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Geant4/processes/electromagnetic/standard/src/G4SauterGavrilaAngularDistribution.cc

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Diff markup

Differences between /processes/electromagnetic/standard/src/G4SauterGavrilaAngularDistribution.cc (Version 11.3.0) and /processes/electromagnetic/standard/src/G4SauterGavrilaAngularDistribution.cc (Version 10.0)


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                                                   >>  26 // $Id: G4SauterGavrilaAngularDistribution.cc 68797 2013-04-05 13:27:11Z gcosmo $
 26 //                                                 27 //
 27 // -------------------------------------------     28 // -------------------------------------------------------------------
 28 //                                                 29 //
 29 // GEANT4 Class file                               30 // GEANT4 Class file
 30 //                                                 31 //
 31 //                                                 32 //
 32 // File name:     G4SauterGavrilaAngularDistri     33 // File name:     G4SauterGavrilaAngularDistribution
 33 //                                                 34 //
 34 // Author:     Vladimir Ivanchenko using Miche     35 // Author:     Vladimir Ivanchenko using Michel Maire algorithm
 35 //             developed for Geant3                36 //             developed for Geant3
 36 //                                                 37 // 
 37 // Creation date: 23 July 2012                     38 // Creation date: 23 July 2012
 38 //                                                 39 //
 39 // Modified:                                   <<  40 //
 40 //   04.05.2017 Marilena Bandieramonte impleme << 
 41 // -------------------------------------------     41 // -------------------------------------------------------------------
 42 //                                                 42 //
 43                                                    43 
 44 #include "G4SauterGavrilaAngularDistribution.h     44 #include "G4SauterGavrilaAngularDistribution.hh"
 45 #include "G4PhysicalConstants.hh"                  45 #include "G4PhysicalConstants.hh"
 46 #include "Randomize.hh"                            46 #include "Randomize.hh"
 47                                                    47 
 48 G4SauterGavrilaAngularDistribution::G4SauterGa     48 G4SauterGavrilaAngularDistribution::G4SauterGavrilaAngularDistribution()
 49   : G4VEmAngularDistribution("SauterGavrila")  <<  49   : G4VEmAngularDistribution("AngularGenSauterGavrila")
 50 {}                                                 50 {}    
 51                                                    51 
 52 G4SauterGavrilaAngularDistribution::~G4SauterG <<  52 G4SauterGavrilaAngularDistribution::~G4SauterGavrilaAngularDistribution() 
 53   = default;                                   <<  53 {}
 54                                                    54 
 55 G4ThreeVector&  G4SauterGavrilaAngularDistribu <<  55 G4ThreeVector& 
                                                   >>  56 G4SauterGavrilaAngularDistribution::SampleDirection(
 56        const G4DynamicParticle* dp, G4double,      57        const G4DynamicParticle* dp, G4double, G4int, const G4Material*)
 57 {                                                  58 {
 58   static const G4double emin = 1*CLHEP::eV;    <<  59   G4double tau = dp->GetKineticEnergy()/electron_mass_c2;
 59   static const G4double emax = 100*CLHEP::MeV; <<  60   static const G4double taulimit = 30.0;
 60                                                    61 
 61   G4double energy = std::max(dp->GetKineticEne <<  62   if (tau > taulimit) {
 62   if (energy > emax) {                         <<  63     fLocalDirection = dp->GetMomentumDirection(); 
 63     fLocalDirection = dp->GetMomentumDirection <<  64     // Bugzilla 1120
                                                   >>  65     // SI on 05/09/2010 as suggested by JG 04/09/10 
 64   } else {                                         66   } else {
 65     // Initial algorithm according Penelope 20 <<  67  
 66     // F.Sauter Ann. Physik 9, 217(1931); 11,  <<  68     G4double invgamma  = 1.0/(tau + 1.0);
