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Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitation of liability. * 17 // * * 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************************************** 25 // 26 // $Id: G4NuTauNucleusNcModel.cc 91806 2015-08-06 12:20:45Z gcosmo $ 27 // 28 // Geant4 Header : G4NuTauNucleusNcModel 29 // 30 // Author : V.Grichine 12.2.19 31 // 32 33 #include "G4NuTauNucleusNcModel.hh" 34 #include "G4NeutrinoNucleusModel.hh" 35 36 // #include "G4NuMuResQX.hh" 37 38 #include "G4SystemOfUnits.hh" 39 #include "G4ParticleTable.hh" 40 #include "G4ParticleDefinition.hh" 41 #include "G4IonTable.hh" 42 #include "Randomize.hh" 43 #include "G4RandomDirection.hh" 44 45 // #include "G4Integrator.hh" 46 #include "G4DataVector.hh" 47 #include "G4PhysicsTable.hh" 48 #include "G4KineticTrack.hh" 49 #include "G4DecayKineticTracks.hh" 50 #include "G4KineticTrackVector.hh" 51 #include "G4Fragment.hh" 52 #include "G4ReactionProductVector.hh" 53 54 55 #include "G4NeutrinoTau.hh" 56 #include "G4AntiNeutrinoTau.hh" 57 #include "G4Nucleus.hh" 58 #include "G4LorentzVector.hh" 59 60 using namespace std; 61 using namespace CLHEP; 62 63 #ifdef G4MULTITHREADED 64 G4Mutex G4NuTauNucleusNcModel::numuNucleusModel = G4MUTEX_INITIALIZER; 65 #endif 66 67 68 G4NuTauNucleusNcModel::G4NuTauNucleusNcModel(const G4String& name) 69 : G4NeutrinoNucleusModel(name) 70 { 71 SetMinEnergy( 0.0*GeV ); 72 SetMaxEnergy( 100.*TeV ); 73 SetMinEnergy(1.e-6*eV); 74 75 theNuTau = G4NeutrinoTau::NeutrinoTau(); 76 theANuTau = G4AntiNeutrinoTau::AntiNeutrinoTau(); 77 78 fMnumu = 0.; 79 fData = fMaster = false; 80 InitialiseModel(); 81 82 } 83 84 85 G4NuTauNucleusNcModel::~G4NuTauNucleusNcModel() 86 {} 87 88 89 void G4NuTauNucleusNcModel::ModelDescription(std::ostream& outFile) const 90 { 91 92 outFile << "G4NuTauNucleusNcModel is a tau-neutrino-nucleus (neutral current) scattering\n" 93 << "model which uses the standard model \n" 94 << "transfer parameterization. The model is fully relativistic\n"; 95 96 } 97 98 ///////////////////////////////////////////////////////// 99 // 100 // Read data from G4PARTICLEXSDATA (locally PARTICLEXSDATA) 101 102 void G4NuTauNucleusNcModel::InitialiseModel() 103 { 104 G4String pName = "nu_mu"; 105 106 G4int nSize(0), i(0), j(0), k(0); 107 108 if(!fData) 109 { 110 #ifdef G4MULTITHREADED 111 G4MUTEXLOCK(&numuNucleusModel); 112 if(!fData) 113 { 114 #endif 115 fMaster = true; 116 #ifdef G4MULTITHREADED 117 } 118 G4MUTEXUNLOCK(&numuNucleusModel); 119 #endif 120 } 121 122 if(fMaster) 123 { 124 const char* path = G4FindDataDir("G4PARTICLEXSDATA"); 125 std::ostringstream ost1, ost2, ost3, ost4; 126 ost1 << path << "/" << "neutrino" << "/" << pName << "/xarraynckr"; 127 128 std::ifstream filein1( ost1.str().c_str() ); 129 130 // filein.open("$PARTICLEXSDATA/"); 131 132 filein1>>nSize; 