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35 // 35 //
36 // %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 36 // %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
37 // 37 //
38 // MODULE: G4WilsonAblationModel. 38 // MODULE: G4WilsonAblationModel.cc
39 // 39 //
40 // Version: 1.0 40 // Version: 1.0
41 // Date: 08/12/2009 41 // Date: 08/12/2009
42 // Author: P R Truscott 42 // Author: P R Truscott
43 // Organisation: QinetiQ Ltd, UK 43 // Organisation: QinetiQ Ltd, UK
44 // Customer: ESA/ESTEC, NOORDWIJK 44 // Customer: ESA/ESTEC, NOORDWIJK
45 // Contract: 17191/03/NL/LvH 45 // Contract: 17191/03/NL/LvH
46 // 46 //
47 // %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 47 // %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
48 // 48 //
49 // CHANGE HISTORY 49 // CHANGE HISTORY
50 // -------------- 50 // --------------
51 // 51 //
52 // 6 October 2003, P R Truscott, QinetiQ Ltd, 52 // 6 October 2003, P R Truscott, QinetiQ Ltd, UK
53 // Created. 53 // Created.
54 // 54 //
55 // 15 March 2004, P R Truscott, QinetiQ Ltd, U 55 // 15 March 2004, P R Truscott, QinetiQ Ltd, UK
56 // Beta release 56 // Beta release
57 // 57 //
58 // 08 December 2009, P R Truscott, QinetiQ Ltd 58 // 08 December 2009, P R Truscott, QinetiQ Ltd, UK
59 // Ver 1.0 59 // Ver 1.0
60 // Updated as a result of changes in the G4Eva 60 // Updated as a result of changes in the G4Evaporation classes. These changes
61 // affect mostly SelectSecondariesByEvaporatio 61 // affect mostly SelectSecondariesByEvaporation, and now you have variables
62 // associated with the evaporation model which 62 // associated with the evaporation model which can be changed:
63 // OPTxs to select the inverse cross-sectio 63 // OPTxs to select the inverse cross-section
64 // OPTxs = 0 => Dostrovski's parameter 64 // OPTxs = 0 => Dostrovski's parameterization
65 // OPTxs = 1 or 2 => Chatterjee's paramater 65 // OPTxs = 1 or 2 => Chatterjee's paramaterization
66 // OPTxs = 3 or 4 => Kalbach's parameteriza 66 // OPTxs = 3 or 4 => Kalbach's parameterization
67 // useSICB => use superimposed Coulo 67 // useSICB => use superimposed Coulomb Barrier for inverse cross
68 // sections 68 // sections
69 // Other problem found with G4Fragment definit 69 // Other problem found with G4Fragment definition using Lorentz vector and
70 // **G4ParticleDefinition**. This does not al 70 // **G4ParticleDefinition**. This does not allow A and Z to be defined for the
71 // fragment for some reason. Now the fragment 71 // fragment for some reason. Now the fragment is defined more explicitly:
72 // G4Fragment *fragment = new G4Fragment(A, 72 // G4Fragment *fragment = new G4Fragment(A, Z, lorentzVector);
73 // to avoid this quirk. Bug found in SelectSe 73 // to avoid this quirk. Bug found in SelectSecondariesByDefault: *type is now
74 // equated to evapType[i] whereas previously i 74 // equated to evapType[i] whereas previously it was equated to fragType[i].
75 // 75 //
76 // 06 August 2015, A. Ribon, CERN 76 // 06 August 2015, A. Ribon, CERN
77 // Migrated std::exp and std::pow to the faste 77 // Migrated std::exp and std::pow to the faster G4Exp and G4Pow.
78 // 78 //
79 // 09 June 2017, C. Mancini Terracciano, INFN <<
80 // Fixed bug on the initialization of Photon E <<
81 // <<
82 // %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 79 // %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
83 ////////////////////////////////////////////// 80 ////////////////////////////////////////////////////////////////////////////////
84 // 81 //
85 #include <iomanip> 82 #include <iomanip>
86 #include <numeric> 83 #include <numeric>
87 84
88 #include "G4WilsonAblationModel.hh" 85 #include "G4WilsonAblationModel.hh"
89 #include "G4PhysicalConstants.hh" 86 #include "G4PhysicalConstants.hh"
90 #include "G4SystemOfUnits.hh" 87 #include "G4SystemOfUnits.hh"
91 #include "Randomize.hh" 88 #include "Randomize.hh"
92 #include "G4ParticleTable.hh" 89 #include "G4ParticleTable.hh"
93 #include "G4IonTable.hh" 90 #include "G4IonTable.hh"
94 #include "G4Alpha.hh" 91 #include "G4Alpha.hh"
95 #include "G4He3.hh" 92 #include "G4He3.hh"
96 #include "G4Triton.hh" 93 #include "G4Triton.hh"
97 #include "G4Deuteron.hh" 94 #include "G4Deuteron.hh"
98 #include "G4Proton.hh" 95 #include "G4Proton.hh"
99 #include "G4Neutron.hh" 96 #include "G4Neutron.hh"
100 #include "G4AlphaEvaporationChannel.hh" 97 #include "G4AlphaEvaporationChannel.hh"
101 #include "G4He3EvaporationChannel.hh" 98 #include "G4He3EvaporationChannel.hh"
102 #include "G4TritonEvaporationChannel.hh" 99 #include "G4TritonEvaporationChannel.hh"
103 #include "G4DeuteronEvaporationChannel.hh" 100 #include "G4DeuteronEvaporationChannel.hh"
104 #include "G4ProtonEvaporationChannel.hh" 101 #include "G4ProtonEvaporationChannel.hh"
105 #include "G4NeutronEvaporationChannel.hh" 102 #include "G4NeutronEvaporationChannel.hh"
106 #include "G4PhotonEvaporation.hh" 103 #include "G4PhotonEvaporation.hh"
107 #include "G4LorentzVector.hh" 104 #include "G4LorentzVector.hh"
108 #include "G4VEvaporationChannel.hh" 105 #include "G4VEvaporationChannel.hh"
109 106
110 #include "G4Exp.hh" 107 #include "G4Exp.hh"
111 #include "G4Pow.hh" 108 #include "G4Pow.hh"
112 109
113 #include "G4PhysicsModelCatalog.hh" <<
114 110
115 ////////////////////////////////////////////// 111 ////////////////////////////////////////////////////////////////////////////////
116 // 112 //
117 G4WilsonAblationModel::G4WilsonAblationModel() 113 G4WilsonAblationModel::G4WilsonAblationModel()
118 { 114 {
119 // 115 //
120 // 116 //
121 // Send message to stdout to advise that the G 117 // Send message to stdout to advise that the G4Abrasion model is being used.
