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26 // 26 //
27 // Geant4 class G4HadronicBuilder 27 // Geant4 class G4HadronicBuilder
28 // 28 //
29 // Author V.Ivanchenko 14.05.2020 29 // Author V.Ivanchenko 14.05.2020
30 // 30 //
31 31
32 #include "G4HadronicBuilder.hh" 32 #include "G4HadronicBuilder.hh"
33 #include "G4HadParticles.hh" 33 #include "G4HadParticles.hh"
34 #include "G4HadProcesses.hh" 34 #include "G4HadProcesses.hh"
35 35
36 #include "G4ParticleDefinition.hh" 36 #include "G4ParticleDefinition.hh"
37 #include "G4ParticleTable.hh" 37 #include "G4ParticleTable.hh"
38 #include "G4PhysicsListHelper.hh" 38 #include "G4PhysicsListHelper.hh"
39 #include "G4SystemOfUnits.hh" <<
40 39
41 #include "G4HadronicParameters.hh" 40 #include "G4HadronicParameters.hh"
42 41
43 #include "G4TheoFSGenerator.hh" 42 #include "G4TheoFSGenerator.hh"
44 #include "G4FTFModel.hh" 43 #include "G4FTFModel.hh"
45 #include "G4ExcitedStringDecay.hh" 44 #include "G4ExcitedStringDecay.hh"
46 #include "G4GeneratorPrecompoundInterface.hh" 45 #include "G4GeneratorPrecompoundInterface.hh"
47 46
48 #include "G4QGSModel.hh" 47 #include "G4QGSModel.hh"
49 #include "G4QGSParticipants.hh" 48 #include "G4QGSParticipants.hh"
50 #include "G4QGSMFragmentation.hh" 49 #include "G4QGSMFragmentation.hh"
51 #include "G4QuasiElasticChannel.hh" 50 #include "G4QuasiElasticChannel.hh"
52 51
53 #include "G4CascadeInterface.hh" 52 #include "G4CascadeInterface.hh"
54 #include "G4CrossSectionDataSetRegistry.hh" 53 #include "G4CrossSectionDataSetRegistry.hh"
55 #include "G4CrossSectionInelastic.hh" 54 #include "G4CrossSectionInelastic.hh"
56 #include "G4CrossSectionElastic.hh" 55 #include "G4CrossSectionElastic.hh"
57 #include "G4HadronElastic.hh" 56 #include "G4HadronElastic.hh"
58 #include "G4CrossSectionDataSetRegistry.hh" 57 #include "G4CrossSectionDataSetRegistry.hh"
59 58
60 #include "G4HadronElasticProcess.hh" 59 #include "G4HadronElasticProcess.hh"
61 #include "G4HadronInelasticProcess.hh" 60 #include "G4HadronInelasticProcess.hh"
62 61
63 #include "G4DecayTable.hh" 62 #include "G4DecayTable.hh"
64 #include "G4VDecayChannel.hh" 63 #include "G4VDecayChannel.hh"
65 #include "G4PhaseSpaceDecayChannel.hh" 64 #include "G4PhaseSpaceDecayChannel.hh"
66 65
67 #include "G4PreCompoundModel.hh" <<
68 #include "G4INCLXXInterface.hh" <<
69 #include "G4ComponentAntiNuclNuclearXS.hh" <<
70 <<
71 <<
72 <<
73 void G4HadronicBuilder::BuildFTFP_BERT(const s 66 void G4HadronicBuilder::BuildFTFP_BERT(const std::vector<G4int>& partList,
74 G4bool 67 G4bool bert, const G4String& xsName) {
75 68
76 G4HadronicParameters* param = G4HadronicPara 69 G4HadronicParameters* param = G4HadronicParameters::Instance();
77 G4PhysicsListHelper* ph = G4PhysicsListHelpe 70 G4PhysicsListHelper* ph = G4PhysicsListHelper::GetPhysicsListHelper();
78 71
79 auto theModel = new G4TheoFSGenerator("FTFP" 72 auto theModel = new G4TheoFSGenerator("FTFP");
80 auto theStringModel = new G4FTFModel(); 73 auto theStringModel = new G4FTFModel();
81 theStringModel->SetFragmentationModel(new G4 74 theStringModel->SetFragmentationModel(new G4ExcitedStringDecay());
82 theModel->SetHighEnergyGenerator( theStringM 75 theModel->SetHighEnergyGenerator( theStringModel );
83 theModel->SetTransport( new G4GeneratorPreco 76 theModel->SetTransport( new G4GeneratorPrecompoundInterface() );
84 theModel->SetMaxEnergy( param->GetMaxEnergy( 77 theModel->SetMaxEnergy( param->GetMaxEnergy() );
85 78
86 G4CascadeInterface* theCascade = nullptr; 79 G4CascadeInterface* theCascade = nullptr;
87 if(bert) { 80 if(bert) {
88 theCascade = new G4CascadeInterface(); 81 theCascade = new G4CascadeInterface();
89 theCascade->SetMaxEnergy( param->GetMaxEne 82 theCascade->SetMaxEnergy( param->GetMaxEnergyTransitionFTF_Cascade() );
90 theModel->SetMinEnergy( param->GetMinEnerg 83 theModel->SetMinEnergy( param->GetMinEnergyTransitionFTF_Cascade() );
91 } 84 }
92 85
93 auto xsinel = G4HadProcesses::InelasticXS( x 86 auto xsinel = G4HadProcesses::InelasticXS( xsName );
94 87
95 G4ParticleTable* table = G4ParticleTable::Ge 88 G4ParticleTable* table = G4ParticleTable::GetParticleTable();
96 for( auto & pdg : partList ) { 89 for( auto & pdg : partList ) {
97 90
98 auto part = table->FindParticle( pdg ); 91 auto part = table->FindParticle( pdg );
99 if ( part == nullptr ) { continue; } 92 if ( part == nullptr ) { continue; }
100 93
101 auto hadi = new G4HadronInelasticProcess( 94 auto hadi = new G4HadronInelasticProcess( part->GetParticleName()+"Inelastic", part );
102 hadi->AddDataSet( xsinel ); 95 hadi->AddDataSet( xsinel );
103 hadi->RegisterMe( theModel ); 96 hadi->RegisterMe( theModel );
104 if( theCascade != nullptr ) hadi->Register 97 if( theCascade != nullptr ) hadi->RegisterMe( theCascade );
105 if( param->ApplyFactorXS() ) hadi->Multipl 98 if( param->ApplyFactorXS() ) hadi->MultiplyCrossSectionBy( param->XSFactorHadronInelastic() );
106 ph->RegisterProcess(hadi, part); 99 ph->RegisterProcess(hadi, part);
107 } 100 }
108 } 101 }
109 102
