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26 // $Id: G4ANuMuNucleusNcModel.cc 91806 2015-08 26 // $Id: G4ANuMuNucleusNcModel.cc 91806 2015-08-06 12:20:45Z gcosmo $
27 // 27 //
28 // Geant4 Header : G4ANuMuNucleusNcModel 28 // Geant4 Header : G4ANuMuNucleusNcModel
29 // 29 //
30 // Author : V.Grichine 12.2.19 30 // Author : V.Grichine 12.2.19
31 // 31 //
32 32
33 #include "G4ANuMuNucleusNcModel.hh" 33 #include "G4ANuMuNucleusNcModel.hh"
34 #include "G4NeutrinoNucleusModel.hh" 34 #include "G4NeutrinoNucleusModel.hh"
35 35
36 // #include "G4NuMuResQX.hh" 36 // #include "G4NuMuResQX.hh"
37 37
38 #include "G4SystemOfUnits.hh" 38 #include "G4SystemOfUnits.hh"
39 #include "G4ParticleTable.hh" 39 #include "G4ParticleTable.hh"
40 #include "G4ParticleDefinition.hh" 40 #include "G4ParticleDefinition.hh"
41 #include "G4IonTable.hh" 41 #include "G4IonTable.hh"
42 #include "Randomize.hh" 42 #include "Randomize.hh"
43 #include "G4RandomDirection.hh" 43 #include "G4RandomDirection.hh"
44 44
45 // #include "G4Integrator.hh" 45 // #include "G4Integrator.hh"
46 #include "G4DataVector.hh" 46 #include "G4DataVector.hh"
47 #include "G4PhysicsTable.hh" 47 #include "G4PhysicsTable.hh"
48 #include "G4KineticTrack.hh" 48 #include "G4KineticTrack.hh"
49 #include "G4DecayKineticTracks.hh" 49 #include "G4DecayKineticTracks.hh"
50 #include "G4KineticTrackVector.hh" 50 #include "G4KineticTrackVector.hh"
51 #include "G4Fragment.hh" 51 #include "G4Fragment.hh"
52 #include "G4ReactionProductVector.hh" 52 #include "G4ReactionProductVector.hh"
53 53
54 54
55 #include "G4NeutrinoMu.hh" 55 #include "G4NeutrinoMu.hh"
56 #include "G4AntiNeutrinoMu.hh" 56 #include "G4AntiNeutrinoMu.hh"
57 #include "G4Nucleus.hh" 57 #include "G4Nucleus.hh"
58 #include "G4LorentzVector.hh" 58 #include "G4LorentzVector.hh"
59 59
60 using namespace std; 60 using namespace std;
61 using namespace CLHEP; 61 using namespace CLHEP;
62 62
63 #ifdef G4MULTITHREADED 63 #ifdef G4MULTITHREADED
64 G4Mutex G4ANuMuNucleusNcModel::numuNucleus 64 G4Mutex G4ANuMuNucleusNcModel::numuNucleusModel = G4MUTEX_INITIALIZER;
65 #endif 65 #endif
66 66
67 67
68 G4ANuMuNucleusNcModel::G4ANuMuNucleusNcModel(c 68 G4ANuMuNucleusNcModel::G4ANuMuNucleusNcModel(const G4String& name)
69 : G4NeutrinoNucleusModel(name) 69 : G4NeutrinoNucleusModel(name)
70 { 70 {
71 SetMinEnergy( 0.0*GeV ); 71 SetMinEnergy( 0.0*GeV );
72 SetMaxEnergy( 100.*TeV ); 72 SetMaxEnergy( 100.*TeV );
73 SetMinEnergy(1.e-6*eV); 73 SetMinEnergy(1.e-6*eV);
74 74
75 // theNuMu = G4NeutrinoMu::NeutrinoMu(); 75 // theNuMu = G4NeutrinoMu::NeutrinoMu();
76 theANuMu = G4AntiNeutrinoMu::AntiNeutrinoMu 76 theANuMu = G4AntiNeutrinoMu::AntiNeutrinoMu();
77 77
78 fMnumu = 0.; 78 fMnumu = 0.;
79 fData = fMaster = false; 79 fData = fMaster = false;
80 InitialiseModel(); 80 InitialiseModel();
81 81
82 } 82 }
83 83
84 84
85 G4ANuMuNucleusNcModel::~G4ANuMuNucleusNcModel( 85 G4ANuMuNucleusNcModel::~G4ANuMuNucleusNcModel()
86 {} 86 {}
87 87
88 88
89 void G4ANuMuNucleusNcModel::ModelDescription(s 89 void G4ANuMuNucleusNcModel::ModelDescription(std::ostream& outFile) const
90 { 90 {
91 91
92 outFile << "G4ANuMuNucleusNcModel is a neu 92 outFile << "G4ANuMuNucleusNcModel is a neutrino-nucleus (neutral current) scattering\n"
93 << "model which uses the standard 93 << "model which uses the standard model \n"
94 << "transfer parameterization. Th 94 << "transfer parameterization. The model is fully relativistic\n";
95 95
96 } 96 }
97 97
98 ////////////////////////////////////////////// 98 /////////////////////////////////////////////////////////
99 // 99 //
100 // Read data from G4PARTICLEXSDATA (locally PA 100 // Read data from G4PARTICLEXSDATA (locally PARTICLEXSDATA)
101 101
102 void G4ANuMuNucleusNcModel::InitialiseModel() 102 void G4ANuMuNucleusNcModel::InitialiseModel()
103 { 103 {
104 G4String pName = "anti_nu_mu"; 104 G4String pName = "anti_nu_mu";
105 105