122 // 118 //
123 PrintWelcomeMessage(); 119 PrintWelcomeMessage();
124 // 120 //
125 // 121 //
126 // Set the default verbose level to 0 - no out 122 // Set the default verbose level to 0 - no output.
127 // 123 //
128 verboseLevel = 0; 124 verboseLevel = 0;
129 // 125 //
130 // 126 //
131 // Set the binding energy per nucleon .... did 127 // Set the binding energy per nucleon .... did I mention that this is a crude
132 // model for nuclear de-excitation? 128 // model for nuclear de-excitation?
133 // 129 //
134 B = 10.0 * MeV; 130 B = 10.0 * MeV;
135 // 131 //
136 // 132 //
137 // It is possuble to switch off secondary part 133 // It is possuble to switch off secondary particle production (other than the
138 // final nuclear fragment). The default is on 134 // final nuclear fragment). The default is on.
139 // 135 //
140 produceSecondaries = true; 136 produceSecondaries = true;
141 // 137 //
142 // 138 //
143 // Now we need to define the decay modes. We' 139 // Now we need to define the decay modes. We're using the G4Evaporation model
144 // to help determine the kinematics of the dec 140 // to help determine the kinematics of the decay.
145 // 141 //
146 nFragTypes = 6; 142 nFragTypes = 6;
147 fragType[0] = G4Alpha::Alpha(); 143 fragType[0] = G4Alpha::Alpha();
148 fragType[1] = G4He3::He3(); 144 fragType[1] = G4He3::He3();
149 fragType[2] = G4Triton::Triton(); 145 fragType[2] = G4Triton::Triton();
150 fragType[3] = G4Deuteron::Deuteron(); 146 fragType[3] = G4Deuteron::Deuteron();
151 fragType[4] = G4Proton::Proton(); 147 fragType[4] = G4Proton::Proton();
152 fragType[5] = G4Neutron::Neutron(); 148 fragType[5] = G4Neutron::Neutron();
153 for(G4int i=0; i<200; ++i) { fSig[i] = 0.0; 149 for(G4int i=0; i<200; ++i) { fSig[i] = 0.0; }
154 // 150 //
155 // 151 //
156 // Set verboseLevel default to no output. 152 // Set verboseLevel default to no output.
157 // 153 //
158 verboseLevel = 0; 154 verboseLevel = 0;
159 theChannelFactory = new G4EvaporationFactory 155 theChannelFactory = new G4EvaporationFactory(new G4PhotonEvaporation());
160 theChannels = theChannelFactory->GetChannel( 156 theChannels = theChannelFactory->GetChannel();
161 // 157 //
162 // 158 //
163 // Set defaults for evaporation classes. Thes 159 // Set defaults for evaporation classes. These can be overridden by user
164 // "set" methods. 160 // "set" methods.
165 // 161 //
166 OPTxs = 3; 162 OPTxs = 3;
167 useSICB = false; 163 useSICB = false;
168 fragmentVector = 0; 164 fragmentVector = 0;
169 <<
170 secID = G4PhysicsModelCatalog::GetModelID("m <<
171 } 165 }
172 ////////////////////////////////////////////// 166 ////////////////////////////////////////////////////////////////////////////////
173 // 167 //
174 G4WilsonAblationModel::~G4WilsonAblationModel( 168 G4WilsonAblationModel::~G4WilsonAblationModel()
175 {} 169 {}
176 170
177 ////////////////////////////////////////////// 171 ////////////////////////////////////////////////////////////////////////////////
178 // 172 //
179 G4FragmentVector *G4WilsonAblationModel::Break 173 G4FragmentVector *G4WilsonAblationModel::BreakItUp
180 (const G4Fragment &theNucleus) 174 (const G4Fragment &theNucleus)
181 { 175 {
182 // 176 //
183 // 177 //
184 // Initilise the pointer to the G4FragmentVect 178 // Initilise the pointer to the G4FragmentVector used to return the information
185 // about the breakup. 179 // about the breakup.
186 // 180 //
187 fragmentVector = new G4FragmentVector; 181 fragmentVector = new G4FragmentVector;
188 fragmentVector->clear(); 182 fragmentVector->clear();
189 // 183 //
190 // 184 //
191 // Get the A, Z and excitation of the nucleus. 185 // Get the A, Z and excitation of the nucleus.