110 void G4HadronicBuilder::BuildFTFQGSP_BERT(cons 103 void G4HadronicBuilder::BuildFTFQGSP_BERT(const std::vector<G4int>& partList,
111 G4bo 104 G4bool bert, const G4String& xsName) {
112 105
113 G4HadronicParameters* param = G4HadronicPara 106 G4HadronicParameters* param = G4HadronicParameters::Instance();
114 G4PhysicsListHelper* ph = G4PhysicsListHelpe 107 G4PhysicsListHelper* ph = G4PhysicsListHelper::GetPhysicsListHelper();
115 108
116 auto theModel = new G4TheoFSGenerator("FTFQG 109 auto theModel = new G4TheoFSGenerator("FTFQGSP");
117 auto theStringModel = new G4FTFModel(); 110 auto theStringModel = new G4FTFModel();
118 theStringModel->SetFragmentationModel(new G4 111 theStringModel->SetFragmentationModel(new G4ExcitedStringDecay( new G4QGSMFragmentation() ) );
119 theModel->SetHighEnergyGenerator( theStringM 112 theModel->SetHighEnergyGenerator( theStringModel );
120 theModel->SetTransport( new G4GeneratorPreco 113 theModel->SetTransport( new G4GeneratorPrecompoundInterface() );
121 theModel->SetMaxEnergy( param->GetMaxEnergy( 114 theModel->SetMaxEnergy( param->GetMaxEnergy() );
122 115
123 G4CascadeInterface* theCascade = nullptr; 116 G4CascadeInterface* theCascade = nullptr;
124 if(bert) { 117 if(bert) {
125 theCascade = new G4CascadeInterface(); 118 theCascade = new G4CascadeInterface();
126 theCascade->SetMaxEnergy( param->GetMaxEne 119 theCascade->SetMaxEnergy( param->GetMaxEnergyTransitionFTF_Cascade() );
127 theModel->SetMinEnergy( param->GetMinEnerg 120 theModel->SetMinEnergy( param->GetMinEnergyTransitionFTF_Cascade() );
128 } 121 }
129 122
130 auto xsinel = G4HadProcesses::InelasticXS( x 123 auto xsinel = G4HadProcesses::InelasticXS( xsName );
131 124
132 G4ParticleTable* table = G4ParticleTable::Ge 125 G4ParticleTable* table = G4ParticleTable::GetParticleTable();
133 for( auto & pdg : partList ) { 126 for( auto & pdg : partList ) {
134 127
135 auto part = table->FindParticle( pdg ); 128 auto part = table->FindParticle( pdg );
136 if ( part == nullptr ) { continue; } 129 if ( part == nullptr ) { continue; }
137 130
138 auto hadi = new G4HadronInelasticProcess( 131 auto hadi = new G4HadronInelasticProcess( part->GetParticleName()+"Inelastic", part );
139 hadi->AddDataSet( xsinel ); 132 hadi->AddDataSet( xsinel );
140 hadi->RegisterMe( theModel ); 133 hadi->RegisterMe( theModel );
141 if( theCascade != nullptr ) hadi->Register 134 if( theCascade != nullptr ) hadi->RegisterMe( theCascade );
142 if( param->ApplyFactorXS() ) hadi->Multipl 135 if( param->ApplyFactorXS() ) hadi->MultiplyCrossSectionBy( param->XSFactorHadronInelastic() );
143 ph->RegisterProcess(hadi, part); 136 ph->RegisterProcess(hadi, part);
144 } 137 }
145 } 138 }
146 139
147 void G4HadronicBuilder::BuildQGSP_FTFP_BERT(co 140 void G4HadronicBuilder::BuildQGSP_FTFP_BERT(const std::vector<G4int>& partList,
148 G4 141 G4bool bert, G4bool quasiElastic,
149 co 142 const G4String& xsName) {
150 143
151 G4HadronicParameters* param = G4HadronicPara 144 G4HadronicParameters* param = G4HadronicParameters::Instance();
152 G4PhysicsListHelper* ph = G4PhysicsListHelpe 145 G4PhysicsListHelper* ph = G4PhysicsListHelper::GetPhysicsListHelper();
153 146
154 auto theTransport = new G4GeneratorPrecompou 147 auto theTransport = new G4GeneratorPrecompoundInterface();
155 148
156 auto theHEModel = new G4TheoFSGenerator("QGS 149 auto theHEModel = new G4TheoFSGenerator("QGSP");
157 G4QGSModel< G4QGSParticipants >* theQGSModel 150 G4QGSModel< G4QGSParticipants >* theQGSModel = new G4QGSModel< G4QGSParticipants >;
158 theQGSModel->SetFragmentationModel( new G4Ex 151 theQGSModel->SetFragmentationModel( new G4ExcitedStringDecay( new G4QGSMFragmentation() ) );
159 theHEModel->SetTransport( theTransport ); 152 theHEModel->SetTransport( theTransport );
160 theHEModel->SetHighEnergyGenerator( theQGSMo 153 theHEModel->SetHighEnergyGenerator( theQGSModel );
161 if (quasiElastic) { 154 if (quasiElastic) {
162 theHEModel->SetQuasiElasticChannel(new G4Q 155 theHEModel->SetQuasiElasticChannel(new G4QuasiElasticChannel());
163 } 156 }
164 theHEModel->SetMinEnergy( param->GetMinEnerg 157 theHEModel->SetMinEnergy( param->GetMinEnergyTransitionQGS_FTF() );
165 theHEModel->SetMaxEnergy( param->GetMaxEnerg 158 theHEModel->SetMaxEnergy( param->GetMaxEnergy() );
166 159
167 auto theLEModel = new G4TheoFSGenerator("FTF 160 auto theLEModel = new G4TheoFSGenerator("FTFP");
168 auto theFTFModel = new G4FTFModel(); 161 auto theFTFModel = new G4FTFModel();
169 theFTFModel->SetFragmentationModel(new G4Exc 162 theFTFModel->SetFragmentationModel(new G4ExcitedStringDecay());
170 theLEModel->SetHighEnergyGenerator( theFTFMo 163 theLEModel->SetHighEnergyGenerator( theFTFModel );
171 theLEModel->SetTransport( theTransport ); 164 theLEModel->SetTransport( theTransport );
172 theLEModel->SetMaxEnergy( param->GetMaxEnerg 165 theLEModel->SetMaxEnergy( param->GetMaxEnergyTransitionQGS_FTF() );
173 166
174 G4CascadeInterface* theCascade = nullptr; 167 G4CascadeInterface* theCascade = nullptr;
175 if(bert) { 168 if(bert) {
176 theCascade = new G4CascadeInterface(); 169 theCascade = new G4CascadeInterface();
