Geant4 Cross Reference

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

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 27 // -------------------------------------------------------------------
 28 //
 29 // GEANT4 Class file
 30 //
 31 //
 32 // File name:     G4SauterGavrilaAngularDistribution
 33 //
 34 // Author:     Vladimir Ivanchenko using Michel Maire algorithm
 35 //             developed for Geant3
 36 // 
 37 // Creation date: 23 July 2012
 38 //
 39 // Modified: 
 40 //   04.05.2017 Marilena Bandieramonte implemented Penelope 2014 algorithm
 41 // -------------------------------------------------------------------
 42 //
 43 
 44 #include "G4SauterGavrilaAngularDistribution.hh"
 45 #include "G4PhysicalConstants.hh"
 46 #include "Randomize.hh"
 47 
 48 G4SauterGavrilaAngularDistribution::G4SauterGavrilaAngularDistribution()
 49   : G4VEmAngularDistribution("SauterGavrila")
 50 {}    
 51 
 52 G4SauterGavrilaAngularDistribution::~G4SauterGavrilaAngularDistribution()
 53   = default;
 54 
 55 G4ThreeVector&  G4SauterGavrilaAngularDistribution::SampleDirection( 
 56        const G4DynamicParticle* dp, G4double, G4int, const G4Material*)
 57 {
 58   static const G4double emin = 1*CLHEP::eV;
 59   static const G4double emax = 100*CLHEP::MeV;
 60 
 61   G4double energy = std::max(dp->GetKineticEnergy(), emin);
 62   if (energy > emax) {
 63     fLocalDirection = dp->GetMomentumDirection();
 64   } else {
 65     // Initial algorithm according Penelope 2008 manual and 
 66     // F.Sauter Ann. Physik 9, 217(1931); 11, 454(1931).
 67     // Modified according Penelope 2014 manual 
 68     G4double costheta = 0.0;
 69 
 70     // 1) initialize energy-dependent variables
 71     // Variable naming according to Eq. (2.24) of Penelope Manual
 72     // (pag. 44)
 73     G4double tau = energy/electron_mass_c2;
 74     G4double gamma = 1.0 + tau;
 75     G4double beta = std::sqrt(tau*(tau + 2.0))/gamma;
 76     
 77     // ac corresponds to "A" of Eq. (2.31)
 78     //
 79     G4double ac = (1.0 - beta)/beta;
 80     G4double a1 = 0.5*beta*gamma*tau*(gamma-2.0);
 81     G4double a2 = ac + 2.0;
 82     // gtmax = maximum of the rejection function according to Eq. (2.28), 
 83     // obtained for tsam=0
 84     G4double gtmax = 2.0*(a1 + 1.0/ac);
 85     
 86     G4double tsam = 0.0;
 87     G4double gtr  = 0.0;
 88     
 89     //2) sampling. Eq. (2.31) of Penelope Manual
 90     // tsam = 1-std::cos(theta)
 91     // gtr = rejection function according to Eq. (2.28)
 92     do{
 93       G4double rand = G4UniformRand();
 94       tsam = 2.0*ac * (2.0*rand + a2*std::sqrt(rand)) / (a2*a2 - 4.0*rand);
 95       gtr = (2.0 - tsam) * (a1 + 1.0/(ac+tsam));
 96       // Loop checking, 03-Aug-2015, Vladimir Ivanchenko
 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), sint*std::sin(phi), costheta);
105     fLocalDirection.rotateUz(dp->GetMomentumDirection());
106   }
107   return fLocalDirection;
108 }
109 
110 void G4SauterGavrilaAngularDistribution::PrintGeneratorInformation() const
111 {
112   G4cout << "\n" << G4endl;
113   G4cout << "Non-polarized photoelectric effect angular generator." << G4endl;
114   G4cout << "The Sauter-Gavrila distribution for the K-shell is used."<<G4endl;
115   G4cout << "Originally developed by M.Maire for Geant3" 
116          << G4endl;
117 } 
118 
119