192 // 186 //
193 G4int A = theNucleus.GetA_asInt(); 187 G4int A = theNucleus.GetA_asInt();
194 G4int Z = theNucleus.GetZ_asInt(); 188 G4int Z = theNucleus.GetZ_asInt();
195 G4double ex = theNucleus.GetExcitationEnergy 189 G4double ex = theNucleus.GetExcitationEnergy();
196 if (verboseLevel >= 2) 190 if (verboseLevel >= 2)
197 { 191 {
198 G4cout <<"oooooooooooooooooooooooooooooooo 192 G4cout <<"oooooooooooooooooooooooooooooooooooooooo"
199 <<"oooooooooooooooooooooooooooooooo 193 <<"oooooooooooooooooooooooooooooooooooooooo"
200 <<G4endl; 194 <<G4endl;
201 G4cout.precision(6); 195 G4cout.precision(6);
202 G4cout <<"IN G4WilsonAblationModel" <<G4en 196 G4cout <<"IN G4WilsonAblationModel" <<G4endl;
203 G4cout <<"Initial prefragment A=" <<A 197 G4cout <<"Initial prefragment A=" <<A
204 <<", Z=" <<Z 198 <<", Z=" <<Z
205 <<", excitation energy = " <<ex/MeV 199 <<", excitation energy = " <<ex/MeV <<" MeV"
206 <<G4endl; 200 <<G4endl;
207 } 201 }
208 // 202 //
209 // 203 //
210 // Check that there is a nucleus to speak of. 204 // Check that there is a nucleus to speak of. It's possible there isn't one
211 // or its just a proton or neutron. In either 205 // or its just a proton or neutron. In either case, the excitation energy
212 // (from the Lorentz vector) is not used. 206 // (from the Lorentz vector) is not used.
213 // 207 //
214 if (A == 0) 208 if (A == 0)
215 { 209 {
216 if (verboseLevel >= 2) 210 if (verboseLevel >= 2)
217 { 211 {
218 G4cout <<"No nucleus to decay" <<G4endl; 212 G4cout <<"No nucleus to decay" <<G4endl;
219 G4cout <<"oooooooooooooooooooooooooooooo 213 G4cout <<"oooooooooooooooooooooooooooooooooooooooo"
220 <<"oooooooooooooooooooooooooooooo 214 <<"oooooooooooooooooooooooooooooooooooooooo"
221 <<G4endl; 215 <<G4endl;
222 } 216 }
223 return fragmentVector; 217 return fragmentVector;
224 } 218 }
225 else if (A == 1) 219 else if (A == 1)
226 { 220 {
227 G4LorentzVector lorentzVector = theNucleus 221 G4LorentzVector lorentzVector = theNucleus.GetMomentum();
228 lorentzVector.setE(lorentzVector.e()-ex+10 222 lorentzVector.setE(lorentzVector.e()-ex+10.0*eV);
229 if (Z == 0) 223 if (Z == 0)
230 { 224 {
231 G4Fragment *fragment = new G4Fragment(lo 225 G4Fragment *fragment = new G4Fragment(lorentzVector,G4Neutron::Neutron());
232 if (fragment != nullptr) { fragment->Set <<
233 fragmentVector->push_back(fragment); 226 fragmentVector->push_back(fragment);
234 } 227 }
235 else 228 else
236 { 229 {
237 G4Fragment *fragment = new G4Fragment(lo 230 G4Fragment *fragment = new G4Fragment(lorentzVector,G4Proton::Proton());
238 if (fragment != nullptr) { fragment->Set <<
239 fragmentVector->push_back(fragment); 231 fragmentVector->push_back(fragment);
240 } 232 }
241 if (verboseLevel >= 2) 233 if (verboseLevel >= 2)
242 { 234 {
243 G4cout <<"Final fragment is in fact only 235 G4cout <<"Final fragment is in fact only a nucleon) :" <<G4endl;
244 G4cout <<(*fragmentVector)[0] <<G4endl; 236 G4cout <<(*fragmentVector)[0] <<G4endl;
245 G4cout <<"oooooooooooooooooooooooooooooo 237 G4cout <<"oooooooooooooooooooooooooooooooooooooooo"
246 <<"oooooooooooooooooooooooooooooo 238 <<"oooooooooooooooooooooooooooooooooooooooo"
247 <<G4endl; 239 <<G4endl;
248 } 240 }
249 return fragmentVector; 241 return fragmentVector;
250 } 242 }
251 // 243 //
252 // 244 //
253 // Then the number of nucleons ablated (either 245 // Then the number of nucleons ablated (either as nucleons or light nuclear
254 // fragments) is based on a simple argument fo 246 // fragments) is based on a simple argument for the binding energy per nucleon.
255 // 247 //
256 G4int DAabl = (G4int) (ex / B); 248 G4int DAabl = (G4int) (ex / B);
257 if (DAabl > A) DAabl = A; 249 if (DAabl > A) DAabl = A;
258 // The following lines are no longer accurate 250 // The following lines are no longer accurate given we now treat the final fragment
259 // if (verboseLevel >= 2) 251 // if (verboseLevel >= 2)
260 // G4cout <<"Number of nucleons ejected = " 252 // G4cout <<"Number of nucleons ejected = " <<DAabl <<G4endl;
261 253
262 // 254 //
263 // 255 //
264 // Determine the nuclear fragment from the abl 256 // Determine the nuclear fragment from the ablation process by sampling the
265 // Rudstam equation. 257 // Rudstam equation.