177 theCascade->SetMaxEnergy( param->GetMaxEne 170 theCascade->SetMaxEnergy( param->GetMaxEnergyTransitionFTF_Cascade() );
178 theLEModel->SetMinEnergy( param->GetMinEne 171 theLEModel->SetMinEnergy( param->GetMinEnergyTransitionFTF_Cascade() );
179 } 172 }
180 173
181 auto xsinel = G4HadProcesses::InelasticXS( x 174 auto xsinel = G4HadProcesses::InelasticXS( xsName );
182 175
183 G4ParticleTable* table = G4ParticleTable::Ge 176 G4ParticleTable* table = G4ParticleTable::GetParticleTable();
184 for( auto & pdg : partList ) { 177 for( auto & pdg : partList ) {
185 178
186 auto part = table->FindParticle( pdg ); 179 auto part = table->FindParticle( pdg );
187 if ( part == nullptr ) { continue; } 180 if ( part == nullptr ) { continue; }
188 181
189 auto hadi = new G4HadronInelasticProcess( 182 auto hadi = new G4HadronInelasticProcess( part->GetParticleName()+"Inelastic", part );
190 hadi->AddDataSet( xsinel ); 183 hadi->AddDataSet( xsinel );
191 hadi->RegisterMe( theHEModel ); 184 hadi->RegisterMe( theHEModel );
192 hadi->RegisterMe( theLEModel ); 185 hadi->RegisterMe( theLEModel );
193 if(theCascade != nullptr) hadi->RegisterMe 186 if(theCascade != nullptr) hadi->RegisterMe( theCascade );
194 if( param->ApplyFactorXS() ) hadi->Multipl 187 if( param->ApplyFactorXS() ) hadi->MultiplyCrossSectionBy( param->XSFactorHadronInelastic() );
195 ph->RegisterProcess(hadi, part); 188 ph->RegisterProcess(hadi, part);
196 } 189 }
197 } 190 }
198 191
199 void G4HadronicBuilder::BuildINCLXX(const std: <<
200 G4bool <<
201 <<
202 // FTF <<
203 G4HadronicParameters* param = G4HadronicPara <<
204 G4PhysicsListHelper* ph = G4PhysicsListHelpe <<
205 <<
206 auto theModel = new G4TheoFSGenerator("FTFP" <<
207 auto theStringModel = new G4FTFModel(); <<
208 theStringModel->SetFragmentationModel(new G4 <<
209 theModel->SetHighEnergyGenerator( theStringM <<
210 theModel->SetTransport( new G4GeneratorPreco <<
211 theModel->SetMaxEnergy( param->GetMaxEnergy( <<
212 <<
213 G4CascadeInterface* theCascade = nullptr; <<
214 if(bert) { <<
215 theCascade = new G4CascadeInterface(); <<
216 theCascade->SetMaxEnergy( param->GetMaxEne <<
217 theModel->SetMinEnergy( param->GetMinEnerg <<
218 } <<
219 <<
220 // INCLXX <<
221 auto theModelINCLXX = new G4INCLXXInterface( <<
222 theModelINCLXX->SetMinEnergy( param->GetMinE <<
223 theModelINCLXX->SetMaxEnergy( param->GetMaxE <<
224 <<
225 // <<
226 auto xsinel = G4HadProcesses::InelasticXS( x <<
227 <<
228 G4ParticleTable* table = G4ParticleTable::Ge <<
229 for( auto & pdg : partList ) { <<
230 <<
231 auto part = table->FindParticle( pdg ); <<
232 if ( part == nullptr ) { continue; } <<
233 <<
234 auto hadi = new G4HadronInelasticProcess( <<
235 if( pdg == -2212 ) { // pbar use INCLXX <<
236 hadi->AddDataSet( xsinel ); <<
237 hadi->RegisterMe( theModelINCLXX ); <<
238 if( param->ApplyFactorXS() ) hadi->Multi <<
239 ph->RegisterProcess(hadi, part); <<
240 } else { // other anti-X use FTF <<
241 hadi->AddDataSet( xsinel ); <<
242 hadi->RegisterMe( theModel ); <<
243 if( theCascade != nullptr ) hadi->Register <<
244 if( param->ApplyFactorXS() ) hadi->Multipl <<
245 ph->RegisterProcess(hadi, part); <<
246 } <<
247 } <<
248 } <<
249 <<
250 void G4HadronicBuilder::BuildElastic(const std 192 void G4HadronicBuilder::BuildElastic(const std::vector<G4int>& partList) {
251 193
252 G4HadronicParameters* param = G4HadronicPara 194 G4HadronicParameters* param = G4HadronicParameters::Instance();
253 G4PhysicsListHelper* ph = G4PhysicsListHelpe 195 G4PhysicsListHelper* ph = G4PhysicsListHelper::GetPhysicsListHelper();
254 196
255 auto xsel = G4HadProcesses::ElasticXS("Glaub 197 auto xsel = G4HadProcesses::ElasticXS("Glauber-Gribov");
256 198
257 auto elModel = new G4HadronElastic(); 199 auto elModel = new G4HadronElastic();
258 elModel->SetMaxEnergy( param->GetMaxEnergy() 200 elModel->SetMaxEnergy( param->GetMaxEnergy() );
259 201
260 G4ParticleTable* table = G4ParticleTable::Ge 202 G4ParticleTable* table = G4ParticleTable::GetParticleTable();
261 for( auto & pdg : partList ) { 203 for( auto & pdg : partList ) {
262 204
263 auto part = table->FindParticle( pdg ); 205 auto part = table->FindParticle( pdg );
264 if ( part == nullptr ) { continue; } 206 if ( part == nullptr ) { continue; }
265 207
266 auto hade = new G4HadronElasticProcess(); 208 auto hade = new G4HadronElasticProcess();
267 hade->AddDataSet( xsel ); 209 hade->AddDataSet( xsel );
268 hade->RegisterMe( elModel ); 210 hade->RegisterMe( elModel );
269 if( param->ApplyFactorXS() ) hade->Multipl 211 if( param->ApplyFactorXS() ) hade->MultiplyCrossSectionBy( param->XSFactorHadronElastic() );
270 ph->RegisterProcess(hade, part); 212 ph->RegisterProcess(hade, part);
271 } 213 }
272 } 214 }
273 215
274 void G4HadronicBuilder::BuildHyperonsFTFP_BERT 216 void G4HadronicBuilder::BuildHyperonsFTFP_BERT() {
275 // For hyperons, Bertini is used at low ener 217 // For hyperons, Bertini is used at low energies;
276 // for anti-hyperons, FTFP can be used down 218 // for anti-hyperons, FTFP can be used down to zero kinetic energy.