106 G4int nSize(0), i(0), j(0), k(0); 106 G4int nSize(0), i(0), j(0), k(0);
107 107
108 if(!fData) 108 if(!fData)
109 { 109 {
110 #ifdef G4MULTITHREADED 110 #ifdef G4MULTITHREADED
111 G4MUTEXLOCK(&numuNucleusModel); 111 G4MUTEXLOCK(&numuNucleusModel);
112 if(!fData) 112 if(!fData)
113 { 113 {
114 #endif 114 #endif
115 fMaster = true; 115 fMaster = true;
116 #ifdef G4MULTITHREADED 116 #ifdef G4MULTITHREADED
117 } 117 }
118 G4MUTEXUNLOCK(&numuNucleusModel); 118 G4MUTEXUNLOCK(&numuNucleusModel);
119 #endif 119 #endif
120 } 120 }
121 121
122 if(fMaster) 122 if(fMaster)
123 { 123 {
124 const char* path = G4FindDataDir("G4PARTIC << 124 char* path = getenv("G4PARTICLEXSDATA");
125 std::ostringstream ost1, ost2, ost3, ost4; 125 std::ostringstream ost1, ost2, ost3, ost4;
126 ost1 << path << "/" << "neutrino" << "/" < 126 ost1 << path << "/" << "neutrino" << "/" << pName << "/xarraynckr";
127 127
128 std::ifstream filein1( ost1.str().c_str() 128 std::ifstream filein1( ost1.str().c_str() );
129 129
130 // filein.open("$PARTICLEXSDATA/"); 130 // filein.open("$PARTICLEXSDATA/");
131 131
132 filein1>>nSize; 132 filein1>>nSize;
133 133
134 for( k = 0; k < fNbin; ++k ) 134 for( k = 0; k < fNbin; ++k )
135 { 135 {
136 for( i = 0; i <= fNbin; ++i ) 136 for( i = 0; i <= fNbin; ++i )
137 { 137 {
138 filein1 >> fNuMuXarrayKR[k][i]; 138 filein1 >> fNuMuXarrayKR[k][i];
139 // G4cout<< fNuMuXarrayKR[k][i] << " 139 // G4cout<< fNuMuXarrayKR[k][i] << " ";
140 } 140 }
141 } 141 }
142 // G4cout<<G4endl<<G4endl; 142 // G4cout<<G4endl<<G4endl;
143 143
144 ost2 << path << "/" << "neutrino" << "/" < 144 ost2 << path << "/" << "neutrino" << "/" << pName << "/xdistrnckr";
145 std::ifstream filein2( ost2.str().c_str() 145 std::ifstream filein2( ost2.str().c_str() );
146 146
147 filein2>>nSize; 147 filein2>>nSize;
148 148
149 for( k = 0; k < fNbin; ++k ) 149 for( k = 0; k < fNbin; ++k )
150 { 150 {
151 for( i = 0; i < fNbin; ++i ) 151 for( i = 0; i < fNbin; ++i )
152 { 152 {
153 filein2 >> fNuMuXdistrKR[k][i]; 153 filein2 >> fNuMuXdistrKR[k][i];
154 // G4cout<< fNuMuXdistrKR[k][i] << " 154 // G4cout<< fNuMuXdistrKR[k][i] << " ";
155 } 155 }
156 } 156 }
157 // G4cout<<G4endl<<G4endl; 157 // G4cout<<G4endl<<G4endl;
158 158
159 ost3 << path << "/" << "neutrino" << "/" < 159 ost3 << path << "/" << "neutrino" << "/" << pName << "/q2arraynckr";
160 std::ifstream filein3( ost3.str().c_str() 160 std::ifstream filein3( ost3.str().c_str() );
161 161
162 filein3>>nSize; 162 filein3>>nSize;
163 163
164 for( k = 0; k < fNbin; ++k ) 164 for( k = 0; k < fNbin; ++k )
165 { 165 {
166 for( i = 0; i <= fNbin; ++i ) 166 for( i = 0; i <= fNbin; ++i )
167 { 167 {
168 for( j = 0; j <= fNbin; ++j ) 168 for( j = 0; j <= fNbin; ++j )
169 { 169 {
170 filein3 >> fNuMuQarrayKR[k][i][j]; 170 filein3 >> fNuMuQarrayKR[k][i][j];
171 // G4cout<< fNuMuQarrayKR[k][i][j] < 171 // G4cout<< fNuMuQarrayKR[k][i][j] << " ";
172 } 172 }
173 } 173 }
174 } 174 }
175 // G4cout<<G4endl<<G4endl; 175 // G4cout<<G4endl<<G4endl;
176 176
177 ost4 << path << "/" << "neutrino" << "/" < 177 ost4 << path << "/" << "neutrino" << "/" << pName << "/q2distrnckr";
178 std::ifstream filein4( ost4.str().c_str() 178 std::ifstream filein4( ost4.str().c_str() );
179 179
180 filein4>>nSize; 180 filein4>>nSize;
181 181
182 for( k = 0; k < fNbin; ++k ) 182 for( k = 0; k < fNbin; ++k )
183 { 183 {
184 for( i = 0; i <= fNbin; ++i ) 184 for( i = 0; i <= fNbin; ++i )
185 { 185 {
186 for( j = 0; j < fNbin; ++j ) 186 for( j = 0; j < fNbin; ++j )
187 { 187 {
188 filein4 >> fNuMuQdistrKR[k][i][j]; 188 filein4 >> fNuMuQdistrKR[k][i][j];
189 // G4cout<< fNuMuQdistrKR[k][i][j] < 189 // G4cout<< fNuMuQdistrKR[k][i][j] << " ";
190 } 190 }
191 } 191 }
192 } 192 }
193 fData = true; 193 fData = true;
194 } 194 }
195 } 195 }
196 196
197 ////////////////////////////////////////////// 197 /////////////////////////////////////////////////////////
198 198
199 G4bool G4ANuMuNucleusNcModel::IsApplicable(con 199 G4bool G4ANuMuNucleusNcModel::IsApplicable(const G4HadProjectile & aPart,