266 // 258 //
267 G4int AF = A - DAabl; 259 G4int AF = A - DAabl;
268 G4int ZF = 0; 260 G4int ZF = 0;
269 261
270 if (AF > 0) 262 if (AF > 0)
271 { 263 {
272 G4Pow* g4calc = G4Pow::GetInstance(); << 264 G4Pow* g4pow = G4Pow::GetInstance();
273 G4double AFd = (G4double) AF; 265 G4double AFd = (G4double) AF;
274 G4double R = 11.8 / g4calc->powZ(AF, 0.45) << 266 G4double R = 11.8 / g4pow->powZ(AF, 0.45);
275 G4int minZ = std::max(1, Z - DAabl); 267 G4int minZ = std::max(1, Z - DAabl);
276 // 268 //
277 // 269 //
278 // Here we define an integral probability dist 270 // Here we define an integral probability distribution based on the Rudstam
279 // equation assuming a constant AF. 271 // equation assuming a constant AF.
280 // 272 //
281 G4int zmax = std::min(199, Z); 273 G4int zmax = std::min(199, Z);
282 G4double sum = 0.0; 274 G4double sum = 0.0;
283 for (ZF=minZ; ZF<=zmax; ++ZF) 275 for (ZF=minZ; ZF<=zmax; ++ZF)
284 { 276 {
285 sum += G4Exp(-R*g4calc->powA(std::abs(ZF << 277 sum += G4Exp(-R*g4pow->powA(std::abs(ZF - 0.486*AFd + 3.8E-04*AFd*AFd),1.5));
286 fSig[ZF] = sum; 278 fSig[ZF] = sum;
287 } 279 }
288 // 280 //
289 // 281 //
290 // Now sample that distribution to determine a 282 // Now sample that distribution to determine a value for ZF.
291 // 283 //
292 sum *= G4UniformRand(); 284 sum *= G4UniformRand();
293 for (ZF=minZ; ZF<=zmax; ++ZF) { 285 for (ZF=minZ; ZF<=zmax; ++ZF) {
294 if(sum <= fSig[ZF]) { break; } 286 if(sum <= fSig[ZF]) { break; }
295 } 287 }
296 } 288 }
297 G4int DZabl = Z - ZF; 289 G4int DZabl = Z - ZF;
298 // 290 //
299 // 291 //
300 // Now determine the nucleons or nuclei which 292 // Now determine the nucleons or nuclei which have bee ablated. The preference
301 // is for the production of alphas, then other 293 // is for the production of alphas, then other nuclei in order of decreasing
302 // binding energy. The energies assigned to th 294 // binding energy. The energies assigned to the products of the decay are
303 // provisional for the moment (the 10eV is jus 295 // provisional for the moment (the 10eV is just to avoid errors with negative
304 // excitation energies due to rounding). 296 // excitation energies due to rounding).
305 // 297 //
306 G4double totalEpost = 0.0; 298 G4double totalEpost = 0.0;
307 evapType.clear(); 299 evapType.clear();
308 for (G4int ift=0; ift<nFragTypes; ift++) 300 for (G4int ift=0; ift<nFragTypes; ift++)
309 { 301 {
310 G4ParticleDefinition *type = fragType[ift] 302 G4ParticleDefinition *type = fragType[ift];
311 G4double n = std::floor((G4double) DAabl 303 G4double n = std::floor((G4double) DAabl / type->GetBaryonNumber() + 1.0E-10);
312 G4double n1 = 1.0E+10; 304 G4double n1 = 1.0E+10;
313 if (fragType[ift]->GetPDGCharge() > 0.0) 305 if (fragType[ift]->GetPDGCharge() > 0.0)
314 n1 = std::floor((G4double) DZabl / type- 306 n1 = std::floor((G4double) DZabl / type->GetPDGCharge() + 1.0E-10);
315 if (n > n1) n = n1; 307 if (n > n1) n = n1;
316 if (n > 0.0) 308 if (n > 0.0)
317 { 309 {
318 G4double mass = type->GetPDGMass(); 310 G4double mass = type->GetPDGMass();
319 for (G4int j=0; j<(G4int) n; j++) 311 for (G4int j=0; j<(G4int) n; j++)
320 { 312 {
321 totalEpost += mass; 313 totalEpost += mass;
322 evapType.push_back(type); 314 evapType.push_back(type);
323 } 315 }
324 DAabl -= (G4int) (n * type->GetBaryonNum 316 DAabl -= (G4int) (n * type->GetBaryonNumber() + 1.0E-10);
325 DZabl -= (G4int) (n * type->GetPDGCharge 317 DZabl -= (G4int) (n * type->GetPDGCharge() + 1.0E-10);
326 } 318 }
327 } 319 }
328 // 320 //
329 // 321 //
330 // Determine the properties of the final nucle 322 // Determine the properties of the final nuclear fragment. Note that if
331 // the final fragment is predicted to have a n 323 // the final fragment is predicted to have a nucleon number of zero, then
332 // really it's the particle last in the vector 324 // really it's the particle last in the vector evapType which becomes the
333 // final fragment. Therefore delete this from 325 // final fragment. Therefore delete this from the vector if this is the
334 // case. 326 // case.