133 134 for( k = 0; k < fNbin; ++k ) 135 { 136 for( i = 0; i <= fNbin; ++i ) 137 { 138 filein1 >> fNuMuXarrayKR[k][i]; 139 // G4cout<< fNuMuXarrayKR[k][i] << " "; 140 } 141 } 142 // G4cout<<G4endl<<G4endl; 143 144 ost2 << path << "/" << "neutrino" << "/" << pName << "/xdistrnckr"; 145 std::ifstream filein2( ost2.str().c_str() ); 146 147 filein2>>nSize; 148 149 for( k = 0; k < fNbin; ++k ) 150 { 151 for( i = 0; i < fNbin; ++i ) 152 { 153 filein2 >> fNuMuXdistrKR[k][i]; 154 // G4cout<< fNuMuXdistrKR[k][i] << " "; 155 } 156 } 157 // G4cout<<G4endl<<G4endl; 158 159 ost3 << path << "/" << "neutrino" << "/" << pName << "/q2arraynckr"; 160 std::ifstream filein3( ost3.str().c_str() ); 161 162 filein3>>nSize; 163 164 for( k = 0; k < fNbin; ++k ) 165 { 166 for( i = 0; i <= fNbin; ++i ) 167 { 168 for( j = 0; j <= fNbin; ++j ) 169 { 170 filein3 >> fNuMuQarrayKR[k][i][j]; 171 // G4cout<< fNuMuQarrayKR[k][i][j] << " "; 172 } 173 } 174 } 175 // G4cout<<G4endl<<G4endl; 176 177 ost4 << path << "/" << "neutrino" << "/" << pName << "/q2distrnckr"; 178 std::ifstream filein4( ost4.str().c_str() ); 179 180 filein4>>nSize; 181 182 for( k = 0; k < fNbin; ++k ) 183 { 184 for( i = 0; i <= fNbin; ++i ) 185 { 186 for( j = 0; j < fNbin; ++j ) 187 { 188 filein4 >> fNuMuQdistrKR[k][i][j]; 189 // G4cout<< fNuMuQdistrKR[k][i][j] << " "; 190 } 191 } 192 } 193 fData = true; 194 } 195 } 196 197 ///////////////////////////////////////////////////////// 198 199 G4bool G4NuTauNucleusNcModel::IsApplicable(const G4HadProjectile & aPart, 200 G4Nucleus & ) 201 { 202 G4bool result = false; 203 G4String pName = aPart.GetDefinition()->GetParticleName(); 204 G4double energy = aPart.GetTotalEnergy(); 205 206 if( pName == "nu_tau" // || pName == "anti_nu_tau" ) 207 && 208 energy > fMinNuEnergy ) 209 { 210 result = true; 211 } 212 213 return result; 214 } 215 216 /////////////////////////////////////////// ClusterDecay //////////////////////////////////////////////////////////// 217 // 218 // 219 220 G4HadFinalState* G4NuTauNucleusNcModel::ApplyYourself( 221 const G4HadProjectile& aTrack, G4Nucleus& targetNucleus) 222 { 223 theParticleChange.Clear(); 224 fProton = f2p2h = fBreak = false; 225 const G4HadProjectile* aParticle = &aTrack; 226 G4double energy = aParticle->GetTotalEnergy(); 227 228 G4String pName = aParticle->GetDefinition()->GetParticleName(); 229 230 if( energy < fMinNuEnergy ) 231 { 232 theParticleChange.SetEnergyChange(energy); 233 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit()); 234 return &theParticleChange; 235 } 236 SampleLVkr( aTrack, targetNucleus); 237 238 if( fBreak == true || fEmu < fMnumu ) // ~5*10^-6 239 { 240 // G4cout<<"ni, "; 241 theParticleChange.SetEnergyChange(energy); 242 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit()); 243 return &theParticleChange; 244 } 245 246 // LVs of initial state 247 248 