200 G4Nucleus & ) << 200 G4Nucleus & targetNucleus)
201 { 201 {
202 G4bool result = false; 202 G4bool result = false;
203 G4String pName = aPart.GetDefinition()->GetP 203 G4String pName = aPart.GetDefinition()->GetParticleName();
204 G4double energy = aPart.GetTotalEnergy(); 204 G4double energy = aPart.GetTotalEnergy();
205 205
206 if( pName == "anti_nu_mu" // || pName == "n 206 if( pName == "anti_nu_mu" // || pName == "nu_mu" )
207 && 207 &&
208 energy > fMinNuEnergy 208 energy > fMinNuEnergy )
209 { 209 {
210 result = true; 210 result = true;
211 } 211 }
>> 212 G4int Z = targetNucleus.GetZ_asInt();
>> 213 Z *= 1;
212 214
213 return result; 215 return result;
214 } 216 }
215 217
216 /////////////////////////////////////////// Cl 218 /////////////////////////////////////////// ClusterDecay ////////////////////////////////////////////////////////////
217 // 219 //
218 // 220 //
219 221
220 G4HadFinalState* G4ANuMuNucleusNcModel::ApplyY 222 G4HadFinalState* G4ANuMuNucleusNcModel::ApplyYourself(
221 const G4HadProjectile& aTrack, G4Nucleus& 223 const G4HadProjectile& aTrack, G4Nucleus& targetNucleus)
222 { 224 {
223 theParticleChange.Clear(); 225 theParticleChange.Clear();
224 fProton = f2p2h = fBreak = false; 226 fProton = f2p2h = fBreak = false;
225 const G4HadProjectile* aParticle = &aTrack; 227 const G4HadProjectile* aParticle = &aTrack;
226 G4double energy = aParticle->GetTotalEnergy( 228 G4double energy = aParticle->GetTotalEnergy();
227 229
228 G4String pName = aParticle->GetDefinition() 230 G4String pName = aParticle->GetDefinition()->GetParticleName();
229 231
230 if( energy < fMinNuEnergy ) 232 if( energy < fMinNuEnergy )
231 { 233 {
232 theParticleChange.SetEnergyChange(energy); 234 theParticleChange.SetEnergyChange(energy);
233 theParticleChange.SetMomentumChange(aTrack 235 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
234 return &theParticleChange; 236 return &theParticleChange;
235 } 237 }
236 SampleLVkr( aTrack, targetNucleus); 238 SampleLVkr( aTrack, targetNucleus);
237 239
238 if( fBreak == true || fEmu < fMnumu ) // ~5* 240 if( fBreak == true || fEmu < fMnumu ) // ~5*10^-6
239 { 241 {
240 // G4cout<<"ni, "; 242 // G4cout<<"ni, ";
241 theParticleChange.SetEnergyChange(energy); 243 theParticleChange.SetEnergyChange(energy);
242 theParticleChange.SetMomentumChange(aTrack 244 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
243 return &theParticleChange; 245 return &theParticleChange;
244 } 246 }
245 247
246 // LVs of initial state 248 // LVs of initial state
247 249
248 G4LorentzVector lvp1 = aParticle->Get4Moment 250 G4LorentzVector lvp1 = aParticle->Get4Momentum();
249 G4LorentzVector lvt1( 0., 0., 0., fM1 ); 251 G4LorentzVector lvt1( 0., 0., 0., fM1 );
250 G4double mPip = G4ParticleTable::GetParticle 252 G4double mPip = G4ParticleTable::GetParticleTable()->FindParticle(211)->GetPDGMass();
251 253
252 // 1-pi by fQtransfer && nu-energy 254 // 1-pi by fQtransfer && nu-energy
253 G4LorentzVector lvpip1( 0., 0., 0., mPip ); 255 G4LorentzVector lvpip1( 0., 0., 0., mPip );
254 G4LorentzVector lvsum, lv2, lvX; 256 G4LorentzVector lvsum, lv2, lvX;
255 G4ThreeVector eP; 257 G4ThreeVector eP;
256 G4double cost(1.), sint(0.), phi(0.), muMom( 258 G4double cost(1.), sint(0.), phi(0.), muMom(0.), massX2(0.);
257 G4DynamicParticle* aLept = nullptr; // lepto 259 G4DynamicParticle* aLept = nullptr; // lepton lv
258 260
259 G4int Z = targetNucleus.GetZ_asInt(); 261 G4int Z = targetNucleus.GetZ_asInt();
260 G4int A = targetNucleus.GetA_asInt(); 262 G4int A = targetNucleus.GetA_asInt();
261 G4double mTarg = targetNucleus.AtomicMass(A 263 G4double mTarg = targetNucleus.AtomicMass(A,Z);
262 G4int pdgP(0), qB(0); 264 G4int pdgP(0), qB(0);
263 // G4double mSum = G4ParticleTable::GetParti 265 // G4double mSum = G4ParticleTable::GetParticleTable()->FindParticle(2212)->GetPDGMass() + mPip;
264 266