277 BuildFTFP_BERT(G4HadParticles::GetHyperons() 219 BuildFTFP_BERT(G4HadParticles::GetHyperons(), true, "Glauber-Gribov");
278 BuildFTFP_BERT(G4HadParticles::GetAntiHypero 220 BuildFTFP_BERT(G4HadParticles::GetAntiHyperons(), false, "Glauber-Gribov");
279 } 221 }
280 222
281 void G4HadronicBuilder::BuildHyperonsFTFQGSP_B 223 void G4HadronicBuilder::BuildHyperonsFTFQGSP_BERT() {
282 // For hyperons, Bertini is used at low ener 224 // For hyperons, Bertini is used at low energies;
283 // for anti-hyperons, FTFP can be used down 225 // for anti-hyperons, FTFP can be used down to zero kinetic energy.
284 BuildFTFQGSP_BERT(G4HadParticles::GetHyperon 226 BuildFTFQGSP_BERT(G4HadParticles::GetHyperons(), true, "Glauber-Gribov");
285 BuildFTFQGSP_BERT(G4HadParticles::GetAntiHyp 227 BuildFTFQGSP_BERT(G4HadParticles::GetAntiHyperons(), false, "Glauber-Gribov");
286 } 228 }
287 229
288 void G4HadronicBuilder::BuildHyperonsQGSP_FTFP 230 void G4HadronicBuilder::BuildHyperonsQGSP_FTFP_BERT(G4bool qElastic) {
289 // For hyperons, Bertini is used at low ener 231 // For hyperons, Bertini is used at low energies;
290 // for anti-hyperons, FTFP can be used down 232 // for anti-hyperons, FTFP can be used down to zero kinetic energy.
291 // QGSP is used at high energies in all case 233 // QGSP is used at high energies in all cases.
292 BuildQGSP_FTFP_BERT(G4HadParticles::GetHyper 234 BuildQGSP_FTFP_BERT(G4HadParticles::GetHyperons(), true, qElastic, "Glauber-Gribov");
293 BuildQGSP_FTFP_BERT(G4HadParticles::GetAntiH 235 BuildQGSP_FTFP_BERT(G4HadParticles::GetAntiHyperons(), false, qElastic, "Glauber-Gribov");
294 } 236 }
295 237
296 void G4HadronicBuilder::BuildKaonsFTFP_BERT() 238 void G4HadronicBuilder::BuildKaonsFTFP_BERT() {
297 BuildFTFP_BERT(G4HadParticles::GetKaons(), t 239 BuildFTFP_BERT(G4HadParticles::GetKaons(), true, "Glauber-Gribov");
298 } 240 }
299 241
300 void G4HadronicBuilder::BuildKaonsFTFQGSP_BERT 242 void G4HadronicBuilder::BuildKaonsFTFQGSP_BERT() {
301 BuildFTFQGSP_BERT(G4HadParticles::GetKaons() << 243 BuildFTFP_BERT(G4HadParticles::GetKaons(), true, "Glauber-Gribov");
302 } 244 }
303 245
304 void G4HadronicBuilder::BuildKaonsQGSP_FTFP_BE 246 void G4HadronicBuilder::BuildKaonsQGSP_FTFP_BERT(G4bool qElastic) {
305 BuildQGSP_FTFP_BERT(G4HadParticles::GetKaons 247 BuildQGSP_FTFP_BERT(G4HadParticles::GetKaons(), true, qElastic, "Glauber-Gribov");
306 } 248 }
307 249
308 void G4HadronicBuilder::BuildAntiLightIonsFTFP 250 void G4HadronicBuilder::BuildAntiLightIonsFTFP() {
309 BuildFTFP_BERT(G4HadParticles::GetLightAntiI 251 BuildFTFP_BERT(G4HadParticles::GetLightAntiIons(), false, "AntiAGlauber");
310 } 252 }
311 253
312 //void G4HadronicBuilder::BuildAntiLightIonsQG 254 //void G4HadronicBuilder::BuildAntiLightIonsQGSP_FTFP(G4bool qElastic) {
313 // Note: currently QGSP cannot be applied for 255 // Note: currently QGSP cannot be applied for any ion or anti-ion!
314 // BuildQGSP_FTFP_BERT(G4HadParticles::GetLig 256 // BuildQGSP_FTFP_BERT(G4HadParticles::GetLightAntiIons(), false, qElastic, "AntiAGlauber");
315 //} 257 //}
316 258
317 void G4HadronicBuilder::BuildAntiLightIonsINCL <<
318 BuildINCLXX(G4HadParticles::GetLightAntiIons <<
319 } <<
320 <<
321 void G4HadronicBuilder::BuildBCHadronsFTFP_BER 259 void G4HadronicBuilder::BuildBCHadronsFTFP_BERT() {
322 if( G4HadronicParameters::Instance()->Enable 260 if( G4HadronicParameters::Instance()->EnableBCParticles() ) {
323 // Bertini is not applicable for charm and 261 // Bertini is not applicable for charm and bottom hadrons, therefore FTFP is used
324 // down to zero kinetic energy (but at ver 262 // down to zero kinetic energy (but at very low energies, a dummy model is used
325 // that returns the projectile heavy hadro 263 // that returns the projectile heavy hadron in the final state).
326 BuildFTFP_BERT(G4HadParticles::GetBCHadron 264 BuildFTFP_BERT(G4HadParticles::GetBCHadrons(), false, "Glauber-Gribov");
327 BuildDecayTableForBCHadrons(); 265 BuildDecayTableForBCHadrons();
328 } 266 }
329 } 267 }
330 268
331 void G4HadronicBuilder::BuildBCHadronsFTFQGSP_ 269 void G4HadronicBuilder::BuildBCHadronsFTFQGSP_BERT() {
332 if( G4HadronicParameters::Instance()->Enable 270 if( G4HadronicParameters::Instance()->EnableBCParticles() ) {
333 // Bertini is not applicable for charm and 271 // Bertini is not applicable for charm and bottom hadrons, therefore FTFP is used
334 // down to zero kinetic energy (but at ver 272 // down to zero kinetic energy (but at very low energies, a dummy model is used
335 // that returns the projectile heavy hadro 273 // that returns the projectile heavy hadron in the final state).