335 // 327 //
336 G4double massFinalFrag = 0.0; 328 G4double massFinalFrag = 0.0;
337 if (AF > 0) 329 if (AF > 0)
338 massFinalFrag = G4ParticleTable::GetPartic 330 massFinalFrag = G4ParticleTable::GetParticleTable()->GetIonTable()->
339 GetIonMass(ZF,AF); 331 GetIonMass(ZF,AF);
340 else 332 else
341 { 333 {
342 G4ParticleDefinition *type = evapType[evap 334 G4ParticleDefinition *type = evapType[evapType.size()-1];
343 AF = type->GetBary 335 AF = type->GetBaryonNumber();
344 ZF = (G4int) (type 336 ZF = (G4int) (type->GetPDGCharge() + 1.0E-10);
345 evapType.erase(evapType.end()-1); 337 evapType.erase(evapType.end()-1);
346 } 338 }
347 totalEpost += massFinalFrag; 339 totalEpost += massFinalFrag;
348 // 340 //
349 // 341 //
350 // Provide verbose output on the nuclear fragm 342 // Provide verbose output on the nuclear fragment if requested.
351 // 343 //
352 if (verboseLevel >= 2) 344 if (verboseLevel >= 2)
353 { 345 {
354 G4cout <<"Final fragment A=" <<AF 346 G4cout <<"Final fragment A=" <<AF
355 <<", Z=" <<ZF 347 <<", Z=" <<ZF
356 <<G4endl; 348 <<G4endl;
357 for (G4int ift=0; ift<nFragTypes; ift++) 349 for (G4int ift=0; ift<nFragTypes; ift++)
358 { 350 {
359 G4ParticleDefinition *type = fragType[if 351 G4ParticleDefinition *type = fragType[ift];
360 G4long n = std::count(evapType.cbegin(), << 352 G4int n = std::count(evapType.begin(),evapType.end(),type);
361 if (n > 0) 353 if (n > 0)
362 G4cout <<"Particle type: " <<std::setw 354 G4cout <<"Particle type: " <<std::setw(10) <<type->GetParticleName()
363 <<", number of particles emitte 355 <<", number of particles emitted = " <<n <<G4endl;
364 } 356 }
365 } 357 }
366 // 358 //
367 // Add the total energy from the fragment. No 359 // Add the total energy from the fragment. Note that the fragment is assumed
368 // to be de-excited and does not undergo photo 360 // to be de-excited and does not undergo photo-evaporation .... I did mention
369 // this is a bit of a crude model? 361 // this is a bit of a crude model?
370 // 362 //
371 G4double massPreFrag = theNucleus.GetGr 363 G4double massPreFrag = theNucleus.GetGroundStateMass();
372 G4double totalEpre = massPreFrag + ex 364 G4double totalEpre = massPreFrag + ex;
373 G4double excess = totalEpre - tota 365 G4double excess = totalEpre - totalEpost;
374 // G4Fragment *resultNucleus(theNucleus); 366 // G4Fragment *resultNucleus(theNucleus);
375 G4Fragment *resultNucleus = new G4Fragment(A 367 G4Fragment *resultNucleus = new G4Fragment(A, Z, theNucleus.GetMomentum());
376 G4ThreeVector boost(0.0,0.0,0.0); 368 G4ThreeVector boost(0.0,0.0,0.0);
377 std::size_t nEvap = 0; << 369 G4int nEvap = 0;
378 if (produceSecondaries && evapType.size()>0) 370 if (produceSecondaries && evapType.size()>0)
379 { 371 {
380 if (excess > 0.0) 372 if (excess > 0.0)
381 { 373 {
382 SelectSecondariesByEvaporation (resultNu 374 SelectSecondariesByEvaporation (resultNucleus);
383 nEvap = fragmentVector->size(); 375 nEvap = fragmentVector->size();
384 boost = resultNucleus->GetMomentum().fin 376 boost = resultNucleus->GetMomentum().findBoostToCM();
385 if (evapType.size() > 0) 377 if (evapType.size() > 0)
386 SelectSecondariesByDefault (boost); 378 SelectSecondariesByDefault (boost);
387 } 379 }
388 else 380 else
389 SelectSecondariesByDefault(G4ThreeVector 381 SelectSecondariesByDefault(G4ThreeVector(0.0,0.0,0.0));
390 } 382 }
391 383
392 if (AF > 0) 384 if (AF > 0)
393 { 385 {
394 G4double mass = G4ParticleTable::GetPartic 386 G4double mass = G4ParticleTable::GetParticleTable()->GetIonTable()->
395 GetIonMass(ZF,AF); 387 GetIonMass(ZF,AF);
396 G4double e = mass + 10.0*eV; 388 G4double e = mass + 10.0*eV;
397 G4double p = std::sqrt(e*e-mass*mass); 389 G4double p = std::sqrt(e*e-mass*mass);
398 G4ThreeVector direction(0.0,0.0,1.0); 390 G4ThreeVector direction(0.0,0.0,1.0);
399 G4LorentzVector lorentzVector = G4LorentzV 391 G4LorentzVector lorentzVector = G4LorentzVector(direction*p, e);
400 lorentzVector.boost(-boost); 392 lorentzVector.boost(-boost);
401 G4Fragment* frag = new G4Fragment(AF, ZF, 393 G4Fragment* frag = new G4Fragment(AF, ZF, lorentzVector);
402 if (frag != nullptr) { frag->SetCreatorMod <<
403 fragmentVector->push_back(frag); 394 fragmentVector->push_back(frag);
404 } 395 }
405 delete resultNucleus; 396 delete resultNucleus;
406 // 397 //
407 // 398 //
408 // Provide verbose output on the ablation prod 399 // Provide verbose output on the ablation products if requested.