G4LorentzVector lvp1 = aParticle->Get4Momentum(); 249 G4LorentzVector lvt1( 0., 0., 0., fM1 ); 250 G4double mPip = G4ParticleTable::GetParticleTable()->FindParticle(211)->GetPDGMass(); 251 252 // 1-pi by fQtransfer && nu-energy 253 G4LorentzVector lvpip1( 0., 0., 0., mPip ); 254 G4LorentzVector lvsum, lv2, lvX; 255 G4ThreeVector eP; 256 G4double cost(1.), sint(0.), phi(0.), muMom(0.), massX2(0.); 257 G4DynamicParticle* aLept = nullptr; // lepton lv 258 259 G4int Z = targetNucleus.GetZ_asInt(); 260 G4int A = targetNucleus.GetA_asInt(); 261 G4double mTarg = targetNucleus.AtomicMass(A,Z); 262 G4int pdgP(0), qB(0); 263 // G4double mSum = G4ParticleTable::GetParticleTable()->FindParticle(2212)->GetPDGMass() + mPip; 264 265 G4int iPi = GetOnePionIndex(energy); 266 G4double p1pi = GetNuMuOnePionProb( iPi, energy); 267 268 if( p1pi > G4UniformRand() && fCosTheta > 0.9 ) // && fQtransfer < 0.95*GeV ) // mu- & coherent pion + nucleus 269 { 270 // lvsum = lvp1 + lvpip1; 271 lvsum = lvp1 + lvt1; 272 // cost = fCosThetaPi; 273 cost = fCosTheta; 274 sint = std::sqrt( (1.0 - cost)*(1.0 + cost) ); 275 phi = G4UniformRand()*CLHEP::twopi; 276 eP = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost ); 277 278 // muMom = sqrt(fEmuPi*fEmuPi-fMnumu*fMnumu); 279 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu); 280 281 eP *= muMom; 282 283 // lv2 = G4LorentzVector( eP, fEmuPi ); 284 lv2 = G4LorentzVector( eP, fEmu ); 285 lv2 = fLVl; 286 287 lvX = lvsum - lv2; 288 lvX = fLVh; 289 massX2 = lvX.m2(); 290 G4double massX = lvX.m(); 291 G4double massR = fLVt.m(); 292 293 // 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: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved 295 if ( lvX.e() <= fM1 ) // 9-3-20 vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved 296 { 297 theParticleChange.SetEnergyChange(energy); 298 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit()); 299 return &theParticleChange; 300 } 301 fW2 = massX2; 302 303 if( pName == "nu_tau" ) aLept = new G4DynamicParticle( theNuTau, lv2 ); 304 else if( pName == "anti_nu_tau") aLept = new G4DynamicParticle( theANuTau, lv2 ); 305 else 306 { 307 theParticleChange.SetEnergyChange(energy); 308 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit()); 309 return &theParticleChange; 310 } 311 312 pdgP = 111; 313 314 G4double eCut; // = fMpi + 0.5*(fMpi*fMpi - massX2)/mTarg; // massX -> fMpi 315 316 if( A > 1 ) 317 { 318 eCut = (fMpi + mTarg)*(fMpi + mTarg) - (massX + massR)*(massX + massR); 319 eCut /= 2.