265 G4int iPi = GetOnePionIndex(energy); 267 G4int iPi = GetOnePionIndex(energy);
266 G4double p1pi = GetNuMuOnePionProb( iPi, ene 268 G4double p1pi = GetNuMuOnePionProb( iPi, energy);
267 269
268 if( p1pi > G4UniformRand() && fCosTheta > 0. 270 if( p1pi > G4UniformRand() && fCosTheta > 0.9 ) // && fQtransfer < 0.95*GeV ) // mu- & coherent pion + nucleus
269 { 271 {
270 // lvsum = lvp1 + lvpip1; 272 // lvsum = lvp1 + lvpip1;
271 lvsum = lvp1 + lvt1; 273 lvsum = lvp1 + lvt1;
272 // cost = fCosThetaPi; 274 // cost = fCosThetaPi;
273 cost = fCosTheta; 275 cost = fCosTheta;
274 sint = std::sqrt( (1.0 - cost)*(1.0 + cost 276 sint = std::sqrt( (1.0 - cost)*(1.0 + cost) );
275 phi = G4UniformRand()*CLHEP::twopi; 277 phi = G4UniformRand()*CLHEP::twopi;
276 eP = G4ThreeVector( sint*std::cos(phi), 278 eP = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost );
277 279
278 // muMom = sqrt(fEmuPi*fEmuPi-fMnumu*fMnum 280 // muMom = sqrt(fEmuPi*fEmuPi-fMnumu*fMnumu);
279 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu); 281 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu);
280 282
281 eP *= muMom; 283 eP *= muMom;
282 284
283 // lv2 = G4LorentzVector( eP, fEmuPi ); 285 // lv2 = G4LorentzVector( eP, fEmuPi );
284 lv2 = G4LorentzVector( eP, fEmu ); 286 lv2 = G4LorentzVector( eP, fEmu );
285 lv2 = fLVl; 287 lv2 = fLVl;
286 288
287 lvX = lvsum - lv2; 289 lvX = lvsum - lv2;
288 lvX = fLVh; 290 lvX = fLVh;
289 massX2 = lvX.m2(); 291 massX2 = lvX.m2();
290 G4double massX = lvX.m(); 292 G4double massX = lvX.m();
291 G4double massR = fLVt.m(); 293 G4double massR = fLVt.m();
292 294
293 // if ( massX2 <= 0. ) // vmg: very rarely 295 // if ( massX2 <= 0. ) // vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved
294 if ( massX2 <= fM1*fM1 ) // 9-3-20 vmg: ve 296 if ( massX2 <= fM1*fM1 ) // 9-3-20 vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved
295 if ( lvX.e() <= fM1 ) // 9-3-20 vmg: ver 297 if ( lvX.e() <= fM1 ) // 9-3-20 vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved
296 { 298 {
297 theParticleChange.SetEnergyChange(energy 299 theParticleChange.SetEnergyChange(energy);
298 theParticleChange.SetMomentumChange(aTra 300 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
299 return &theParticleChange; 301 return &theParticleChange;
300 } 302 }
301 fW2 = massX2; 303 fW2 = massX2;
302 304
303 if( pName == "anti_nu_mu" ) aLept 305 if( pName == "anti_nu_mu" ) aLept = new G4DynamicParticle( theANuMu, lv2 );
304 // else if( pName == "anti_nu_mu") aLept = 306 // else if( pName == "anti_nu_mu") aLept = new G4DynamicParticle( theANuMu, lv2 );
305 else 307 else
306 { 308 {
307 theParticleChange.SetEnergyChange(energy 309 theParticleChange.SetEnergyChange(energy);
308 theParticleChange.SetMomentumChange(aTra 310 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
309 return &theParticleChange; 311 return &theParticleChange;
310 } 312 }
311 313
312 pdgP = 111; 314 pdgP = 111;
313 315
314 G4double eCut; // = fMpi + 0.5*(fMpi*fMpi 316 G4double eCut; // = fMpi + 0.5*(fMpi*fMpi - massX2)/mTarg; // massX -> fMpi
315 317
316 if( A > 1 ) 318 if( A > 1 )
317 { 319 {
318 eCut = (fMpi + mTarg)*(fMpi + mTarg) - ( 320 eCut = (fMpi + mTarg)*(fMpi + mTarg) - (massX + massR)*(massX + massR);
319 eCut /= 2.*massR; 321 eCut /= 2.*massR;
320 eCut += massX; 322 eCut += massX;
321 } 323 }
322 else eCut = fM1 + fMpi; 324 else eCut = fM1 + fMpi;
323 325
324 if ( lvX.e() > eCut ) // && sqrt( GetW2() 326 if ( lvX.e() > eCut ) // && sqrt( GetW2() ) < 1.4*GeV ) //
325 { 327 {
326 CoherentPion( lvX, pdgP, targetNucleus); 328 CoherentPion( lvX, pdgP, targetNucleus);
327 } 329 }
328 else 330 else
329 { 331 {
330 theParticleChange.SetEnergyChange(energy 332 theParticleChange.SetEnergyChange(energy);
331 theParticleChange.SetMomentumChange(aTra 333 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
332 return &theParticleChange; 334 return &theParticleChange;
333 } 335 }