409 // 400 //
410 if (verboseLevel >= 2) 401 if (verboseLevel >= 2)
411 { 402 {
412 if (nEvap > 0) 403 if (nEvap > 0)
413 { 404 {
414 G4cout <<"----------------------" <<G4en 405 G4cout <<"----------------------" <<G4endl;
415 G4cout <<"Evaporated particles :" <<G4en 406 G4cout <<"Evaporated particles :" <<G4endl;
416 G4cout <<"----------------------" <<G4en 407 G4cout <<"----------------------" <<G4endl;
417 } 408 }
418 std::size_t ie = 0; << 409 G4int ie = 0;
419 for (auto iter = fragmentVector->cbegin(); << 410 G4FragmentVector::iterator iter;
420 iter != fragmentVector->cend(); << 411 for (iter = fragmentVector->begin(); iter != fragmentVector->end(); iter++)
421 { 412 {
422 if (ie == nEvap) 413 if (ie == nEvap)
423 { 414 {
424 // G4cout <<*iter <<G4endl; 415 // G4cout <<*iter <<G4endl;
425 G4cout <<"---------------------------- 416 G4cout <<"---------------------------------" <<G4endl;
426 G4cout <<"Particles from default emiss 417 G4cout <<"Particles from default emission :" <<G4endl;
427 G4cout <<"---------------------------- 418 G4cout <<"---------------------------------" <<G4endl;
428 } 419 }
429 G4cout <<*iter <<G4endl; 420 G4cout <<*iter <<G4endl;
430 } 421 }
431 G4cout <<"oooooooooooooooooooooooooooooooo 422 G4cout <<"oooooooooooooooooooooooooooooooooooooooo"
432 <<"oooooooooooooooooooooooooooooooo 423 <<"oooooooooooooooooooooooooooooooooooooooo"
433 <<G4endl; 424 <<G4endl;
434 } 425 }
435 426
436 return fragmentVector; 427 return fragmentVector;
437 } 428 }
438 ////////////////////////////////////////////// 429 ////////////////////////////////////////////////////////////////////////////////
439 // 430 //
440 void G4WilsonAblationModel::SelectSecondariesB 431 void G4WilsonAblationModel::SelectSecondariesByEvaporation
441 (G4Fragment *intermediateNucleus) 432 (G4Fragment *intermediateNucleus)
442 { 433 {
443 G4Fragment theResidualNucleus = *intermediat 434 G4Fragment theResidualNucleus = *intermediateNucleus;
444 G4bool evaporate = true; 435 G4bool evaporate = true;
445 // Loop checking, 05-Aug-2015, Vladimir Ivan 436 // Loop checking, 05-Aug-2015, Vladimir Ivanchenko
446 while (evaporate && evapType.size() != 0) 437 while (evaporate && evapType.size() != 0)
447 { 438 {
448 // 439 //
449 // 440 //
450 // Here's the cheaky bit. We're hijacking the 441 // Here's the cheaky bit. We're hijacking the G4Evaporation model, in order to
451 // more accurately sample to kinematics, but t 442 // more accurately sample to kinematics, but the species of the nuclear
452 // fragments will be the ones of our choosing 443 // fragments will be the ones of our choosing as above.
453 // 444 //
454 std::vector <G4VEvaporationChannel*> theC 445 std::vector <G4VEvaporationChannel*> theChannels1;
455 theChannels1.clear(); 446 theChannels1.clear();
456 std::vector <G4VEvaporationChannel*>::iter 447 std::vector <G4VEvaporationChannel*>::iterator i;
457 VectorOfFragmentTypes::iterator iter; 448 VectorOfFragmentTypes::iterator iter;
458 std::vector <VectorOfFragmentTypes::iterat 449 std::vector <VectorOfFragmentTypes::iterator> iters;
459 iters.clear(); 450 iters.clear();
460 iter = std::find(evapType.begin(), evapTyp 451 iter = std::find(evapType.begin(), evapType.end(), G4Alpha::Alpha());
461 if (iter != evapType.end()) 452 if (iter != evapType.end())
462 { 453 {
463 theChannels1.push_back(new G4AlphaEvapor 454 theChannels1.push_back(new G4AlphaEvaporationChannel);
464 i = theChannels1.end() - 1; 455 i = theChannels1.end() - 1;
465 (*i)->SetOPTxs(OPTxs); 456 (*i)->SetOPTxs(OPTxs);
466 (*i)->UseSICB(useSICB); 457 (*i)->UseSICB(useSICB);
467 // (*i)->Initialize(theResidualNucleus); 458 // (*i)->Initialize(theResidualNucleus);
468 iters.push_back(iter); 459 iters.push_back(iter);
469 } 460 }
470 iter = std::find(evapType.begin(), evapTyp 461 iter = std::find(evapType.begin(), evapType.end(), G4He3::He3());
471 if (iter != evapType.end()) 462 if (iter != evapType.end())
472 { 463 {
473 theChannels1.push_back(new G4He3Evaporat 464 theChannels1.push_back(new G4He3EvaporationChannel);
