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1 // 2 // ******************************************************************** 3 // * License and Disclaimer * 4 // * * 5 // * The Geant4 software is copyright of the Copyright Holders of * 6 // * the Geant4 Collaboration. It is provided under the terms and * 7 // * conditions of the Geant4 Software License, included in the file * 8 // * LICENSE and available at http://cern.ch/geant4/license . These * 9 // * include a list of copyright holders. * 10 // * * 11 // * Neither the authors of this software system, nor their employing * 12 // * institutes,nor the agencies providing financial support for this * 13 // * work make any representation or warranty, express or implied, * 14 // * regarding this software system or assume any liability for its * 15 // * use. 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 // 27 // ------------------------------------------------------------------- 28 // 29 // GEANT4 Class file 30 // 31 // 32 // File name: G4MuPairProductionModel 33 // 34 // Author: Vladimir Ivanchenko on base of Laszlo Urban code 35 // 36 // Creation date: 24.06.2002 37 // 38 // Modifications: 39 // 40 // 04-12-02 Change G4DynamicParticle constructor in PostStep (V.Ivanchenko) 41 // 23-12-02 Change interface in order to move to cut per region (V.Ivanchenko) 42 // 24-01-03 Fix for compounds (V.Ivanchenko) 43 // 27-01-03 Make models region aware (V.Ivanchenko) 44 // 13-02-03 Add model (V.Ivanchenko) 45 // 06-06-03 Fix in cross section calculation for high energy (V.Ivanchenko) 46 // 20-10-03 2*xi in ComputeDDMicroscopicCrossSection (R.Kokoulin) 47 // 8 integration points in ComputeDMicroscopicCrossSection 48 // 12-01-04 Take min cut of e- and e+ not its sum (V.Ivanchenko) 49 // 10-02-04 Update parameterisation using R.Kokoulin model (V.Ivanchenko) 50 // 28-04-04 For complex materials repeat calculation of max energy for each 51 // material (V.Ivanchenko) 52 // 01-11-04 Fix bug inside ComputeDMicroscopicCrossSection (R.Kokoulin) 53 // 08-04-05 Major optimisation of internal interfaces (V.Ivantchenko) 54 // 03-08-05 Add SetParticle method (V.Ivantchenko) 55 // 23-10-05 Add protection in sampling of e+e- pair energy needed for 56 // low cuts (V.Ivantchenko) 57 // 13-02-06 Add ComputeCrossSectionPerAtom (mma) 58 // 24-04-07 Add protection in SelectRandomAtom method (V.Ivantchenko) 59 // 12-05-06 Updated sampling (use cut) in SelectRandomAtom (A.Bogdanov) 60 // 11-10-07 Add ignoreCut flag (V.Ivanchenko) 61 62 // 63 // Class Description: 64 // 65 // 66 // ------------------------------------------------------------------- 67 // 68 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 69 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 70 71 #include "G4MuPairProductionModel.hh" 72 #include "G4PhysicalConstants.hh" 73 #include "G4SystemOfUnits.hh" 74 #include "G4EmParameters.hh" 75 #include "G4Electron.hh" 76 #include "G4Positron.hh" 77 #include "G4MuonMinus.hh" 78 #include "G4MuonPlus.hh" 79 #include "Randomize.hh" 80 #include "G4Material.hh" 81 #include "G4Element.hh" 82 #include "G4ElementVector.hh" 83 #include "G4ElementDataRegistry.hh" 84 #include "G4ProductionCutsTable.hh" 85 #include "G4ParticleChangeForLoss.hh" 86 #include "G4ModifiedMephi.hh" 87 #include "G4Log.hh" 88 #include "G4Exp.hh" 89 #include "G4AutoLock.hh" 90 91 #include <iostream> 92 #include <fstream> 93 94 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 95 96 const G4int G4MuPairProductionModel::ZDATPAIR[] = {1, 4, 13, 29, 92}; 97 98 const G4double G4MuPairProductionModel::xgi[] = { 99 0.0198550717512320, 0.1016667612931865, 0.2372337950418355, 0.4082826787521750, 100 0.5917173212478250, 0.7627662049581645, 0.8983332387068135, 0.9801449282487680 101 }; 102 103 const G4double G4MuPairProductionModel::wgi[] = { 104 0.0506142681451880, 0.1111905172266870, 0.1568533229389435, 0.1813418916891810, 105 0.1813418916891810, 0.1568533229389435, 0.1111905172266870, 0.0506142681451880 106 }; 107 108 namespace 109 { 110 G4Mutex theMuPairMutex = G4MUTEX_INITIALIZER; 111 112 const G4double ak1 = 6.9; 113 const G4double ak2 = 1.0; 114 } 115 116 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 117 118 G4MuPairProductionModel::G4MuPairProductionModel(const G4ParticleDefinition* p, 119 const G4String& nam) 120 : G4VEmModel(nam), 121 factorForCross(CLHEP::fine_structure_const*CLHEP::fine_structure_const* 122 CLHEP::classic_electr_radius*CLHEP::classic_electr_radius* 123 4./(3.*CLHEP::pi)), 124 sqrte(std::sqrt(G4Exp(1.))), 125 minPairEnergy(4.*CLHEP::electron_mass_c2), 126 lowestKinEnergy(0.85*CLHEP::GeV) 127 { 128 nist = G4NistManager::Instance(); 129 130 theElectron = G4Electron::Electron(); 131 thePositron = G4Positron::Positron(); 132 133 if(nullptr != p) { 134 SetParticle(p); 135 lowestKinEnergy = std::max(lowestKinEnergy, p->GetPDGMass()*8.0); 136 } 137 emin = lowestKinEnergy; 138 emax = emin*10000.; 139 SetAngularDistribution(new G4ModifiedMephi()); 140 } 141 142 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 143 144 G4double G4MuPairProductionModel::MinPrimaryEnergy(const G4Material*, 145 const G4ParticleDefinition*, 146 G4double cut) 147 { 148 return std::max(lowestKinEnergy, cut); 149 } 150 151 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 152 153 void G4MuPairProductionModel::Initialise(const G4ParticleDefinition* p, 154 const G4DataVector& cuts) 155 { 156 SetParticle(p); 157 158 if (nullptr == fParticleChange) { 159 fParticleChange = GetParticleChangeForLoss(); 160 161 // define scale of internal table for each thread only once 162 if (0 == nbine) { 163 emin = std::max(lowestKinEnergy, LowEnergyLimit()); 164 emax = std::max(HighEnergyLimit(), emin*2); 165 nbine = std::size_t(nYBinPerDecade*std::log10(emax/emin)); 166 if(nbine < 3) { nbine = 3; } 167 168 ymin = G4Log(minPairEnergy/emin); 169 dy = -ymin/G4double(nbiny); 170 } 171 if (p == particle) { 172 G4int pdg = std::abs(p->GetPDGEncoding()); 173 if (pdg == 2212) { 174 dataName = "pEEPairProd"; 175 } else if (pdg == 321) { 176 dataName = "kaonEEPairProd"; 177 } else if (pdg == 211) { 178 dataName = "pionEEPairProd"; 179 } else if (pdg == 11) { 180 dataName = "eEEPairProd"; 181 } else if (pdg == 13) { 182 if (GetName() == "muToMuonPairProd") { 183 