334 theParticleChange.AddSecondary( aLept, fSe << 336 theParticleChange.AddSecondary( aLept );
335 337
336 return &theParticleChange; 338 return &theParticleChange;
337 } 339 }
338 else // lepton part in lab 340 else // lepton part in lab
339 { 341 {
340 lvsum = lvp1 + lvt1; 342 lvsum = lvp1 + lvt1;
341 cost = fCosTheta; 343 cost = fCosTheta;
342 sint = std::sqrt( (1.0 - cost)*(1.0 + cost 344 sint = std::sqrt( (1.0 - cost)*(1.0 + cost) );
343 phi = G4UniformRand()*CLHEP::twopi; 345 phi = G4UniformRand()*CLHEP::twopi;
344 eP = G4ThreeVector( sint*std::cos(phi), 346 eP = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost );
345 347
346 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu); 348 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu);
347 349
348 eP *= muMom; 350 eP *= muMom;
349 351
350 lv2 = G4LorentzVector( eP, fEmu ); 352 lv2 = G4LorentzVector( eP, fEmu );
351 353
352 lvX = lvsum - lv2; 354 lvX = lvsum - lv2;
353 355
354 massX2 = lvX.m2(); 356 massX2 = lvX.m2();
355 357
356 if ( massX2 <= 0. ) // vmg: very rarely ~ 358 if ( massX2 <= 0. ) // vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved
357 { 359 {
358 theParticleChange.SetEnergyChange(energy 360 theParticleChange.SetEnergyChange(energy);
359 theParticleChange.SetMomentumChange(aTra 361 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
360 return &theParticleChange; 362 return &theParticleChange;
361 } 363 }
362 fW2 = massX2; 364 fW2 = massX2;
363 365
364 aLept = new G4DynamicParticle( theANuMu, l 366 aLept = new G4DynamicParticle( theANuMu, lv2 );
365 367
366 theParticleChange.AddSecondary( aLept, fSe << 368 theParticleChange.AddSecondary( aLept );
367 } 369 }
368 370
369 // hadron part 371 // hadron part
370 372
371 fRecoil = nullptr; 373 fRecoil = nullptr;
372 fCascade = false; 374 fCascade = false;
373 fString = false; 375 fString = false;
374 376
375 if( A == 1 ) 377 if( A == 1 )
376 { 378 {
377 qB = 1; 379 qB = 1;
378 380
379 // if( G4UniformRand() > 0.1 ) // > 0.999 381 // if( G4UniformRand() > 0.1 ) // > 0.9999 ) // > 0.0001 ) //
380 { 382 {
381 ClusterDecay( lvX, qB ); 383 ClusterDecay( lvX, qB );
382 } 384 }
383 return &theParticleChange; 385 return &theParticleChange;
384 } 386 }
385 G4Nucleus recoil; 387 G4Nucleus recoil;
386 G4double ratio = G4double(Z)/G4double(A); << 388 G4double rM(0.), ratio = G4double(Z)/G4double(A);
387 389
388 if( ratio > G4UniformRand() ) // proton is e 390 if( ratio > G4UniformRand() ) // proton is excited
389 { 391 {
390 fProton = true; 392 fProton = true;
391 recoil = G4Nucleus(A-1,Z-1); 393 recoil = G4Nucleus(A-1,Z-1);
392 fRecoil = &recoil; 394 fRecoil = &recoil;
>> 395 rM = recoil.AtomicMass(A-1,Z-1);
>> 396
393 fMt = G4ParticleTable::GetParticleTable()- 397 fMt = G4ParticleTable::GetParticleTable()->FindParticle(2212)->GetPDGMass()
394 + G4ParticleTable::GetParticleTable( 398 + G4ParticleTable::GetParticleTable()->FindParticle(111)->GetPDGMass();
395 } 399 }
396 else // excited neutron 400 else // excited neutron
397 { 401 {
398 fProton = false; 402 fProton = false;
399 recoil = G4Nucleus(A-1,Z); 403 recoil = G4Nucleus(A-1,Z);
400 fRecoil = &recoil; 404 fRecoil = &recoil;
>> 405 rM = recoil.AtomicMass(A-1,Z);
>> 406
401 fMt = G4ParticleTable::GetParticleTable()- 407 fMt = G4ParticleTable::GetParticleTable()->FindParticle(2112)->GetPDGMass()
402 + G4ParticleTable::GetParticleTable( 408 + G4ParticleTable::GetParticleTable()->FindParticle(111)->GetPDGMass();
403 } 409 }
404 // G4int index = GetEnergyIndex(energy << 410 G4int index = GetEnergyIndex(energy);
405 G4int nepdg = aParticle->GetDefinition()->Ge << 411 G4double qeTotRat = GetNuMuQeTotRat(index, energy);
406 <<
407 G4double qeTotRat; // = GetNuMuQeTotRat(inde <<
408 qeTotRat = CalculateQEratioA( Z, A, energy, <<
409 412
410 G4ThreeVector dX = (lvX.vect()).unit(); 413 G4ThreeVector dX = (lvX.vect()).unit();
411 G4double eX = lvX.e(); // excited nucleon 414 G4double eX = lvX.e(); // excited nucleon