336 BuildFTFQGSP_BERT(G4HadParticles::GetBCHad 274 BuildFTFQGSP_BERT(G4HadParticles::GetBCHadrons(), false, "Glauber-Gribov");
337 BuildDecayTableForBCHadrons(); 275 BuildDecayTableForBCHadrons();
338 } 276 }
339 } 277 }
340 278
341 void G4HadronicBuilder::BuildBCHadronsQGSP_FTF 279 void G4HadronicBuilder::BuildBCHadronsQGSP_FTFP_BERT(G4bool qElastic) {
342 if( G4HadronicParameters::Instance()->Enable 280 if( G4HadronicParameters::Instance()->EnableBCParticles() ) {
343 // Bertini is not applicable for charm and 281 // Bertini is not applicable for charm and bottom hadrons, therefore FTFP is used
344 // down to zero kinetic energy (but at ver 282 // down to zero kinetic energy (but at very low energies, a dummy model is used
345 // that returns the projectile heavy hadro 283 // that returns the projectile heavy hadron in the final state).
346 // QGSP is used at high energies in all ca 284 // QGSP is used at high energies in all cases.
347 BuildQGSP_FTFP_BERT(G4HadParticles::GetBCH 285 BuildQGSP_FTFP_BERT(G4HadParticles::GetBCHadrons(), false, qElastic, "Glauber-Gribov");
348 BuildDecayTableForBCHadrons(); 286 BuildDecayTableForBCHadrons();
349 } 287 }
350 } 288 }
351 289
352 void G4HadronicBuilder::BuildDecayTableForBCHa 290 void G4HadronicBuilder::BuildDecayTableForBCHadrons() {
353 // Geant4 does not define the decay of most 291 // Geant4 does not define the decay of most of charmed and bottom hadrons.
354 // The reason is that most of these heavy ha 292 // The reason is that most of these heavy hadrons have many different
355 // decay channels, with a complex dynamics, 293 // decay channels, with a complex dynamics, quite different from the flat
356 // phase space kinematical treatment used in 294 // phase space kinematical treatment used in Geant4 for most of hadronic decays.
357 // High-energy experiments usually use dedic 295 // High-energy experiments usually use dedicated Monte Carlo Event Generators
358 // for the decays of charmed and bottom hadr 296 // for the decays of charmed and bottom hadrons; therefore, these heavy
359 // hadrons, which are passed to Geant4 as pr 297 // hadrons, which are passed to Geant4 as primary tracks, have pre-assigned
360 // decays. Moreover, no charmed or bottom se 298 // decays. Moreover, no charmed or bottom secondary hadrons were created
361 // in Geant4 hadronic interactions before Ge 299 // in Geant4 hadronic interactions before Geant4 10.7.
362 // With the extension of Geant4 hadronic int 300 // With the extension of Geant4 hadronic interactions to charmed and bottom
363 // hadrons, in version Geant4 10.7, we do ne 301 // hadrons, in version Geant4 10.7, we do need to define decays in Geant4
364 // for these heavy hadrons, for two reasons: 302 // for these heavy hadrons, for two reasons:
365 // 1. For testing purposes, unless we pre-as 303 // 1. For testing purposes, unless we pre-assign decays of heavy hadrons
366 // (as the HEP experiments normally do by 304 // (as the HEP experiments normally do by using MC Event Generators);
367 // 2. To avoid crashes (due to missing decay 305 // 2. To avoid crashes (due to missing decay channels) whenever charmed or
368 // bottom secondary hadrons are produced 306 // bottom secondary hadrons are produced by Geant4 hadronic interactions,
369 // even with ordinary (i.e. not heavy) ha 307 // even with ordinary (i.e. not heavy) hadron projectiles, because in
370 // this case we cannot (easily!) pre-assi 308 // this case we cannot (easily!) pre-assign decays to them.
371 // Given that 1. is just a convenience for t 309 // Given that 1. is just a convenience for testing, and 2. happens rather
372 // rarely in practice - because very few pri 310 // rarely in practice - because very few primary energetic (i.e. boosted)
373 // heavy hadrons fly enough to reach the bea 311 // heavy hadrons fly enough to reach the beam pipe or the tracker and
374 // having an inelastic interaction there, an 312 // having an inelastic interaction there, and the very low probability
375 // to create a heavy hadrons from the string 313 // to create a heavy hadrons from the string fragmentation in ordinary
376 // (i.e. not heavy) hadronic interactions - 314 // (i.e. not heavy) hadronic interactions - there is no need in practice
377 // to define accurately the decays of heavy 315 // to define accurately the decays of heavy hadrons in Geant4.
378 // So, for our practical purposes, it is eno 316 // So, for our practical purposes, it is enough to define very simple,
379 // "dummy" decays of charmed and bottom hadr 317 // "dummy" decays of charmed and bottom hadrons.
380 // Here we use a single, fully hadronic chan 318 // Here we use a single, fully hadronic channel, with 2 or 3 or 4
381 // daughters, for each of these heavy hadron 319 // daughters, for each of these heavy hadrons, assigning to this single
382 // decay channel a 100% branching ratio, alt 320 // decay channel a 100% branching ratio, although in reality such a
383 // channel is one between hundreds of possib 321 // channel is one between hundreds of possible ones (and therefore its
384 // real branching ratio is typical of a few 322 // real branching ratio is typical of a few per-cent); moreover, we treat
385 // the decay without any dynamics, i.e. with 323 // the decay without any dynamics, i.e. with a flat phase space kinematical
386 // treatment. 324 // treatment.
387 // Note that some of the charmed and bottom 325 // Note that some of the charmed and bottom hadrons such as SigmaC++,
388 // SigmaC+, SigmaC0, SigmaB+, SigmaB0 and Si 326 // SigmaC+, SigmaC0, SigmaB+, SigmaB0 and SigmaB- have one dominant
389 // decay channel (to LambdaC/B + Pion) which 327 // decay channel (to LambdaC/B + Pion) which is already defined in Geant4.
390 // This is not the case for EtaC, JPsi and U 328 // This is not the case for EtaC, JPsi and Upsilon, whose decays need to
391 // be defined here (although they decay so q 329 // be defined here (although they decay so quickly that their hadronic
392 // interactions can be neglected, as we do f 330 // interactions can be neglected, as we do for Pi0 and Sigma0).
393 // Note that our definition of the decay tab 331 // Note that our definition of the decay tables for these heavy hadrons
394 // do not interfere with the pre-assign deca 332 // do not interfere with the pre-assign decays of primary charmed and
395 // bottom tracks made by the HEP experiments 333 // bottom tracks made by the HEP experiments. In fact, pre-assign decays
396 // have priority over (i.e. override) decay 334 // have priority over (i.e. override) decay tables.
