack, theMaterial->GetElement(i), theMaterial->GetTemperature());
112
113 //xSec[i] = theFission[index].GetXsec(aThermalE.GetThermalEnergy(aTrack,
114 // theMaterial->GetElement(i),
115 // theMaterial->GetTemperature()));
116 xSec[i] = theFission[index].GetXsec(x);
117
118 xSec[i] *= rWeight;
119 sum+=xSec[i];
120 }
121 G4double random = G4UniformRand();
122 G4double running = 0;
123 for (i=0; i<n; i++)
124 {
125 running += xSec[i];
126 index = theMaterial->GetElement(i)->GetIndex();
127 if(random<=running/sum) break;
128 }
129 delete [] xSec;
130 // it is element-wise initialised.
131 }
132 return theFission[index].ApplyYourself(aTrack);
133}
134
135
136
137G4bool G4NeutronHPorLFission::IsThisElementOK( G4String name )
138{
139 if ( unavailable_elements.find( name ) == unavailable_elements.end() )
140 return TRUE;
141 else
142 return FALSE;
143}
144
145
146
147void G4NeutronHPorLFission::createXSectionDataSet()
148{
149 theDataSet = new G4NeutronHPorLFissionData ( theFission , &unavailable_elements );
150}
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