412 G4double mX = sqrt(massX2); 415 G4double mX = sqrt(massX2);
413 416
414 if( qeTotRat > G4UniformRand() || mX <= fMt 417 if( qeTotRat > G4UniformRand() || mX <= fMt ) // || eX <= 1232.*MeV) // QE
415 { 418 {
416 fString = false; 419 fString = false;
417 420
418 G4double rM; <<
419 if( fProton ) 421 if( fProton )
420 { 422 {
421 fPDGencoding = 2212; 423 fPDGencoding = 2212;
422 fMr = proton_mass_c2; 424 fMr = proton_mass_c2;
423 recoil = G4Nucleus(A-1,Z-1); 425 recoil = G4Nucleus(A-1,Z-1);
424 fRecoil = &recoil; 426 fRecoil = &recoil;
425 rM = recoil.AtomicMass(A-1,Z-1); 427 rM = recoil.AtomicMass(A-1,Z-1);
426 } 428 }
427 else 429 else
428 { 430 {
429 fPDGencoding = 2112; 431 fPDGencoding = 2112;
430 fMr = G4ParticleTable::GetParticleTabl 432 fMr = G4ParticleTable::GetParticleTable()->
431 FindParticle(fPDGencoding)->GetPDGMass(); // 433 FindParticle(fPDGencoding)->GetPDGMass(); // 939.5654133*MeV;
432 recoil = G4Nucleus(A-1,Z); 434 recoil = G4Nucleus(A-1,Z);
433 fRecoil = &recoil; 435 fRecoil = &recoil;
434 rM = recoil.AtomicMass(A-1,Z); 436 rM = recoil.AtomicMass(A-1,Z);
435 } 437 }
436 G4double eTh = fMr+0.5*(fMr*fMr-mX*mX)/rM; 438 G4double eTh = fMr+0.5*(fMr*fMr-mX*mX)/rM;
437 439
438 if(eX <= eTh) // vmg, very rarely out of k 440 if(eX <= eTh) // vmg, very rarely out of kinematics
439 { 441 {
440 theParticleChange.SetEnergyChange(energy 442 theParticleChange.SetEnergyChange(energy);
441 theParticleChange.SetMomentumChange(aTra 443 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit());
442 return &theParticleChange; 444 return &theParticleChange;
443 } 445 }
444 FinalBarion( lvX, 0, fPDGencoding ); // p( 446 FinalBarion( lvX, 0, fPDGencoding ); // p(n)+deexcited recoil
445 } 447 }
446 else // if ( eX < 9500000.*GeV ) // < 25.*Ge 448 else // if ( eX < 9500000.*GeV ) // < 25.*GeV) // < 95.*GeV ) // < 2.5*GeV ) //cluster decay
447 { 449 {
448 if ( fProton && pName == "anti_nu_mu" 450 if ( fProton && pName == "anti_nu_mu" ) qB = 1;
449 else if( !fProton && pName == "anri_nu_mu" 451 else if( !fProton && pName == "anri_nu_mu" ) qB = 0;
450 452
451 ClusterDecay( lvX, qB ); 453 ClusterDecay( lvX, qB );
452 } 454 }
453 return &theParticleChange; 455 return &theParticleChange;
454 } 456 }
455 457
456 458
457 ////////////////////////////////////////////// 459 /////////////////////////////////////////////////////////////////////
458 ////////////////////////////////////////////// 460 ////////////////////////////////////////////////////////////////////
459 ////////////////////////////////////////////// 461 ///////////////////////////////////////////////////////////////////
460 462
461 ////////////////////////////////////////////// 463 /////////////////////////////////////////////////
462 // 464 //
463 // sample x, then Q2 465 // sample x, then Q2
464 466
465 void G4ANuMuNucleusNcModel::SampleLVkr(const G 467 void G4ANuMuNucleusNcModel::SampleLVkr(const G4HadProjectile & aTrack, G4Nucleus& targetNucleus)
466 { 468 {
467 fBreak = false; 469 fBreak = false;
468 G4int A = targetNucleus.GetA_asInt(), iTer(0 470 G4int A = targetNucleus.GetA_asInt(), iTer(0), iTerMax(100);
469 G4int Z = targetNucleus.GetZ_asInt(); 471 G4int Z = targetNucleus.GetZ_asInt();
470 G4double e3(0.), pMu2(0.), pX2(0.), nMom(0.) 472 G4double e3(0.), pMu2(0.), pX2(0.), nMom(0.), rM(0.), hM(0.), tM = targetNucleus.AtomicMass(A,Z);
471 G4double cost(1.), sint(0.), phi(0.), muMom( 473 G4double cost(1.), sint(0.), phi(0.), muMom(0.);
472 G4ThreeVector eP, bst; 474 G4ThreeVector eP, bst;
473 const G4HadProjectile* aParticle = &aTrack; 475 const G4HadProjectile* aParticle = &aTrack;
474 G4LorentzVector lvp1 = aParticle->Get4Moment 476 G4LorentzVector lvp1 = aParticle->Get4Momentum();
475 nMom = NucleonMomentum( targetNucleus ); 477 nMom = NucleonMomentum( targetNucleus );
476 478
477 if( A == 1 || nMom == 0. ) // hydrogen, no F 479 if( A == 1 || nMom == 0. ) // hydrogen, no Fermi motion ???