dataName = "muMuMuPairProd"; 184 } else { 185 dataName = "muEEPairProd"; 186 } 187 } 188 } 189 } 190 191 // for low-energy application this process should not work 192 if(lowestKinEnergy >= HighEnergyLimit()) { return; } 193 194 if (p == particle) { 195 fElementData = 196 G4ElementDataRegistry::Instance()->GetElementDataByName(dataName); 197 if (nullptr == fElementData) { 198 G4AutoLock l(&theMuPairMutex); 199 fElementData = 200 G4ElementDataRegistry::Instance()->GetElementDataByName(dataName); 201 if (nullptr == fElementData) { 202 fElementData = new G4ElementData(NZDATPAIR); 203 fElementData->SetName(dataName); 204 } 205 G4bool useDataFile = G4EmParameters::Instance()->RetrieveMuDataFromFile(); 206 if (useDataFile) { useDataFile = RetrieveTables(); } 207 if (!useDataFile) { MakeSamplingTables(); } 208 if (fTableToFile) { StoreTables(); } 209 l.unlock(); 210 } 211 if (IsMaster()) { 212 InitialiseElementSelectors(p, cuts); 213 } 214 } 215 } 216 217 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 218 219 void G4MuPairProductionModel::InitialiseLocal(const G4ParticleDefinition* p, 220 G4VEmModel* masterModel) 221 { 222 if(p == particle && lowestKinEnergy < HighEnergyLimit()) { 223 SetElementSelectors(masterModel->GetElementSelectors()); 224 } 225 } 226 227 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 228 229 G4double G4MuPairProductionModel::ComputeDEDXPerVolume( 230 const G4Material* material, 231 const G4ParticleDefinition*, 232 G4double kineticEnergy, 233 G4double cutEnergy) 234 { 235 G4double dedx = 0.0; 236 if (cutEnergy <= minPairEnergy || kineticEnergy <= lowestKinEnergy) 237 { return dedx; } 238 239 const G4ElementVector* theElementVector = material->GetElementVector(); 240 const G4double* theAtomicNumDensityVector = 241 material->GetAtomicNumDensityVector(); 242 243 // loop for elements in the material 244 for (std::size_t i=0; i<material->GetNumberOfElements(); ++i) { 245 G4double Z = (*theElementVector)[i]->GetZ(); 246 G4double tmax = MaxSecondaryEnergyForElement(kineticEnergy, Z); 247 G4double loss = ComputMuPairLoss(Z, kineticEnergy, cutEnergy, tmax); 248 dedx += loss*theAtomicNumDensityVector[i]; 249 } 250 dedx = std::max(dedx, 0.0); 251 return dedx; 252 } 253 254 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 255 256 G4double G4MuPairProductionModel::ComputMuPairLoss(G4double Z, 257 G4double tkin, 258 G4double cutEnergy, 259 G4double tmax) 260 { 261 G4double loss = 0.0; 262 263 G4double cut = std::min(cutEnergy, tmax); 264 if(cut <= minPairEnergy) { return loss; } 265 266 // calculate the rectricted loss 267 // numerical integration in log(PairEnergy) 268 G4double aaa = G4Log(minPairEnergy); 269 G4double bbb = G4Log(cut); 270 271 G4int kkk = std::min(std::max(G4lrint((bbb-aaa)/ak1 + ak2), 8), 1); 272 G4double hhh = (bbb-aaa)/kkk; 273 G4double x = aaa; 274 275 for (G4int l=0 ; l<kkk; ++l) { 276 for (G4int ll=0; ll<NINTPAIR; ++ll) { 277 G4double ep = G4Exp(x+xgi[ll]*hhh); 278 loss += wgi[ll]*ep*ep*ComputeDMicroscopicCrossSection(tkin, Z, ep); 279 } 280 x += hhh; 281 } 282 loss *= hhh; 283 loss = std::max(loss, 0.0); 284 return loss; 285 } 286 