397 static G4bool isFirstCall = true; 335 static G4bool isFirstCall = true;
398 if ( ! isFirstCall ) return; 336 if ( ! isFirstCall ) return;
399 isFirstCall = false; 337 isFirstCall = false;
400 G4ParticleTable* particleTable = G4ParticleT 338 G4ParticleTable* particleTable = G4ParticleTable::GetParticleTable();
401 for ( auto & pdg : G4HadParticles::GetBCHadr 339 for ( auto & pdg : G4HadParticles::GetBCHadrons() ) {
402 auto part = particleTable->FindParticle( p 340 auto part = particleTable->FindParticle( pdg );
403 if ( part == nullptr ) { 341 if ( part == nullptr ) {
404 G4cout << "G4HadronicBuilder::BuildDecay 342 G4cout << "G4HadronicBuilder::BuildDecayTableForBCHadrons : ERROR ! particlePDG="
405 << pdg << " is not defined !" << 343 << pdg << " is not defined !" << G4endl;
406 continue; 344 continue;
407 } 345 }
408 if ( part->GetDecayTable() ) { 346 if ( part->GetDecayTable() ) {
409 G4cout << "G4HadronicBuilder::BuildDecay 347 G4cout << "G4HadronicBuilder::BuildDecayTableForBCHadrons : WARNING ! particlePDG="
410 << pdg << " has already a decay t 348 << pdg << " has already a decay table defined !" << G4endl;
411 continue; 349 continue;
412 } 350 }
413 G4DecayTable* decayTable = new G4DecayTabl 351 G4DecayTable* decayTable = new G4DecayTable;
414 const G4int numberDecayChannels = 1; 352 const G4int numberDecayChannels = 1;
415 G4VDecayChannel** mode = new G4VDecayChann 353 G4VDecayChannel** mode = new G4VDecayChannel*[ numberDecayChannels ];
416 for ( G4int i = 0; i < numberDecayChannels <<
417 switch ( pdg ) { 354 switch ( pdg ) {
418 // Charmed mesons 355 // Charmed mesons
419 case 411 : // D+ 356 case 411 : // D+
420 mode[0] = new G4PhaseSpaceDecayChannel 357 mode[0] = new G4PhaseSpaceDecayChannel( "D+", 1.0, 3, "kaon-", "pi+", "pi+" );
421 break; 358 break;
422 case -411 : // D- 359 case -411 : // D-
423 mode[0] = new G4PhaseSpaceDecayChannel 360 mode[0] = new G4PhaseSpaceDecayChannel( "D-", 1.0, 3, "kaon+", "pi-", "pi-" );
424 break; 361 break;
425 case 421 : // D0 362 case 421 : // D0
426 mode[0] = new G4PhaseSpaceDecayChannel 363 mode[0] = new G4PhaseSpaceDecayChannel( "D0", 1.0, 3, "kaon-", "pi+", "pi0" );
427 break; 364 break;
428 case -421 : // anti_D0 365 case -421 : // anti_D0
429 mode[0] = new G4PhaseSpaceDecayChannel 366 mode[0] = new G4PhaseSpaceDecayChannel( "anti_D0", 1.0, 3, "kaon+", "pi-", "pi0" );
430 break; 367 break;
431 case 431 : // Ds+ 368 case 431 : // Ds+
432 mode[0] = new G4PhaseSpaceDecayChannel 369 mode[0] = new G4PhaseSpaceDecayChannel( "Ds+", 1.0, 3, "kaon+", "kaon-", "pi+" );
433 break; 370 break;
434 case -431 : // Ds- 371 case -431 : // Ds-
435 mode[0] = new G4PhaseSpaceDecayChannel 372 mode[0] = new G4PhaseSpaceDecayChannel( "Ds-", 1.0, 3, "kaon-", "kaon+", "pi-" );
436 break; 373 break;
437 // Bottom mesons 374 // Bottom mesons
438 case 521 : // B+ 375 case 521 : // B+
439 mode[0] = new G4PhaseSpaceDecayChannel 376 mode[0] = new G4PhaseSpaceDecayChannel( "B+", 1.0, 3, "anti_D0", "pi+", "pi0" );
440 break; 377 break;
441 case -521 : // B- 378 case -521 : // B-
442 mode[0] = new G4PhaseSpaceDecayChannel 379 mode[0] = new G4PhaseSpaceDecayChannel( "B-", 1.0, 3, "D0", "pi-", "pi0" );
443 break; 380 break;
444 case 511 : // B0 381 case 511 : // B0
445 mode[0] = new G4PhaseSpaceDecayChannel 382 mode[0] = new G4PhaseSpaceDecayChannel( "B0", 1.0, 3, "D-", "pi+", "pi0" );
446 break; 383 break;
447 case -511 : // anti_B0 384 case -511 : // anti_B0
448 mode[0] = new G4PhaseSpaceDecayChannel 385 mode[0] = new G4PhaseSpaceDecayChannel( "anti_B0", 1.0, 3, "D+", "pi-", "pi0" );
449 break; 386 break;
450 case 531 : // Bs0 387 case 531 : // Bs0
451 mode[0] = new G4PhaseSpaceDecayChannel 388 mode[0] = new G4PhaseSpaceDecayChannel( "Bs0", 1.0, 3, "Ds-", "pi+", "pi0" );
452 break; 389 break;
453 case -531 : // anti_Bs0 390 case -531 : // anti_Bs0
454 mode[0] = new G4PhaseSpaceDecayChannel 391 mode[0] = new G4PhaseSpaceDecayChannel( "anti_Bs0", 1.0, 3, "Ds+", "pi-", "pi0" );
455 break; 392 break;
456 case 541 : // Bc+ 393 case 541 : // Bc+
457 mode[0] = new G4PhaseSpaceDecayChannel 394 mode[0] = new G4PhaseSpaceDecayChannel( "Bc+", 1.0, 2, "J/psi", "pi+" );
458 break; 395 break;
459 case -541 : // Bc- 396 case -541 : // Bc-
460 mode[0] = new G4PhaseSpaceDecayChannel 397 mode[0] = new G4PhaseSpaceDecayChannel( "Bc-", 1.0, 2, "J/psi", "pi-" );
461 break; 398 break;
462 // Charmed baryons (and anti-baryons) 399 // Charmed baryons (and anti-baryons)
463 case 4122 : // lambda_c+ 400 case 4122 : // lambda_c+
464 mode[0] = new G4PhaseSpaceDecayChannel 401 mode[0] = new G4PhaseSpaceDecayChannel( "lambda_c+", 1.0, 3, "proton", "kaon-", "pi+" );
