source: trunk/source/processes/hadronic/models/neutron_hp/src/G4NeutronHPInelasticData.cc@ 893

Last change on this file since 893 was 819, checked in by garnier, 17 years ago

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25//
26// neutron_hp -- source file
27// J.P. Wellisch, Nov-1996
28// A prototype of the low energy neutron transport model.
29//
30// 070523 add neglecting doppler broadening on the fly. T. Koi
31// 070613 fix memory leaking by T. Koi
32// 071002 enable cross section dump by T. Koi
33//
34#include "G4NeutronHPInelasticData.hh"
35#include "G4Neutron.hh"
36#include "G4ElementTable.hh"
37#include "G4NeutronHPData.hh"
38
39G4bool G4NeutronHPInelasticData::IsApplicable(const G4DynamicParticle*aP, const G4Element*)
40{
41 G4bool result = true;
42 G4double eKin = aP->GetKineticEnergy();
43 if(eKin>20*MeV||aP->GetDefinition()!=G4Neutron::Neutron()) result = false;
44 return result;
45}
46
47G4NeutronHPInelasticData::G4NeutronHPInelasticData()
48{
49// TKDB
50 theCrossSections = 0;
51 BuildPhysicsTable(*G4Neutron::Neutron());
52}
53
54G4NeutronHPInelasticData::~G4NeutronHPInelasticData()
55{
56// TKDB
57 if ( theCrossSections != 0 )
58 { theCrossSections->clearAndDestroy(); }
59 delete theCrossSections;
60}
61
62void G4NeutronHPInelasticData::BuildPhysicsTable(const G4ParticleDefinition& aP)
63{
64 if(&aP!=G4Neutron::Neutron())
65 throw G4HadronicException(__FILE__, __LINE__, "Attempt to use NeutronHP data for particles other than neutrons!!!");
66 size_t numberOfElements = G4Element::GetNumberOfElements();
67// theCrossSections = new G4PhysicsTable( numberOfElements );
68// TKDB
69 if ( theCrossSections == 0 )
70 { theCrossSections = new G4PhysicsTable( numberOfElements ); }
71
72 // make a PhysicsVector for each element
73
74 static const G4ElementTable *theElementTable = G4Element::GetElementTable();
75 for( size_t i=0; i<numberOfElements; ++i )
76 {
77 G4PhysicsVector* physVec = G4NeutronHPData::
78 Instance()->MakePhysicsVector((*theElementTable)[i], this);
79 theCrossSections->push_back(physVec);
80 }
81}
82
83void G4NeutronHPInelasticData::DumpPhysicsTable(const G4ParticleDefinition& aP)
84{
85 if(&aP!=G4Neutron::Neutron())
86 throw G4HadronicException(__FILE__, __LINE__, "Attempt to use NeutronHP data for particles other than neutrons!!!");
87
88//
89// Dump element based cross section
90// range 10e-5 eV to 20 MeV
91// 10 point per decade
92// in barn
93//
94
95 G4cout << G4endl;
96 G4cout << G4endl;
97 G4cout << "Inelastic Cross Section of Neutron HP"<< G4endl;
98 G4cout << "(Pointwise cross-section at 0 Kelvin.)" << G4endl;
99 G4cout << G4endl;
100 G4cout << "Name of Element" << G4endl;
101 G4cout << "Energy[eV] XS[barn]" << G4endl;
102 G4cout << G4endl;
103
104 size_t numberOfElements = G4Element::GetNumberOfElements();
105 static const G4ElementTable *theElementTable = G4Element::GetElementTable();
106
107 for ( size_t i = 0 ; i < numberOfElements ; ++i )
108 {
109
110 G4cout << (*theElementTable)[i]->GetName() << G4endl;
111
112 G4int ie = 0;
113
114 for ( ie = 0 ; ie < 130 ; ie++ )
115 {
116 G4double eKinetic = 1.0e-5 * std::pow ( 10.0 , ie/10.0 ) *eV;
117 G4bool outOfRange = false;
118
119 if ( eKinetic < 20*MeV )
120 {
121 G4cout << eKinetic/eV << " " << (*((*theCrossSections)(i))).GetValue(eKinetic, outOfRange)/barn << G4endl;
122 }
123
124 }
125
126 G4cout << G4endl;
127 }
128
129 //G4cout << "G4NeutronHPInelasticData::DumpPhysicsTable still to be implemented"<<G4endl;
130}
131
132#include "G4NucleiPropertiesTable.hh"
133
134G4double G4NeutronHPInelasticData::
135GetCrossSection(const G4DynamicParticle* aP, const G4Element*anE, G4double aT)
136{
137 G4double result = 0;
138 G4bool outOfRange;
139 G4int index = anE->GetIndex();
140
141 // prepare neutron
142 G4double eKinetic = aP->GetKineticEnergy();
143
144 // T. K.