*massR; 320 eCut += massX; 321 } 322 else eCut = fM1 + fMpi; 323 324 if ( lvX.e() > eCut ) // && sqrt( GetW2() ) < 1.4*GeV ) // 325 { 326 CoherentPion( lvX, pdgP, targetNucleus); 327 } 328 else 329 { 330 theParticleChange.SetEnergyChange(energy); 331 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit()); 332 return &theParticleChange; 333 } 334 theParticleChange.AddSecondary( aLept, fSecID ); 335 336 return &theParticleChange; 337 } 338 else // lepton part in lab 339 { 340 lvsum = lvp1 + lvt1; 341 cost = fCosTheta; 342 sint = std::sqrt( (1.0 - cost)*(1.0 + cost) ); 343 phi = G4UniformRand()*CLHEP::twopi; 344 eP = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost ); 345 346 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu); 347 348 eP *= muMom; 349 350 lv2 = G4LorentzVector( eP, fEmu ); 351 352 lvX = lvsum - lv2; 353 354 massX2 = lvX.m2(); 355 356 if ( massX2 <= 0. ) // vmg: very rarely ~ (1-4)e-6 due to big Q2/x, to be improved 357 { 358 theParticleChange.SetEnergyChange(energy); 359 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit()); 360 return &theParticleChange; 361 } 362 fW2 = massX2; 363 364 aLept = new G4DynamicParticle( theNuTau, lv2 ); 365 366 theParticleChange.AddSecondary( aLept, fSecID ); 367 } 368 369 // hadron part 370 371 fRecoil = nullptr; 372 fCascade = false; 373 fString = false; 374 375 if( A == 1 ) 376 { 377 qB = 1; 378 379 // if( G4UniformRand() > 0.1 ) // > 0.9999 ) // > 0.0001 ) // 380 { 381 ClusterDecay( lvX, qB ); 382 } 383 return &theParticleChange; 384 } 385 G4Nucleus recoil; 386 G4double ratio = G4double(Z)/G4double(A); 387 388 if( ratio > G4UniformRand() ) // proton is excited 389 { 390 fProton = true; 391 recoil = G4Nucleus(A-1,Z-1); 392 fRecoil = &recoil; 393 fMt = G4ParticleTable::GetParticleTable()->FindParticle(2212)->GetPDGMass() 394 + G4ParticleTable::GetParticleTable()->FindParticle(111)->GetPDGMass(); 395 } 396 else // excited neutron 397 { 398 fProton = false; 399 recoil = G4Nucleus(A-1,Z); 400 fRecoil = &recoil; 401 fMt = G4ParticleTable::GetParticleTable()->FindParticle(2112)->GetPDGMass() 402 + G4ParticleTable::GetParticleTable()->FindParticle(111)->GetPDGMass(); 403 } 404 // G4int index = GetEnergyIndex(energy); 405 G4int nepdg = aParticle->GetDefinition()->GetPDGEncoding(); 406 407 G4double qeTotRat; // = GetNuMuQeTotRat(index, energy); 408 qeTotRat = CalculateQEratioA( Z, A, energy, nepdg); 409 410 G4ThreeVector dX = (lvX.vect()).unit(); 411 G4double eX = lvX.e(); // excited nucleon 412 G4double mX = sqrt(massX2); 413 414 if( qeTotRat > G4UniformRand() || mX <= fMt ) // || eX <= 1232.*MeV) // QE 415 { 416 fString = false; 417 418 G4double rM; 419 if( fProton ) 420 { 421 fPDGencoding = 2212; 422 fMr = proton_mass_c2; 423 recoil = G4Nucleus(A-1,Z-1); 424 fRecoil = &recoil; 425 rM = recoil.AtomicMass(A-1,Z-1); 426 } 427 else 428 { 429 fPDGencoding = 2112; 430 fMr = G4ParticleTable::GetParticleTable()-> 431 FindParticle(fPDGencoding)->GetPDGMass(); // 939.5654133*MeV; 432 recoil = G4Nucleus(A-1,Z); 433 fRecoil = &recoil; 434 rM = recoil.AtomicMass(A-1,Z); 435 } 436 G4double eTh = fMr+0.5*(fMr*fMr-mX*mX)/rM; 437 438 if(eX <= eTh) // vmg, very rarely out of kinematics 439 { 440 theParticleChange.SetEnergyChange(energy); 441 theParticleChange.SetMomentumChange(aTrack.Get4Momentum().vect().unit()); 442 return &theParticleChange; 443 } 444 FinalBarion( lvX, 0, fPDGencoding ); // p(n)+deexcited recoil 445 } 446 else // if ( eX < 9500000.