478 { 480 {
479 fNuEnergy = aParticle->GetTotalEnergy(); 481 fNuEnergy = aParticle->GetTotalEnergy();
480 iTer = 0; 482 iTer = 0;
481 483
482 do 484 do
483 { 485 {
484 fXsample = SampleXkr(fNuEnergy); 486 fXsample = SampleXkr(fNuEnergy);
485 fQtransfer = SampleQkr(fNuEnergy, fXsamp 487 fQtransfer = SampleQkr(fNuEnergy, fXsample);
486 fQ2 = fQtransfer*fQtransfer; 488 fQ2 = fQtransfer*fQtransfer;
487 489
488 if( fXsample > 0. ) 490 if( fXsample > 0. )
489 { 491 {
490 fW2 = fM1*fM1 - fQ2 + fQ2/fXsample; // 492 fW2 = fM1*fM1 - fQ2 + fQ2/fXsample; // sample excited hadron mass
491 fEmu = fNuEnergy - fQ2/2./fM1/fXsample 493 fEmu = fNuEnergy - fQ2/2./fM1/fXsample;
492 } 494 }
493 else 495 else
494 { 496 {
495 fW2 = fM1*fM1; 497 fW2 = fM1*fM1;
496 fEmu = fNuEnergy; 498 fEmu = fNuEnergy;
497 } 499 }
498 e3 = fNuEnergy + fM1 - fEmu; 500 e3 = fNuEnergy + fM1 - fEmu;
499 501
500 // if( e3 < sqrt(fW2) ) G4cout<<"energy 502 // if( e3 < sqrt(fW2) ) G4cout<<"energyX = "<<e3/GeV<<", fW = "<<sqrt(fW2)/GeV<<G4endl; // vmg ~10^-5 for NC
501 503
502 pMu2 = fEmu*fEmu - fMnumu*fMnumu; 504 pMu2 = fEmu*fEmu - fMnumu*fMnumu;
503 pX2 = e3*e3 - fW2; 505 pX2 = e3*e3 - fW2;
504 506
505 fCosTheta = fNuEnergy*fNuEnergy + pMu2 507 fCosTheta = fNuEnergy*fNuEnergy + pMu2 - pX2;
506 fCosTheta /= 2.*fNuEnergy*sqrt(pMu2); 508 fCosTheta /= 2.*fNuEnergy*sqrt(pMu2);
507 iTer++; 509 iTer++;
508 } 510 }
509 while( ( abs(fCosTheta) > 1. || fEmu < fMn 511 while( ( abs(fCosTheta) > 1. || fEmu < fMnumu ) && iTer < iTerMax );
510 512
511 if( iTer >= iTerMax ) { fBreak = true; ret 513 if( iTer >= iTerMax ) { fBreak = true; return; }
512 514
513 if( abs(fCosTheta) > 1.) // vmg: due to bi 515 if( abs(fCosTheta) > 1.) // vmg: due to big Q2/x values. To be improved ...
514 { 516 {
515 G4cout<<"H2: fCosTheta = "<<fCosTheta<<" 517 G4cout<<"H2: fCosTheta = "<<fCosTheta<<", fEmu = "<<fEmu<<G4endl;
516 // fCosTheta = -1. + 2.*G4UniformRand(); 518 // fCosTheta = -1. + 2.*G4UniformRand();
517 if(fCosTheta < -1.) fCosTheta = -1.; 519 if(fCosTheta < -1.) fCosTheta = -1.;
518 if(fCosTheta > 1.) fCosTheta = 1.; 520 if(fCosTheta > 1.) fCosTheta = 1.;
519 } 521 }
520 // LVs 522 // LVs
521 523
522 G4LorentzVector lvt1 = G4LorentzVector( 0 524 G4LorentzVector lvt1 = G4LorentzVector( 0., 0., 0., fM1 );
523 G4LorentzVector lvsum = lvp1 + lvt1; 525 G4LorentzVector lvsum = lvp1 + lvt1;
524 526
525 cost = fCosTheta; 527 cost = fCosTheta;
526 sint = std::sqrt( (1.0 - cost)*(1.0 + cost 528 sint = std::sqrt( (1.0 - cost)*(1.0 + cost) );
527 phi = G4UniformRand()*CLHEP::twopi; 529 phi = G4UniformRand()*CLHEP::twopi;
528 eP = G4ThreeVector( sint*std::cos(phi), 530 eP = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost );
529 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu); 531 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu);
530 eP *= muMom; 532 eP *= muMom;
531 fLVl = G4LorentzVector( eP, fEmu ); 533 fLVl = G4LorentzVector( eP, fEmu );
532 534
533 fLVh = lvsum - fLVl; 535 fLVh = lvsum - fLVl;
534 fLVt = G4LorentzVector( 0., 0., 0., 0. ); 536 fLVt = G4LorentzVector( 0., 0., 0., 0. ); // no recoil
535 } 537 }
536 else // Fermi motion, Q2 in nucleon rest fra 538 else // Fermi motion, Q2 in nucleon rest frame
537 { 539 {
538 G4ThreeVector nMomDir = nMom*G4RandomDirec 540 G4ThreeVector nMomDir = nMom*G4RandomDirection();
539 541
540 if( !f2p2h ) // 1p1h 542 if( !f2p2h ) // 1p1h
541 { 543 {
542 G4Nucleus recoil(A-1,Z); 544 G4Nucleus recoil(A-1,Z);
543 rM = sqrt( recoil.AtomicMass(A-1,Z)*reco 545 rM = sqrt( recoil.AtomicMass(A-1,Z)*recoil.AtomicMass(A-1,Z) + nMom*nMom );
544 hM = tM - rM; 546 hM = tM - rM;
545 547
546 fLVt = G4LorentzVector( nMomDir, sqrt( r 548 fLVt = G4LorentzVector( nMomDir, sqrt( rM*rM+nMom*nMom ) );
547 fLVh = G4LorentzVector(-nMomDir, sqrt( h 549 fLVh = G4LorentzVector(-nMomDir, sqrt( hM*hM+nMom*nMom ) );
548 } 550 }
549 else // 2p2h 551 else // 2p2h
550 { 552 {
551 G4Nucleus recoil(A-2,Z-1); 553 G4Nucleus recoil(A-2,Z-1);
552 rM = recoil.AtomicMass(A-2,Z-1)+sqrt(nMo 554 rM = recoil.AtomicMass(A-2,Z-1)+sqrt(nMom*nMom+fM1*fM1);
553 hM = tM - rM; 555 hM = tM - rM;
554 556
555 fLVt = G4LorentzVector( nMomDir, sqrt( r 557 fLVt = G4LorentzVector( nMomDir, sqrt( rM*rM+nMom*nMom ) );
556 fLVh = G4LorentzVector(-nMomDir, sqrt( h 558 fLVh = G4LorentzVector(-nMomDir, sqrt( hM*hM+nMom*nMom ) );
557 } 559 }
558 // G4cout<<hM<<", "; 560 // G4cout<<hM<<", ";
559 // bst = fLVh.boostVector(); // 9-3-20 561 // bst = fLVh.boostVector(); // 9-3-20
560 562
561 // lvp1.boost(-bst); // 9-3-20 -> nucleon 563 // lvp1.boost(-bst); // 9-3-20 -> nucleon rest system, where Q2 transfer is ???