287 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 288 289 G4double G4MuPairProductionModel::ComputeMicroscopicCrossSection( 290 G4double tkin, 291 G4double Z, 292 G4double cutEnergy) 293 { 294 G4double cross = 0.; 295 G4double tmax = MaxSecondaryEnergyForElement(tkin, Z); 296 G4double cut = std::max(cutEnergy, minPairEnergy); 297 if (tmax <= cut) { return cross; } 298 299 G4double aaa = G4Log(cut); 300 G4double bbb = G4Log(tmax); 301 G4int kkk = std::min(std::max(G4lrint((bbb-aaa)/ak1 + ak2), 8), 1); 302 303 G4double hhh = (bbb-aaa)/(kkk); 304 G4double x = aaa; 305 306 for (G4int l=0; l<kkk; ++l) { 307 for (G4int i=0; i<NINTPAIR; ++i) { 308 G4double ep = G4Exp(x + xgi[i]*hhh); 309 cross += ep*wgi[i]*ComputeDMicroscopicCrossSection(tkin, Z, ep); 310 } 311 x += hhh; 312 } 313 314 cross *= hhh; 315 cross = std::max(cross, 0.0); 316 return cross; 317 } 318 319 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 320 321 G4double G4MuPairProductionModel::ComputeDMicroscopicCrossSection( 322 G4double tkin, 323 G4double Z, 324 G4double pairEnergy) 325 // Calculates the differential (D) microscopic cross section 326 // using the cross section formula of R.P. Kokoulin (18/01/98) 327 // Code modified by R.P. Kokoulin, V.N. Ivanchenko (27/01/04) 328 { 329 static const G4double bbbtf= 183. ; 330 static const G4double bbbh = 202.4 ; 331 static const G4double g1tf = 1.95e-5 ; 332 static const G4double g2tf = 5.3e-5 ; 333 static const G4double g1h = 4.4e-5 ; 334 static const G4double g2h = 4.8e-5 ; 335 336 if (pairEnergy <= minPairEnergy) 337 return 0.0; 338 339 G4double totalEnergy = tkin + particleMass; 340 G4double residEnergy = totalEnergy - pairEnergy; 341 342 if (residEnergy <= 0.75*sqrte*z13*particleMass) 343 return 0.0; 344 345 G4double a0 = 1.0 / (totalEnergy * residEnergy); 346 G4double alf = 4.0 * electron_mass_c2 / pairEnergy; 347 G4double rt = std::sqrt(1.0 - alf); 348 G4double delta = 6.0 * particleMass * particleMass * a0; 349 G4double tmnexp = alf/(1.0 + rt) + delta*rt; 350 351 if(tmnexp >= 1.0) { return 0.0; } 352 353 G4double tmn = G4Log(tmnexp); 354 355 G4double massratio = particleMass/CLHEP::electron_mass_c2; 356 G4double massratio2 = massratio*massratio; 357 G4double inv_massratio2 = 1.0 / massratio2; 358 359 // zeta calculation 360 G4double bbb,g1,g2; 361 if( Z < 1.5 ) { bbb = bbbh ; g1 = g1h ; g2 = g2h ; } 362 else { bbb = bbbtf; g1 = g1tf; g2 = g2tf; } 363 364 G4double zeta = 0.0; 365 G4double z1exp = totalEnergy / (particleMass + g1*z23*totalEnergy); 366 367 // 35.221047195922 is the root of zeta1(x) = 0.073 * log(x) - 0.26, so the 368 // condition below is the same as zeta1 > 0.0, but without calling log(x) 369 if (z1exp > 35.221047195922) 370 { 371 G4double z2exp = totalEnergy / (particleMass + g2*z13*totalEnergy); 372 zeta = (0.073 * G4Log(z1exp) - 0.26) / (0.058 * G4Log(z2exp) - 0.14); 373 } 374 375 G4double z2 = Z*(Z+zeta); 376 G4double screen0 = 2.