*GeV ) // < 25.*GeV) // < 95.*GeV ) // < 2.5*GeV ) //cluster decay 447 { 448 if ( fProton && pName == "nu_tau" ) qB = 1; 449 else if( !fProton && pName == "nu_tau" ) qB = 0; 450 451 ClusterDecay( lvX, qB ); 452 } 453 return &theParticleChange; 454 } 455 456 457 ///////////////////////////////////////////////////////////////////// 458 //////////////////////////////////////////////////////////////////// 459 /////////////////////////////////////////////////////////////////// 460 461 ///////////////////////////////////////////////// 462 // 463 // sample x, then Q2 464 465 void G4NuTauNucleusNcModel::SampleLVkr(const G4HadProjectile & aTrack, G4Nucleus& targetNucleus) 466 { 467 fBreak = false; 468 G4int A = targetNucleus.GetA_asInt(), iTer(0), iTerMax(100); 469 G4int Z = targetNucleus.GetZ_asInt(); 470 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(0.); 472 G4ThreeVector eP, bst; 473 const G4HadProjectile* aParticle = &aTrack; 474 G4LorentzVector lvp1 = aParticle->Get4Momentum(); 475 nMom = NucleonMomentum( targetNucleus ); 476 477 if( A == 1 || nMom == 0. ) // hydrogen, no Fermi motion ??? 478 { 479 fNuEnergy = aParticle->GetTotalEnergy(); 480 iTer = 0; 481 482 do 483 { 484 fXsample = SampleXkr(fNuEnergy); 485 fQtransfer = SampleQkr(fNuEnergy, fXsample); 486 fQ2 = fQtransfer*fQtransfer; 487 488 if( fXsample > 0. ) 489 { 490 fW2 = fM1*fM1 - fQ2 + fQ2/fXsample; // sample excited hadron mass 491 fEmu = fNuEnergy - fQ2/2./fM1/fXsample; 492 } 493 else 494 { 495 fW2 = fM1*fM1; 496 fEmu = fNuEnergy; 497 } 498 e3 = fNuEnergy + fM1 - fEmu; 499 500 // if( e3 < sqrt(fW2) ) G4cout<<"energyX = "<<e3/GeV<<", fW = "<<sqrt(fW2)/GeV<<G4endl; // vmg ~10^-5 for NC 501 502 pMu2 = fEmu*fEmu - fMnumu*fMnumu; 503 pX2 = e3*e3 - fW2; 504 505 fCosTheta = fNuEnergy*fNuEnergy + pMu2 - pX2; 506 fCosTheta /= 2.*fNuEnergy*sqrt(pMu2); 507 iTer++; 508 } 509 while( ( abs(fCosTheta) > 1. || fEmu < fMnumu ) && iTer < iTerMax ); 510 511 if( iTer >= iTerMax ) { fBreak = true; return; } 512 513 if( abs(fCosTheta) > 1.) // vmg: due to big Q2/x values. To be improved ... 514 { 515 G4cout<<"H2: fCosTheta = "<<fCosTheta<<", fEmu = "<<fEmu<<G4endl; 516 // fCosTheta = -1. + 2.*G4UniformRand(); 517 if(fCosTheta < -1.) fCosTheta = -1.; 518 if(fCosTheta > 1.) fCosTheta = 1.; 519 } 520 // LVs 521 522 G4LorentzVector lvt1 = G4LorentzVector( 0., 0., 0., fM1 ); 523 G4LorentzVector lvsum = lvp1 + lvt1; 524 525 cost = fCosTheta; 526 sint = std::sqrt( (1.0 - cost)*(1.0 + cost) ); 527 phi = G4UniformRand()*CLHEP::twopi; 528 eP = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost ); 529 