562 564
563 fNuEnergy = lvp1.e(); 565 fNuEnergy = lvp1.e();
564 iTer = 0; 566 iTer = 0;
565 567
566 do 568 do
567 { 569 {
568 fXsample = SampleXkr(fNuEnergy); 570 fXsample = SampleXkr(fNuEnergy);
569 fQtransfer = SampleQkr(fNuEnergy, fXsamp 571 fQtransfer = SampleQkr(fNuEnergy, fXsample);
570 fQ2 = fQtransfer*fQtransfer; 572 fQ2 = fQtransfer*fQtransfer;
571 573
572 if( fXsample > 0. ) 574 if( fXsample > 0. )
573 { 575 {
574 fW2 = fM1*fM1 - fQ2 + fQ2/fXsample; // 576 fW2 = fM1*fM1 - fQ2 + fQ2/fXsample; // sample excited hadron mass
575 fEmu = fNuEnergy - fQ2/2./fM1/fXsample 577 fEmu = fNuEnergy - fQ2/2./fM1/fXsample;
576 } 578 }
577 else 579 else
578 { 580 {
579 fW2 = fM1*fM1; 581 fW2 = fM1*fM1;
580 fEmu = fNuEnergy; 582 fEmu = fNuEnergy;
581 } 583 }
582 584
583 // if(fEmu < 0.) G4cout<<"fEmu = "<<fEmu 585 // if(fEmu < 0.) G4cout<<"fEmu = "<<fEmu<<" hM = "<<hM<<G4endl;
584 586
585 e3 = fNuEnergy + fM1 - fEmu; 587 e3 = fNuEnergy + fM1 - fEmu;
586 588
587 // if( e3 < sqrt(fW2) ) G4cout<<"energy 589 // if( e3 < sqrt(fW2) ) G4cout<<"energyX = "<<e3/GeV<<", fW = "<<sqrt(fW2)/GeV<<G4endl;
588 590
589 pMu2 = fEmu*fEmu - fMnumu*fMnumu; 591 pMu2 = fEmu*fEmu - fMnumu*fMnumu;
590 pX2 = e3*e3 - fW2; 592 pX2 = e3*e3 - fW2;
591 593
592 fCosTheta = fNuEnergy*fNuEnergy + pMu2 594 fCosTheta = fNuEnergy*fNuEnergy + pMu2 - pX2;
593 fCosTheta /= 2.*fNuEnergy*sqrt(pMu2); 595 fCosTheta /= 2.*fNuEnergy*sqrt(pMu2);
594 iTer++; 596 iTer++;
595 } 597 }
596 while( ( abs(fCosTheta) > 1. || fEmu < fMn 598 while( ( abs(fCosTheta) > 1. || fEmu < fMnumu ) && iTer < iTerMax );
597 599
598 if( iTer >= iTerMax ) { fBreak = true; ret 600 if( iTer >= iTerMax ) { fBreak = true; return; }
599 601
600 if( abs(fCosTheta) > 1.) // vmg: due to bi 602 if( abs(fCosTheta) > 1.) // vmg: due to big Q2/x values. To be improved ...
601 { 603 {
602 G4cout<<"FM: fCosTheta = "<<fCosTheta<<" 604 G4cout<<"FM: fCosTheta = "<<fCosTheta<<", fEmu = "<<fEmu<<G4endl;
603 // fCosTheta = -1. + 2.*G4UniformRand(); 605 // fCosTheta = -1. + 2.*G4UniformRand();
604 if(fCosTheta < -1.) fCosTheta = -1.; 606 if(fCosTheta < -1.) fCosTheta = -1.;
605 if(fCosTheta > 1.) fCosTheta = 1.; 607 if(fCosTheta > 1.) fCosTheta = 1.;
606 } 608 }
607 // LVs 609 // LVs
608 G4LorentzVector lvt1 = G4LorentzVector( 0 610 G4LorentzVector lvt1 = G4LorentzVector( 0., 0., 0., fM1 );
609 G4LorentzVector lvsum = lvp1 + lvt1; 611 G4LorentzVector lvsum = lvp1 + lvt1;
610 612
611 cost = fCosTheta; 613 cost = fCosTheta;
612 sint = std::sqrt( (1.0 - cost)*(1.0 + cost 614 sint = std::sqrt( (1.0 - cost)*(1.0 + cost) );
613 phi = G4UniformRand()*CLHEP::twopi; 615 phi = G4UniformRand()*CLHEP::twopi;
614 eP = G4ThreeVector( sint*std::cos(phi), 616 eP = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost );
615 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu); 617 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu);
616 eP *= muMom; 618 eP *= muMom;
617 fLVl = G4LorentzVector( eP, fEmu ); 619 fLVl = G4LorentzVector( eP, fEmu );
618 fLVh = lvsum - fLVl; 620 fLVh = lvsum - fLVl;
619 // back to lab system 621 // back to lab system
620 // fLVl.boost(bst); // 9-3-20 622 // fLVl.boost(bst); // 9-3-20
621 // fLVh.boost(bst); // 9-3-20 623 // fLVh.boost(bst); // 9-3-20
622 } 624 }
623 //G4cout<<iTer<<", "<<fBreak<<"; "; 625 //G4cout<<iTer<<", "<<fBreak<<"; ";
624 } 626 }
625 627
626 // 628 //
627 // 629 //
628 /////////////////////////// 630 ///////////////////////////
629 631