474 i = theChannels1.end() - 1; 465 i = theChannels1.end() - 1;
475 (*i)->SetOPTxs(OPTxs); 466 (*i)->SetOPTxs(OPTxs);
476 (*i)->UseSICB(useSICB); 467 (*i)->UseSICB(useSICB);
477 // (*i)->Initialize(theResidualNucleus); 468 // (*i)->Initialize(theResidualNucleus);
478 iters.push_back(iter); 469 iters.push_back(iter);
479 } 470 }
480 iter = std::find(evapType.begin(), evapTyp 471 iter = std::find(evapType.begin(), evapType.end(), G4Triton::Triton());
481 if (iter != evapType.end()) 472 if (iter != evapType.end())
482 { 473 {
483 theChannels1.push_back(new G4TritonEvapo 474 theChannels1.push_back(new G4TritonEvaporationChannel);
484 i = theChannels1.end() - 1; 475 i = theChannels1.end() - 1;
485 (*i)->SetOPTxs(OPTxs); 476 (*i)->SetOPTxs(OPTxs);
486 (*i)->UseSICB(useSICB); 477 (*i)->UseSICB(useSICB);
487 // (*i)->Initialize(theResidualNucleus); 478 // (*i)->Initialize(theResidualNucleus);
488 iters.push_back(iter); 479 iters.push_back(iter);
489 } 480 }
490 iter = std::find(evapType.begin(), evapTyp 481 iter = std::find(evapType.begin(), evapType.end(), G4Deuteron::Deuteron());
491 if (iter != evapType.end()) 482 if (iter != evapType.end())
492 { 483 {
493 theChannels1.push_back(new G4DeuteronEva 484 theChannels1.push_back(new G4DeuteronEvaporationChannel);
494 i = theChannels1.end() - 1; 485 i = theChannels1.end() - 1;
495 (*i)->SetOPTxs(OPTxs); 486 (*i)->SetOPTxs(OPTxs);
496 (*i)->UseSICB(useSICB); 487 (*i)->UseSICB(useSICB);
497 // (*i)->Initialize(theResidualNucleus); 488 // (*i)->Initialize(theResidualNucleus);
498 iters.push_back(iter); 489 iters.push_back(iter);
499 } 490 }
500 iter = std::find(evapType.begin(), evapTyp 491 iter = std::find(evapType.begin(), evapType.end(), G4Proton::Proton());
501 if (iter != evapType.end()) 492 if (iter != evapType.end())
502 { 493 {
503 theChannels1.push_back(new G4ProtonEvapo 494 theChannels1.push_back(new G4ProtonEvaporationChannel);
504 i = theChannels1.end() - 1; 495 i = theChannels1.end() - 1;
505 (*i)->SetOPTxs(OPTxs); 496 (*i)->SetOPTxs(OPTxs);
506 (*i)->UseSICB(useSICB); 497 (*i)->UseSICB(useSICB);
507 // (*i)->Initialize(theResidualNucleus); 498 // (*i)->Initialize(theResidualNucleus);
508 iters.push_back(iter); 499 iters.push_back(iter);
509 } 500 }
510 iter = std::find(evapType.begin(), evapTyp 501 iter = std::find(evapType.begin(), evapType.end(), G4Neutron::Neutron());
511 if (iter != evapType.end()) 502 if (iter != evapType.end())
512 { 503 {
513 theChannels1.push_back(new G4NeutronEvap 504 theChannels1.push_back(new G4NeutronEvaporationChannel);
514 i = theChannels1.end() - 1; 505 i = theChannels1.end() - 1;
515 (*i)->SetOPTxs(OPTxs); 506 (*i)->SetOPTxs(OPTxs);
516 (*i)->UseSICB(useSICB); 507 (*i)->UseSICB(useSICB);
517 // (*i)->Initialize(theResidualNucleus); 508 // (*i)->Initialize(theResidualNucleus);
518 iters.push_back(iter); 509 iters.push_back(iter);
519 } 510 }
520 std::size_t nChannels = theChannels1.size( << 511 G4int nChannels = theChannels1.size();
521 512
522 G4double totalProb = 0.0; 513 G4double totalProb = 0.0;
523 G4int ich = 0; 514 G4int ich = 0;
524 G4double probEvapType[6] = {0.0}; 515 G4double probEvapType[6] = {0.0};
525 for (auto iterEv=theChannels1.cbegin(); << 516 std::vector<G4VEvaporationChannel*>::iterator iterEv;
526 iterEv!=theChannels1.cend(); ++i << 517 for (iterEv=theChannels1.begin(); iterEv!=theChannels1.end(); iterEv++) {
527 totalProb += (*iterEv)->GetEmissionProba 518 totalProb += (*iterEv)->GetEmissionProbability(intermediateNucleus);
528 probEvapType[ich] = totalProb; 519 probEvapType[ich] = totalProb;
529 ++ich; 520 ++ich;
530 } 521 }
531 if (totalProb > 0.0) { 522 if (totalProb > 0.0) {
532 // 523 //
533 // 524 //
534 // The emission probability for at least one o 525 // The emission probability for at least one of the evaporation channels is
535 // positive, therefore work out which one shou 526 // positive, therefore work out which one should be selected and decay
536 // the nucleus. 527 // the nucleus.