 67     // Modified according Penelope 2014 manual <<  69     G4double beta      = std::sqrt(tau*(tau + 2.0))*invgamma;
 68     G4double costheta = 0.0;                   <<  70     G4double b         = 0.5*tau*(tau*tau - 1.0);
 69                                                <<  71     G4double invgamma2 = invgamma*invgamma;
 70     // 1) initialize energy-dependent variable <<  72    
 71     // Variable naming according to Eq. (2.24) <<  73     G4double rndm,term,greject,grejsup,costeta,sint2;
 72     // (pag. 44)                               <<  74     if (tau < 1.) { grejsup = (1.+b-beta*b)/invgamma2; }
 73     G4double tau = energy/electron_mass_c2;    <<  75     else          { grejsup = (1.+b+beta*b)/invgamma2; }
 74     G4double gamma = 1.0 + tau;                <<  76 
 75     G4double beta = std::sqrt(tau*(tau + 2.0)) <<  77     do { 
 76                                                <<  78       rndm    = 1 - 2*G4UniformRand();
 77     // ac corresponds to "A" of Eq. (2.31)     <<  79       costeta = (rndm + beta)/(rndm*beta + 1);
 78     //                                         <<  80       term    = invgamma2/(1 + beta*rndm);
 79     G4double ac = (1.0 - beta)/beta;           <<  81       sint2   = (1 - costeta)*(1 + costeta);
 80     G4double a1 = 0.5*beta*gamma*tau*(gamma-2. <<  82       greject = sint2*(1 + b*term)/(term*term);
 81     G4double a2 = ac + 2.0;                    <<  83 
 82     // gtmax = maximum of the rejection functi <<  84     } while(greject < G4UniformRand()*grejsup);
 83     // obtained for tsam=0                     <<  85        
 84     G4double gtmax = 2.0*(a1 + 1.0/ac);        <<  86     G4double sinteta = std::sqrt(sint2);
 85                                                <<  87     G4double phi  = CLHEP::twopi*G4UniformRand(); 
 86     G4double tsam = 0.0;                       <<  88 
 87     G4double gtr  = 0.0;                       <<  89     fLocalDirection.set(sinteta*std::cos(phi), sinteta*std::sin(phi), costeta);
 88                                                << 
 89     //2) sampling. Eq. (2.31) of Penelope Manu << 
 90     // tsam = 1-std::cos(theta)                << 
 91     // gtr = rejection function according to E << 
 92     do{                                        << 
 93       G4double rand = G4UniformRand();         << 
 94       tsam = 2.0*ac * (2.0*rand + a2*std::sqrt << 
 95       gtr = (2.0 - tsam) * (a1 + 1.0/(ac+tsam) << 
 96       // Loop checking, 03-Aug-2015, Vladimir  << 
 97     } while(G4UniformRand()*gtmax > gtr);      << 
 98                                                << 
 99     costheta = 1.0 - tsam;                     << 
100                                                << 
101     G4double sint = std::sqrt(tsam*(2.0 - tsam << 
102     G4double phi  = CLHEP::twopi*G4UniformRand << 
103                                                << 
104     fLocalDirection.set(sint*std::cos(phi), si << 
105     fLocalDirection.rotateUz(dp->GetMomentumDi     90     fLocalDirection.rotateUz(dp->GetMomentumDirection());
106   }                                                91   }
107   return fLocalDirection;                          92   return fLocalDirection;
108 }                                                  93 }
109                                                    94 
110 void G4SauterGavrilaAngularDistribution::Print     95 void G4SauterGavrilaAngularDistribution::PrintGeneratorInformation() const
111 {                                                  96 {
112   G4cout << "\n" << G4endl;                        97   G4cout << "\n" << G4endl;
113   G4cout << "Non-polarized photoelectric effec     98   G4cout << "Non-polarized photoelectric effect angular generator." << G4endl;
114   G4cout << "The Sauter-Gavrila distribution f     99   G4cout << "The Sauter-Gavrila distribution for the K-shell is used."<<G4endl;
115   G4cout << "Originally developed by M.Maire f    100   G4cout << "Originally developed by M.Maire for Geant3" 
116          << G4endl;                            << 101    << G4endl;
117 }                                                 102 } 
118                                                << 
119                                                   103