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu); 530 eP *= muMom; 531 fLVl = G4LorentzVector( eP, fEmu ); 532 533 fLVh = lvsum - fLVl; 534 fLVt = G4LorentzVector( 0., 0., 0., 0. ); // no recoil 535 } 536 else // Fermi motion, Q2 in nucleon rest frame 537 { 538 G4ThreeVector nMomDir = nMom*G4RandomDirection(); 539 540 if( !f2p2h ) // 1p1h 541 { 542 G4Nucleus recoil(A-1,Z); 543 rM = sqrt( recoil.AtomicMass(A-1,Z)*recoil.AtomicMass(A-1,Z) + nMom*nMom ); 544 hM = tM - rM; 545 546 fLVt = G4LorentzVector( nMomDir, sqrt( rM*rM+nMom*nMom ) ); 547 fLVh = G4LorentzVector(-nMomDir, sqrt( hM*hM+nMom*nMom ) ); 548 } 549 else // 2p2h 550 { 551 G4Nucleus recoil(A-2,Z-1); 552 rM = recoil.AtomicMass(A-2,Z-1)+sqrt(nMom*nMom+fM1*fM1); 553 hM = tM - rM; 554 555 fLVt = G4LorentzVector( nMomDir, sqrt( rM*rM+nMom*nMom ) ); 556 fLVh = G4LorentzVector(-nMomDir, sqrt( hM*hM+nMom*nMom ) ); 557 } 558 // G4cout<<hM<<", "; 559 // bst = fLVh.boostVector(); // 9-3-20 560 561 // lvp1.boost(-bst); // 9-3-20 -> nucleon rest system, where Q2 transfer is ??? 562 563 fNuEnergy = lvp1.e(); 564 iTer = 0; 565 566 do 567 { 568 fXsample = SampleXkr(fNuEnergy); 569 fQtransfer = SampleQkr(fNuEnergy, fXsample); 570 fQ2 = fQtransfer*fQtransfer; 571 572 if( fXsample > 0. ) 573 { 574 fW2 = fM1*fM1 - fQ2 + fQ2/fXsample; // sample excited hadron mass 575 fEmu = fNuEnergy - fQ2/2./fM1/fXsample; 576 } 577 else 578 { 579 fW2 = fM1*fM1; 580 fEmu = fNuEnergy; 581 } 582 583 // if(fEmu < 0.) G4cout<<"fEmu = "<<fEmu<<" hM = "<<hM<<G4endl; 584 585 e3 = fNuEnergy + fM1 - fEmu; 586 587 // if( e3 < sqrt(fW2) ) G4cout<<"energyX = "<<e3/GeV<<", fW = "<<sqrt(fW2)/GeV<<G4endl; 588 589 pMu2 = fEmu*fEmu - fMnumu*fMnumu; 590 pX2 = e3*e3 - fW2; 591 592 fCosTheta = fNuEnergy*fNuEnergy + pMu2 - pX2; 593 fCosTheta /= 2.*fNuEnergy*sqrt(pMu2); 594 iTer++; 595 } 596 while( ( abs(fCosTheta) > 1. || fEmu < fMnumu ) && iTer < iTerMax ); 597 598 if( iTer >= iTerMax ) { fBreak = true; return; } 599 600 if( abs(fCosTheta) > 1.) // vmg: due to big Q2/x values. To be improved ... 601 { 602 G4cout<<"FM: fCosTheta = "<<fCosTheta<<", fEmu = "<<fEmu<<G4endl; 603 // fCosTheta = -1. + 2.*G4UniformRand(); 604 if(fCosTheta < -1.) fCosTheta = -1.; 605 if(fCosTheta > 1.) fCosTheta = 1.; 606 } 607 // LVs 608 G4LorentzVector lvt1 = G4LorentzVector( 0., 0., 0., fM1 ); 609 G4LorentzVector lvsum = lvp1 + lvt1; 610 611 cost = fCosTheta; 612 sint = std::sqrt( (1.0 - cost)*(1.0 + cost) ); 613 phi = G4UniformRand()*CLHEP::twopi; 614 eP = G4ThreeVector( sint*std::cos(phi), sint*std::sin(phi), cost ); 615 muMom = sqrt(fEmu*fEmu-fMnumu*fMnumu); 616 eP *= muMom; 617 fLVl = G4LorentzVector( eP, fEmu ); 618 fLVh = lvsum - fLVl; 619 // back to lab system 620 // fLVl.boost(bst); // 9-3-20 621 // fLVh.boost(bst); // 9-3-20 622 } 623 //G4cout<<iTer<<", "<<fBreak<<"; "; 624 } 625 626 // 627 // 628 /////////////////////////// 629