537 // 528 //
538 G4double xi = totalProb*G4UniformRand(); 529 G4double xi = totalProb*G4UniformRand();
539 std::size_t ii = 0; << 530 G4int ii = 0;
540 for (ii=0; ii<nChannels; ++ii) << 531 for (ii=0; ii<nChannels; ii++) {
541 { <<
542 if (xi < probEvapType[ii]) { break; } 532 if (xi < probEvapType[ii]) { break; }
543 } 533 }
544 if (ii >= nChannels) { ii = nChannels - 534 if (ii >= nChannels) { ii = nChannels - 1; }
545 G4FragmentVector *evaporationResult = th 535 G4FragmentVector *evaporationResult = theChannels1[ii]->
546 BreakUpFragment(intermediateNucleus); << 536 BreakUp(*intermediateNucleus);
547 if ((*evaporationResult)[0] != nullptr) <<
548 { <<
549 (*evaporationResult)[0]->SetCreatorMod <<
550 } <<
551 fragmentVector->push_back((*evaporationR 537 fragmentVector->push_back((*evaporationResult)[0]);
552 intermediateNucleus = (*evaporationResul << 538 *intermediateNucleus = *(*evaporationResult)[1];
>> 539 //delete evaporationResult->back();
553 delete evaporationResult; 540 delete evaporationResult;
>> 541 //evapType.erase(iters[ii]);
554 } 542 }
555 else 543 else
556 { 544 {
557 // 545 //
558 // 546 //
559 // Probability for further evaporation is nil 547 // Probability for further evaporation is nil so have to escape from this
560 // routine and set the energies of the seconda 548 // routine and set the energies of the secondaries to 10eV.
561 // 549 //
562 evaporate = false; 550 evaporate = false;
563 } 551 }
564 } 552 }
565 553
566 return; 554 return;
567 } 555 }
568 ////////////////////////////////////////////// 556 ////////////////////////////////////////////////////////////////////////////////
569 // 557 //
570 void G4WilsonAblationModel::SelectSecondariesB 558 void G4WilsonAblationModel::SelectSecondariesByDefault (G4ThreeVector boost)
571 { 559 {
572 for (std::size_t i=0; i<evapType.size(); ++i << 560 for (unsigned i=0; i<evapType.size(); i++)
573 { 561 {
574 G4ParticleDefinition *type = evapType[i]; 562 G4ParticleDefinition *type = evapType[i];
575 G4double mass = type->GetPDGM 563 G4double mass = type->GetPDGMass();
576 G4double e = mass + 10.0*e 564 G4double e = mass + 10.0*eV;
577 G4double p = std::sqrt(e*e 565 G4double p = std::sqrt(e*e-mass*mass);
578 G4double costheta = 2.0*G4Uniform 566 G4double costheta = 2.0*G4UniformRand() - 1.0;
579 G4double sintheta = std::sqrt((1. 567 G4double sintheta = std::sqrt((1.0 - costheta)*(1.0 + costheta));
580 G4double phi = twopi * G4Uni 568 G4double phi = twopi * G4UniformRand() * rad;
581 G4ThreeVector direction(sintheta*std::cos( 569 G4ThreeVector direction(sintheta*std::cos(phi),sintheta*std::sin(phi),costheta);
582 G4LorentzVector lorentzVector = G4LorentzV 570 G4LorentzVector lorentzVector = G4LorentzVector(direction*p, e);
583 lorentzVector.boost(-boost); 571 lorentzVector.boost(-boost);
584 // Possibility that the following line is not 572 // Possibility that the following line is not correctly carrying over A and Z
585 // from particle definition. Force values. P 573 // from particle definition. Force values. PRT 03/12/2009.
586 // G4Fragment *fragment = 574 // G4Fragment *fragment =
587 // new G4Fragment(lorentzVector, type); 575 // new G4Fragment(lorentzVector, type);
588 G4int A = type->GetBaryonNumber(); 576 G4int A = type->GetBaryonNumber();
589 G4int Z = (G4int) (type->GetPDGCharge() + 577 G4int Z = (G4int) (type->GetPDGCharge() + 1.0E-10);
590 G4Fragment *fragment = 578 G4Fragment *fragment =
591 new G4Fragment(A, Z, lorentzVector); 579 new G4Fragment(A, Z, lorentzVector);
592 if (fragment != nullptr) { fragment->SetCr << 580
593 fragmentVector->push_back(fragment); 581 fragmentVector->push_back(fragment);
594 } 582 }
595 } 583 }
596 ////////////////////////////////////////////// 584 ////////////////////////////////////////////////////////////////////////////////
597 // 585 //
598 void G4WilsonAblationModel::PrintWelcomeMessag 586 void G4WilsonAblationModel::PrintWelcomeMessage ()
599 { 587 {
600 G4cout <<G4endl; 588 G4cout <<G4endl;
601 G4cout <<" ********************************* 589 G4cout <<" *****************************************************************"
602 <<G4endl; 590 <<G4endl;
603 G4cout <<" Nuclear ablation model for nuclea 591 G4cout <<" Nuclear ablation model for nuclear-nuclear interactions activated"
604 <<G4endl; 592 <<G4endl;
605 G4cout <<" (Written by QinetiQ Ltd for the E 593 G4cout <<" (Written by QinetiQ Ltd for the European Space Agency)"
606 <<G4endl; 594 <<G4endl;
607 G4cout <<" !!! WARNING: This model is not we 595 G4cout <<" !!! WARNING: This model is not well validation and should not be used for accurate simulation !!!"
608 <<G4endl; 596 <<G4endl;
609 G4cout <<" ********************************* 597 G4cout <<" *****************************************************************"
610 <<G4endl; 598 <<G4endl;
611 G4cout << G4endl; 599 G4cout << G4endl;
612 600
613 return; 601 return;
614 } 602 }
615 ////////////////////////////////////////////// 603 ////////////////////////////////////////////////////////////////////////////////
616 // 604 //
617 605