*electron_mass_c2*sqrte*bbb/(z13*pairEnergy); 377 G4double beta = 0.5*pairEnergy*pairEnergy*a0; 378 G4double xi0 = 0.5*massratio2*beta; 379 380 // Gaussian integration in ln(1-ro) ( with 8 points) 381 G4double rho[NINTPAIR]; 382 G4double rho2[NINTPAIR]; 383 G4double xi[NINTPAIR]; 384 G4double xi1[NINTPAIR]; 385 G4double xii[NINTPAIR]; 386 387 for (G4int i = 0; i < NINTPAIR; ++i) 388 { 389 rho[i] = G4Exp(tmn*xgi[i]) - 1.0; // rho = -asymmetry 390 rho2[i] = rho[i] * rho[i]; 391 xi[i] = xi0*(1.0-rho2[i]); 392 xi1[i] = 1.0 + xi[i]; 393 xii[i] = 1.0 / xi[i]; 394 } 395 396 G4double ye1[NINTPAIR]; 397 G4double ym1[NINTPAIR]; 398 399 G4double b40 = 4.0 * beta; 400 G4double b62 = 6.0 * beta + 2.0; 401 402 for (G4int i = 0; i < NINTPAIR; ++i) 403 { 404 G4double yeu = (b40 + 5.0) + (b40 - 1.0) * rho2[i]; 405 G4double yed = b62*G4Log(3.0 + xii[i]) + (2.0 * beta - 1.0)*rho2[i] - b40; 406 407 G4double ymu = b62 * (1.0 + rho2[i]) + 6.0; 408 G4double ymd = (b40 + 3.0)*(1.0 + rho2[i])*G4Log(3.0 + xi[i]) 409 + 2.0 - 3.0 * rho2[i]; 410 411 ye1[i] = 1.0 + yeu / yed; 412 ym1[i] = 1.0 + ymu / ymd; 413 } 414 415 G4double be[NINTPAIR]; 416 G4double bm[NINTPAIR]; 417 418 for(G4int i = 0; i < NINTPAIR; ++i) { 419 if(xi[i] <= 1000.0) { 420 be[i] = ((2.0 + rho2[i])*(1.0 + beta) + 421 xi[i]*(3.0 + rho2[i]))*G4Log(1.0 + xii[i]) + 422 (1.0 - rho2[i] - beta)/xi1[i] - (3.0 + rho2[i]); 423 } else { 424 be[i] = 0.5*(3.0 - rho2[i] + 2.0*beta*(1.0 + rho2[i]))*xii[i]; 425 } 426 427 if(xi[i] >= 0.001) { 428 G4double a10 = (1.0 + 2.0 * beta) * (1.0 - rho2[i]); 429 bm[i] = ((1.0 + rho2[i])*(1.0 + 1.5 * beta) - a10*xii[i])*G4Log(xi1[i]) + 430 xi[i] * (1.0 - rho2[i] - beta)/xi1[i] + a10; 431 } else { 432 bm[i] = 0.5*(5.0 - rho2[i] + beta * (3.0 + rho2[i]))*xi[i]; 433 } 434 } 435 436 G4double sum = 0.0; 437 438 for (G4int i = 0; i < NINTPAIR; ++i) { 439 G4double screen = screen0*xi1[i]/(1.0 - rho2[i]); 440 G4double ale = G4Log(bbb/z13*std::sqrt(xi1[i]*ye1[i])/(1. + screen*ye1[i])); 441 G4double cre = 0.5*G4Log(1. + 2.25*z23*xi1[i]*ye1[i]*inv_massratio2); 442 443 G4double fe = (ale-cre)*be[i]; 444 fe = std::max(fe, 0.0); 445 446 G4double alm_crm = G4Log(bbb*massratio/(1.5*z23*(1. + screen*ym1[i]))); 447 G4double fm = std::max(alm_crm*bm[i], 0.0)*inv_massratio2; 448 449 sum += wgi[i]*(1.0 + rho[i])*(fe + fm); 450 } 451 452 return -tmn*sum*factorForCross*z2*residEnergy/(totalEnergy*pairEnergy); 453 } 454 455 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 456 457 G4double G4MuPairProductionModel::ComputeCrossSectionPerAtom( 458 const G4ParticleDefinition*, 459 G4double kineticEnergy, 460 G4double Z, G4double, 461 G4double cutEnergy, 462 G4double maxEnergy) 463 { 464 G4double cross = 0.0; 465 if (kineticEnergy <= lowestKinEnergy) { return cross; } 466 467 G4double maxPairEnergy = MaxSecondaryEnergyForElement(kineticEnergy, Z); 468 G4double tmax = std::min(maxEnergy, maxPairEnergy); 469 G4double cut = std::max(cutEnergy, minPairEnergy); 470 if (cut >= tmax) { return cross; } 471 472 cross = ComputeMicroscopicCrossSection(kineticEnergy, Z, cut); 473 if(tmax < kineticEnergy) { 474 cross -= ComputeMicroscopicCrossSection(kineticEnergy, Z, tmax); 475 } 476 return cross; 477 } 478 479 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 480 481 void G4MuPairProductionModel::MakeSamplingTables() 482 { 483 G4double factore = G4Exp(G4Log(emax/emin)/G4double(nbine)); 484 485 for (G4int iz=0; iz<NZDATPAIR; ++iz) { 486 487 G4double Z = ZDATPAIR[iz]; 488 G4Physics2DVector* pv = new G4Physics2DVector(nbiny+1,nbine+1); 489 G4double kinEnergy = emin; 490 491 for (std::size_t it=0; it<=nbine; ++it) { 492 493 pv->PutY(it, G4Log(kinEnergy/CLHEP::MeV)); 494 G4double maxPairEnergy = MaxSecondaryEnergyForElement(kinEnergy, Z); 495 /* 496 G4cout << "it= " << it << " E= " << kinEnergy 497 << " " << particle->GetParticleName() 498 << " maxE= " << maxPairEnergy << " minE= " << minPairEnergy 499 << " ymin= " << ymin << G4endl; 500 */ 501 G4double coef = G4Log(minPairEnergy/kinEnergy)/ymin; 502 G4double ymax = G4Log(maxPairEnergy/kinEnergy)/coef; 503 G4double fac = (ymax - ymin)/dy; 504 std::size_t imax = (std::size_t)fac; 505 fac -= (G4double)imax; 506 507 G4double xSec = 0.0; 508 G4double x = ymin; 509 /* 510 G4cout << "Z= " << currentZ << " z13= " << z13 511 << " mE= " << maxPairEnergy << " ymin= " << ymin 512 << " dy= " << dy << " c= " << coef << G4endl; 513 */ 514 // start from zero 515 pv->PutValue(0, it, 0.0); 516 if(0 == it) { pv->PutX(nbiny, 0.0); } 517 518 for (std::size_t i=0; i<nbiny; ++i) { 519 520 if(0 == it) { pv->PutX(i, x); } 521 522 if(i < imax) { 523 G4double ep = kinEnergy*G4Exp(coef*(x + dy*0.5)); 524 525 // not multiplied by interval, because table 526 // will be used only for sampling 527 //G4cout << "i= " << i << " x= " << x << "E= " << kinEnergy 528 // << " Egamma= " << ep << G4endl; 529 xSec += ep*ComputeDMicroscopicCrossSection(kinEnergy, Z, ep); 530 531 // last bin before the kinematic limit 532 } else if(i == imax) { 533 G4double ep = kinEnergy*G4Exp(coef*(x + fac*dy*0.5)); 534 xSec += ep*fac*ComputeDMicroscopicCrossSection(kinEnergy, Z, ep); 535 } 536 pv->PutValue(i + 1, it, xSec); 537 x += dy; 538 } 539 kinEnergy *= factore; 540 541 // to avoid precision lost 542 if(it+1 == nbine) { kinEnergy = emax; } 543 } 544 fElementData->InitialiseForElement(iz, pv); 545 } 546 } 547 548 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 549 550 void G4MuPairProductionModel::SampleSecondaries( 551 std::vector<G4DynamicParticle*>* vdp, 552 const G4MaterialCutsCouple* couple, 553 const G4DynamicParticle* aDynamicParticle, 554 G4double tmin, 555 G4double tmax) 556 { 557 G4double kinEnergy = aDynamicParticle->GetKineticEnergy(); 558 //G4cout << "------- G4MuPairProductionModel::SampleSecondaries E(MeV)= " 559 // << kinEnergy << " " 560 // << aDynamicParticle->GetDefinition()->GetParticleName() << G4endl; 561 G4double totalEnergy = kinEnergy + particleMass; 562 G4double totalMomentum = 563 std::sqrt(kinEnergy*(kinEnergy + 2.0*particleMass)); 564 565 G4ThreeVector partDirection = aDynamicParticle->GetMomentumDirection(); 566 567 // select randomly one element constituing the material 568 const G4Element* anElement = SelectRandomAtom(couple,particle,kinEnergy); 569 570 // define interval of energy transfer 571 G4double maxPairEnergy = MaxSecondaryEnergyForElement(kinEnergy, 572 anElement->GetZ()); 573 G4double maxEnergy = std::min(tmax, maxPairEnergy); 574 G4double minEnergy = std::max(tmin, minPairEnergy); 