145 if ( getenv( "G4NEUTRONHP_NEGLECT_DOPPLER" ) )
146 {
147 G4double factor = 1.0;
148 if ( eKinetic < aT * k_Boltzmann )
149 {
150 // below 0.1 eV neutrons
151 // Have to do some, but now just igonre.
152 // Will take care after performance check.
153 // factor = factor * targetV;
154 }
155 return ( (*((*theCrossSections)(index))).GetValue(eKinetic, outOfRange) )* factor;
156 }
157
158 G4ReactionProduct theNeutron( aP->GetDefinition() );
159 theNeutron.SetMomentum( aP->GetMomentum() );
160 theNeutron.SetKineticEnergy( eKinetic );
161
162 // prepare thermal nucleus
163 G4Nucleus aNuc;
164 G4double eps = 0.0001;
165 G4double theA = anE->GetN();
166 G4double theZ = anE->GetZ();
167 G4double eleMass;
168 eleMass = ( G4NucleiPropertiesTable::GetNuclearMass(static_cast<G4int>(theZ+eps), static_cast<G4int>(theA+eps))
169 ) / G4Neutron::Neutron()->GetPDGMass();
170
171 G4ReactionProduct boosted;
172 G4double aXsection;
173
174 // MC integration loop
175 G4int counter = 0;
176 G4int failCount = 0;
177 G4double buffer = 0;
178 G4int size = G4int(std::max(10., aT/60*kelvin));
179 G4ThreeVector neutronVelocity = 1./G4Neutron::Neutron()->GetPDGMass()*theNeutron.GetMomentum();
180 G4double neutronVMag = neutronVelocity.mag();
181
182 while(counter == 0 || std::abs(buffer-result/std::max(1,counter)) > 0.01*buffer)
183 {
184 if(counter) buffer = result/counter;
185 while (counter<size)
186 {
187 counter ++;
188 G4ReactionProduct aThermalNuc = aNuc.GetThermalNucleus(eleMass, aT);
189 boosted.Lorentz(theNeutron, aThermalNuc);
190 G4double theEkin = boosted.GetKineticEnergy();
191 aXsection = (*((*theCrossSections)(index))).GetValue(theEkin, outOfRange);
192 if(aXsection <0)
193 {
194 if(failCount<1000)
195 {
196 failCount++;
197 counter--;
198 continue;
199 }
200 else
201 {
202 aXsection = 0;
203 }
204 }
205 // velocity correction.
206 G4ThreeVector targetVelocity = 1./aThermalNuc.GetMass()*aThermalNuc.GetMomentum();
207 aXsection *= (targetVelocity-neutronVelocity).mag()/neutronVMag;
208 result += aXsection;
209 }
210 size += size;
211 }
212 result /= counter;
213/*
214 // Checking impact of G4NEUTRONHP_NEGLECT_DOPPLER
215 G4cout << " result " << result << " "
216 << (*((*theCrossSections)(index))).GetValue(eKinetic, outOfRange) << " "
217 << (*((*theCrossSections)(index))).GetValue(eKinetic, outOfRange) /result << G4endl;
218*/
219 return result;
220}
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