465 break; 402 break;
466 case -4122 : // anti_lambda_c+ 403 case -4122 : // anti_lambda_c+
467 mode[0] = new G4PhaseSpaceDecayChannel 404 mode[0] = new G4PhaseSpaceDecayChannel( "anti_lambda_c+", 1.0, 3, "anti_proton", "kaon+", "pi-" );
468 break; 405 break;
469 case 4232 : // xi_c+ 406 case 4232 : // xi_c+
470 mode[0] = new G4PhaseSpaceDecayChannel 407 mode[0] = new G4PhaseSpaceDecayChannel( "xi_c+", 1.0, 3, "sigma+", "kaon-", "pi+" );
471 break; 408 break;
472 case -4232 : // anti_xi_c+ 409 case -4232 : // anti_xi_c+
473 mode[0] = new G4PhaseSpaceDecayChannel 410 mode[0] = new G4PhaseSpaceDecayChannel( "anti_xi_c+", 1.0, 3, "anti_sigma+", "kaon+", "pi-" );
474 break; 411 break;
475 case 4132 : // xi_c0 412 case 4132 : // xi_c0
476 mode[0] = new G4PhaseSpaceDecayChannel 413 mode[0] = new G4PhaseSpaceDecayChannel( "xi_c0", 1.0, 3, "lambda", "kaon-", "pi+" );
477 break; 414 break;
478 case -4132 : // anti_xi_c0 415 case -4132 : // anti_xi_c0
479 mode[0] = new G4PhaseSpaceDecayChannel 416 mode[0] = new G4PhaseSpaceDecayChannel( "anti_xi_c0", 1.0, 3, "anti_lambda", "kaon+", "pi-" );
480 break; 417 break;
481 case 4332 : // omega_c0 418 case 4332 : // omega_c0
482 mode[0] = new G4PhaseSpaceDecayChannel 419 mode[0] = new G4PhaseSpaceDecayChannel( "omega_c0", 1.0, 3, "xi0", "kaon-", "pi+" );
483 break; 420 break;
484 case -4332 : // anti_omega_c0 421 case -4332 : // anti_omega_c0
485 mode[0] = new G4PhaseSpaceDecayChannel 422 mode[0] = new G4PhaseSpaceDecayChannel( "anti_omega_c0", 1.0, 3, "anti_xi0", "kaon+", "pi-" );
486 break; 423 break;
487 // Bottom baryons (and anti-baryons) 424 // Bottom baryons (and anti-baryons)
488 case 5122 : // lambda_b 425 case 5122 : // lambda_b
489 mode[0] = new G4PhaseSpaceDecayChannel 426 mode[0] = new G4PhaseSpaceDecayChannel( "lambda_b", 1.0, 4, "lambda_c+", "pi+", "pi-", "pi-" );
490 break; 427 break;
491 case -5122 : // anti_lambda_b 428 case -5122 : // anti_lambda_b
492 mode[0] = new G4PhaseSpaceDecayChannel 429 mode[0] = new G4PhaseSpaceDecayChannel( "anti_lambda_b", 1.0, 4, "anti_lambda_c+", "pi-", "pi+", "pi+" );
493 break; 430 break;
494 case 5232 : // xi_b0 431 case 5232 : // xi_b0
495 mode[0] = new G4PhaseSpaceDecayChannel 432 mode[0] = new G4PhaseSpaceDecayChannel( "xi_b0", 1.0, 3, "lambda_c+", "kaon-", "pi0" );
496 break; 433 break;
497 case -5232 : // anti_xi_b0 434 case -5232 : // anti_xi_b0
498 mode[0] = new G4PhaseSpaceDecayChannel 435 mode[0] = new G4PhaseSpaceDecayChannel( "anti_xi_b0", 1.0, 3, "anti_lambda_c+", "kaon+", "pi0" );
499 break; 436 break;
500 case 5132 : // xi_b- 437 case 5132 : // xi_b-
501 mode[0] = new G4PhaseSpaceDecayChannel 438 mode[0] = new G4PhaseSpaceDecayChannel( "xi_b-", 1.0, 3, "lambda_c+", "kaon-", "pi-" );
502 break; 439 break;
503 case -5132 : // anti_xi_b- 440 case -5132 : // anti_xi_b-
504 mode[0] = new G4PhaseSpaceDecayChannel 441 mode[0] = new G4PhaseSpaceDecayChannel( "anti_xi_b-", 1.0, 3, "anti_lambda_c+", "kaon+", "pi+" );
505 break; 442 break;
506 case 5332 : // omega_b- 443 case 5332 : // omega_b-
507 mode[0] = new G4PhaseSpaceDecayChannel 444 mode[0] = new G4PhaseSpaceDecayChannel( "omega_b-", 1.0, 3, "xi_c+", "kaon-", "pi-" );
508 break; 445 break;
509 case -5332 : // anti_omega_b- 446 case -5332 : // anti_omega_b-
510 mode[0] = new G4PhaseSpaceDecayChannel 447 mode[0] = new G4PhaseSpaceDecayChannel( "anti_omega_b-", 1.0, 3, "anti_xi_c+", "kaon+", "pi+" );
511 break; 448 break;
512 default : 449 default :
513 G4cout << "G4HadronicBuilder::BuildDec 450 G4cout << "G4HadronicBuilder::BuildDecayTableForBCHadrons : UNKNOWN particlePDG=" << pdg << G4endl;
514 } // End of the switch 451 } // End of the switch
515 452
516 for ( G4int index = 0; index < numberDecay 453 for ( G4int index = 0; index < numberDecayChannels; ++index ) decayTable->Insert( mode[index] );
517 delete [] mode; 454 delete [] mode;
518 part->SetDecayTable( decayTable ); 455 part->SetDecayTable( decayTable );
519 } // End of the for loop over heavy hadrons 456 } // End of the for loop over heavy hadrons
520 // Add now the decay for etac, JPsi and Upsi 457 // Add now the decay for etac, JPsi and Upsilon because these can be produced as
521 // secondaries in hadronic interactions, whi 458 // secondaries in hadronic interactions, while they are not part of the heavy
522 // hadrons included in G4HadParticles::GetBC 459 // hadrons included in G4HadParticles::GetBCHadrons() because they live too shortly
523 // and therefore their hadronic interactions 460 // and therefore their hadronic interactions can be neglected (as we do for pi0 and sigma0).
