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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: G4DynamicParticleFluctuation 33 // 34 // Author: V. Ivanchenko 35 // 36 // Creation date: 23.08.2024 37 // 38 // ------------------------------------------------------------------- 39 40 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 41 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 42 43 #include "G4DynamicParticleFluctuation.hh" 44 #include "G4PhysicalConstants.hh" 45 #include "G4SystemOfUnits.hh" 46 #include "Randomize.hh" 47 #include "G4Poisson.hh" 48 #include "G4Material.hh" 49 #include "G4MaterialCutsCouple.hh" 50 #include "G4DynamicParticle.hh" 51 #include "G4Log.hh" 52 53 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 54 55 G4DynamicParticleFluctuation::G4DynamicParticleFluctuation(const G4String& nam) 56 : G4UniversalFluctuation(nam) 57 {} 58 59 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 60 61 void G4DynamicParticleFluctuation::InitialiseLocal(const G4DynamicParticle* part) 62 { 63 particleMass = part->GetMass(); 64 const G4double q = part->GetCharge()/CLHEP::eplus; 65 66 // Derived quantities 67 m_Inv_particleMass = 1.0 / particleMass; 68 m_massrate = CLHEP::electron_mass_c2 * m_Inv_particleMass; 69 chargeSquare = q*q; 70 } 71 72 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 73 74 G4double G4DynamicParticleFluctuation::SampleFluctuations( 75 const G4MaterialCutsCouple* couple, 76 const G4DynamicParticle* dp, 77 const G4double tcut, 78 const G4double tmax, 79 const G4double length, 80 const G4double averageLoss) 81 { 82 // Calculate actual loss from the mean loss. 83 // The model used to get the fluctuations is essentially the same 84 // as in Glandz in Geant3 (Cern program library W5013, phys332). 85 // L. Urban et al. NIM A362, p.416 (1995) and Geant4 Physics Reference Manual 86 87 // shortcut for very small loss or from a step nearly equal to the range 88 // (out of validity of the model) 89 // 90 if (averageLoss < minLoss) { return averageLoss; } 91 meanLoss = averageLoss; 92 const G4double tkin = dp->GetKineticEnergy(); 93 //G4cout<< "Emean= "<< meanLoss<< " tmax= "<< tmax<< " L= "<<length<<G4endl; 94 95 CLHEP::HepRandomEngine* rndmEngineF = G4Random::getTheEngine(); 96 97 InitialiseLocal(dp); 98 const G4double gam = tkin * m_Inv_particleMass + 1.0; 99 const G4double gam2 = gam*gam; 100 const G4double beta = dp->GetBeta(); 101 const G4double beta2 = beta*beta; 102 103 G4double loss(0.), siga(0.); 104 105 const G4Material* material = couple->GetMaterial(); 106 107 // Gaussian regime 108 // for heavy particles only and conditions 109 // for Gauusian fluct. has been changed 110 // 111 if (particleMass > CLHEP::electron_mass_c2 && 112 meanLoss >= minNumberInteractionsBohr*tcut && tmax <= 2.*tcut) { 113 114 siga = std::sqrt((tmax/beta2 - 0.5*tcut)*CLHEP::twopi_mc2_rcl2* 115 length*chargeSquare*material->GetElectronDensity()); 116 const G4double sn = meanLoss/siga; 117 118 // thick target case 119 if (sn >= 2.0) { 120 121 const G4double twomeanLoss = meanLoss + meanLoss; 122 do { 123 loss = G4RandGauss::shoot(rndmEngineF, meanLoss, siga); 124 // Loop checking, 03-Aug-2015, Vladimir Ivanchenko 125 } while (0.0 > loss || twomeanLoss < loss); 126 127 // Gamma distribution 128 } else { 129 130 const G4double neff = sn*sn; 131 loss = meanLoss*G4RandGamma::shoot(rndmEngineF, neff, 1.0)/neff; 132 } 133 //G4cout << "Gauss: " << loss << G4endl; 134 return loss; 135 } 136 137 auto ioni = material->GetIonisation(); 138 e0 = ioni->GetEnergy0fluct(); 139 140 // very small step or low-density material 141 if(tcut <= e0) { return meanLoss; } 142 143 ipotFluct = ioni->GetMeanExcitationEnergy(); 144 ipotLogFluct = ioni->GetLogMeanExcEnergy(); 145 146 // width correction for small cuts 147 const G4double scaling = std::min(1.+0.5*CLHEP::keV/tcut, 1.50); 148 meanLoss /= scaling; 149 150 w2 = (tcut > ipotFluct) ? 151 G4Log(2.*CLHEP::electron_mass_c2*beta2*gam2) - beta2 : 0.0; 152 return SampleGlandz(rndmEngineF, material, tcut)*scaling; 153 } 154 155 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 156 157 158 G4double G4DynamicParticleFluctuation::Dispersion( 159 const G4Material* material, 160 const G4DynamicParticle* dp, 161 const G4double tcut, 162 const G4double tmax, 163 const G4double length) 164 { 165 InitialiseLocal(dp); 166 const G4double beta = dp->GetBeta(); 167 return (tmax/(beta*beta) - 0.5*tcut) * CLHEP::twopi_mc2_rcl2 * length 168 * material->GetElectronDensity() * chargeSquare; 169 } 170 171 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 172