575 576 if (minEnergy >= maxEnergy) { return; } 577 //G4cout << "emin= " << minEnergy << " emax= " << maxEnergy 578 // << " minPair= " << minPairEnergy << " maxpair= " << maxPairEnergy 579 // << " ymin= " << ymin << " dy= " << dy << G4endl; 580 581 G4double coeff = G4Log(minPairEnergy/kinEnergy)/ymin; 582 583 // compute limits 584 G4double yymin = G4Log(minEnergy/kinEnergy)/coeff; 585 G4double yymax = G4Log(maxEnergy/kinEnergy)/coeff; 586 587 //G4cout << "yymin= " << yymin << " yymax= " << yymax << G4endl; 588 589 // units should not be used, bacause table was built without 590 G4double logTkin = G4Log(kinEnergy/CLHEP::MeV); 591 592 // sample e-e+ energy, pair energy first 593 594 // select sample table via Z 595 G4int iz1(0), iz2(0); 596 for (G4int iz=0; iz<NZDATPAIR; ++iz) { 597 if(currentZ == ZDATPAIR[iz]) { 598 iz1 = iz2 = iz; 599 break; 600 } else if(currentZ < ZDATPAIR[iz]) { 601 iz2 = iz; 602 if(iz > 0) { iz1 = iz-1; } 603 else { iz1 = iz2; } 604 break; 605 } 606 } 607 if (0 == iz1) { iz1 = iz2 = NZDATPAIR-1; } 608 609 G4double pairEnergy = 0.0; 610 G4int count = 0; 611 //G4cout << "start loop Z1= " << iz1 << " Z2= " << iz2 << G4endl; 612 do { 613 ++count; 614 // sampling using only one random number 615 G4double rand = G4UniformRand(); 616 617 G4double x = FindScaledEnergy(iz1, rand, logTkin, yymin, yymax); 618 if(iz1 != iz2) { 619 G4double x2 = FindScaledEnergy(iz2, rand, logTkin, yymin, yymax); 620 G4double lz1= nist->GetLOGZ(ZDATPAIR[iz1]); 621 G4double lz2= nist->GetLOGZ(ZDATPAIR[iz2]); 622 //G4cout << count << ". x= " << x << " x2= " << x2 623 // << " Z1= " << iz1 << " Z2= " << iz2 << G4endl; 624 x += (x2 - x)*(lnZ - lz1)/(lz2 - lz1); 625 } 626 //G4cout << "x= " << x << " coeff= " << coeff << G4endl; 627 pairEnergy = kinEnergy*G4Exp(x*coeff); 628 629 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko 630 } while((pairEnergy < minEnergy || pairEnergy > maxEnergy) && 10 > count); 631 632 //G4cout << "## pairEnergy(GeV)= " << pairEnergy/GeV 633 // << " Etot(GeV)= " << totalEnergy/GeV << G4endl; 634 635 // sample r=(E+-E-)/pairEnergy ( uniformly .....) 636 G4double rmax = 637 (1.-6.*particleMass*particleMass/(totalEnergy*(totalEnergy-pairEnergy))) 638 *std::sqrt(1.-minPairEnergy/pairEnergy); 639 G4double r = rmax * (-1.+2.*G4UniformRand()) ; 640 641 // compute energies from pairEnergy,r 642 G4double eEnergy = (1.-r)*pairEnergy*0.5; 643 G4double pEnergy = pairEnergy - eEnergy; 644 645 // Sample angles 646 G4ThreeVector eDirection, pDirection; 647 // 648 GetAngularDistribution()->SamplePairDirections(aDynamicParticle, 649 eEnergy, pEnergy, 650 eDirection, pDirection); 651 // create G4DynamicParticle object for e+e- 652 eEnergy = std::max(eEnergy - CLHEP::electron_mass_c2, 0.0); 653 pEnergy = std::max(pEnergy - CLHEP::electron_mass_c2, 0.0); 654 auto aParticle1 = new G4DynamicParticle(theElectron,eDirection,eEnergy); 655 auto aParticle2 = new G4DynamicParticle(thePositron,pDirection,pEnergy); 656 // Fill output vector 657 vdp->push_back(aParticle1); 658 vdp->push_back(aParticle2); 659 660 // primary change 661 kinEnergy -= pairEnergy; 662 partDirection *= totalMomentum; 663 partDirection -= (aParticle1->GetMomentum() + aParticle2->GetMomentum()); 664 partDirection = partDirection.unit(); 665 666 // if energy transfer is higher than threshold (very high by default) 667 // then stop tracking the primary particle and create a new secondary 668 if (pairEnergy > SecondaryThreshold()) { 669 fParticleChange->ProposeTrackStatus(fStopAndKill); 670 fParticleChange->SetProposedKineticEnergy(0.0); 671 auto newdp = new G4DynamicParticle(particle, partDirection, kinEnergy); 672 vdp->push_back(newdp); 673 } else { // continue tracking the primary e-/e+ otherwise 674 fParticleChange->SetProposedMomentumDirection(partDirection); 675 fParticleChange->SetProposedKineticEnergy(kinEnergy); 676 } 677 //G4cout << "-- G4MuPairProductionModel::SampleSecondaries done" << G4endl; 678 } 679 680 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 681 682 G4double 683 G4MuPairProductionModel::FindScaledEnergy(G4int iz, G4double rand, 684 G4double logTkin, 685 G4double yymin, G4double yymax) 686 { 687 G4double res = yymin; 688 G4Physics2DVector* pv = fElementData->GetElement2DData(iz); 689 if (nullptr != pv) { 690 G4double pmin = pv->Value(yymin, logTkin); 691 G4double pmax = pv->Value(yymax, logTkin); 692 G4double p0 = pv->Value(0.0, logTkin); 693 if(p0 <= 0.0) { DataCorrupted(ZDATPAIR[iz], logTkin); } 694 else { res = pv->FindLinearX((pmin + rand*(pmax - pmin))/p0, logTkin); } 695 } else { 696 DataCorrupted(ZDATPAIR[iz], logTkin); 697 } 698 return res; 699 } 700 701 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 702 703 void G4MuPairProductionModel::DataCorrupted(G4int Z, G4double logTkin) const 704 { 705 G4ExceptionDescription ed; 706 ed << "G4ElementData is not properly initialized Z= " << Z 707 << " Ekin(MeV)= " << G4Exp(logTkin) 708 << " IsMasterThread= " << IsMaster() 709 << " Model " << GetName(); 710 G4Exception("G4MuPairProductionModel::()", "em0033", FatalException, ed, ""); 711 } 712 713 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 714 715 void G4MuPairProductionModel::StoreTables() const 716 { 717 for (G4int iz=0; iz<NZDATPAIR; ++iz) { 718 G4int Z = ZDATPAIR[iz]; 719 G4Physics2DVector* pv = fElementData->GetElement2DData(Z); 720 if(nullptr == pv) { 721 DataCorrupted(Z, 1.0); 722 return; 723 } 724 std::ostringstream ss; 725 ss << "mupair/" << particle->GetParticleName() << Z << ".dat"; 726 std::ofstream outfile(ss.str()); 727 pv->Store(outfile); 728 } 729 } 730 731 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 732 733 G4bool G4MuPairProductionModel::RetrieveTables() 734 { 735 for (G4int iz=0; iz<NZDATPAIR; ++iz) { 736 G4double Z = ZDATPAIR[iz]; 737 G4Physics2DVector* pv = new G4Physics2DVector(nbiny+1,nbine+1); 738 std::ostringstream ss; 739 ss << G4EmParameters::Instance()->GetDirLEDATA() << "/mupair/" 740 << particle->GetParticleName() << Z << ".dat"; 741 std::ifstream infile(ss.str(), std::ios::in); 742 if(!pv->Retrieve(infile)) { 743 delete pv; 744 return false; 745 } 746 fElementData->InitialiseForElement(iz, pv); 747 } 748 return true; 749 } 750 751 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 752