524 if ( ! G4Etac::Definition()->GetDecayTable() 461 if ( ! G4Etac::Definition()->GetDecayTable() ) {
525 G4DecayTable* decayTable = new G4DecayTabl 462 G4DecayTable* decayTable = new G4DecayTable;
526 const G4int numberDecayChannels = 1; 463 const G4int numberDecayChannels = 1;
527 G4VDecayChannel** mode = new G4VDecayChann 464 G4VDecayChannel** mode = new G4VDecayChannel*[ numberDecayChannels ];
528 for ( G4int i = 0; i < numberDecayChannels <<
529 mode[0] = new G4PhaseSpaceDecayChannel( "e 465 mode[0] = new G4PhaseSpaceDecayChannel( "etac", 1.0, 3, "eta", "pi+", "pi-" );
530 for ( G4int index = 0; index < numberDecay 466 for ( G4int index = 0; index < numberDecayChannels; ++index ) decayTable->Insert( mode[index] );
531 delete [] mode; 467 delete [] mode;
532 G4Etac::Definition()->SetDecayTable( decay 468 G4Etac::Definition()->SetDecayTable( decayTable );
533 } 469 }
534 if ( ! G4JPsi::Definition()->GetDecayTable() 470 if ( ! G4JPsi::Definition()->GetDecayTable() ) {
535 G4DecayTable* decayTable = new G4DecayTabl 471 G4DecayTable* decayTable = new G4DecayTable;
536 const G4int numberDecayChannels = 1; 472 const G4int numberDecayChannels = 1;
537 G4VDecayChannel** mode = new G4VDecayChann 473 G4VDecayChannel** mode = new G4VDecayChannel*[ numberDecayChannels ];
538 for ( G4int i = 0; i < numberDecayChannels <<
539 mode[0] = new G4PhaseSpaceDecayChannel( "J 474 mode[0] = new G4PhaseSpaceDecayChannel( "J/psi", 1.0, 3, "pi0", "pi+", "pi-" );
540 for ( G4int index = 0; index < numberDecay 475 for ( G4int index = 0; index < numberDecayChannels; ++index ) decayTable->Insert( mode[index] );
541 delete [] mode; 476 delete [] mode;
542 G4JPsi::Definition()->SetDecayTable( decay 477 G4JPsi::Definition()->SetDecayTable( decayTable );
543 } 478 }
544 if ( ! G4Upsilon::Definition()->GetDecayTabl 479 if ( ! G4Upsilon::Definition()->GetDecayTable() ) {
545 G4DecayTable* decayTable = new G4DecayTabl 480 G4DecayTable* decayTable = new G4DecayTable;
546 const G4int numberDecayChannels = 1; 481 const G4int numberDecayChannels = 1;
547 G4VDecayChannel** mode = new G4VDecayChann 482 G4VDecayChannel** mode = new G4VDecayChannel*[ numberDecayChannels ];
548 for ( G4int i = 0; i < numberDecayChannels <<
549 mode[0] = new G4PhaseSpaceDecayChannel( "U 483 mode[0] = new G4PhaseSpaceDecayChannel( "Upsilon", 1.0, 3, "eta_prime", "pi+", "pi-" );
550 for ( G4int index = 0; index < numberDecay 484 for ( G4int index = 0; index < numberDecayChannels; ++index ) decayTable->Insert( mode[index] );
551 delete [] mode; 485 delete [] mode;
552 G4Upsilon::Definition()->SetDecayTable( de 486 G4Upsilon::Definition()->SetDecayTable( decayTable );
553 } 487 }
554 } <<
555 <<
556 <<
557 void G4HadronicBuilder::BuildHyperNucleiFTFP_B <<
558 if ( G4HadronicParameters::Instance()->Enabl <<
559 // Bertini intra-nuclear cascade model is <<
560 // hypernuclei, therefore FTFP is used dow <<
561 // very low energies, a dummy model is use <<
562 // hypernucleus in the final state). <<
563 BuildFTFP_BERT( G4HadParticles::GetHyperNu <<
564 } <<
565 } <<
566 <<
567 <<
568 void G4HadronicBuilder::BuildHyperAntiNucleiFT <<
569 if ( G4HadronicParameters::Instance()->Enabl <<
570 // FTFP can be used down to zero kinetic e <<
571 BuildFTFP_BERT( G4HadParticles::GetHyperAn <<
572 } <<
573 } <<
574 <<
575 <<
576 void G4HadronicBuilder::BuildHyperNucleiFTFP_I <<
577 if ( G4HadronicParameters::Instance()->Enabl <<
578 BuildFTFP_INCLXX( G4HadParticles::GetHyper <<
579 } <<
580 } <<
581 <<
582 <<
583 void G4HadronicBuilder::BuildFTFP_INCLXX( cons <<
584 G4HadronicParameters* param = G4HadronicPara <<
585 G4PhysicsListHelper* ph = G4PhysicsListHelpe <<
586 auto theTheoFSModel = new G4TheoFSGenerator( <<
587 auto theStringModel = new G4FTFModel; <<
588 theStringModel->SetFragmentationModel( new G <<
589 theTheoFSModel->SetHighEnergyGenerator( theS <<
590 theTheoFSModel->SetTransport( new G4Generato <<
591 theTheoFSModel->SetMaxEnergy( param->GetMaxE <<
592 theTheoFSModel->SetMinEnergy( 15.0*CLHEP::Ge <<
593 G4VPreCompoundModel* thePrecoModel = new G4P <<
594 thePrecoModel->SetMinEnergy( 0.0 ); <<
595 thePrecoModel->SetMaxEnergy( 2.0*CLHEP::MeV <<
596 G4INCLXXInterface* theINCLXXModel = new G4IN <<
597 theINCLXXModel->SetMinEnergy( 1.0*CLHEP::MeV <<
598 theINCLXXModel->SetMaxEnergy( 20.0*CLHEP::Ge <<
599 auto xsinel = G4HadProcesses::InelasticXS( x <<
600 G4ParticleTable* table = G4ParticleTable::Ge <<
601 for ( auto & pdg : partList ) { <<
602 auto part = table->FindParticle( pdg ); <<
603 if ( part == nullptr ) continue; <<
604 auto hadi = new G4HadronInelasticProcess( <<
605 hadi->AddDataSet( xsinel ); <<
606 hadi->RegisterMe( theTheoFSModel ); <<
607 hadi->RegisterMe( theINCLXXModel ); <<
608 if ( param->ApplyFactorXS() ) hadi->Multip <<
609 ph->RegisterProcess( hadi, part ); <<
610 } <<
611 } 488 }
612 489