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geant4/source/processes/electromagnetic/standard/include/G4ScreeningMottCrossSection.hh
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// G4ScreeningMottCrossSection.hh
//-------------------------------------------------------------------
//
// GEANT4 Class header file
//
// File name: G4ScreeningMottCrossSection
//
// Author: Cristina Consolandi
//
// Creation date: 20.10.2011
//
// Modifications:
//
// Class Description:
// Computation of electron Coulomb Scattering Cross Section.
// Suitable for high energy electrons and light target materials.
//
// Reference:
// M.J. Boschini et al.
// "Non Ionizing Energy Loss induced by Electrons in the Space Environment"
// Proc. of the 13th Int. Conf. on Particle Physics and Advanced Technology
// (13th ICPPAT, Como 3-7/10/2011), World Scientific (Singapore).
// Available at: http://arxiv.org/abs/1111.4042v4
//
// 1) Mott Differential Cross Section Approximation:
// For Target material up to Z=92 (U):
// As described in http://arxiv.org/abs/1111.4042v4
// par. 2.1 , eq. (16)-(17)
// Else (Z>92):
// W. A. McKinley and H. Fashbach, Phys. Rev. 74, (1948) 1759.
// 2) Screening coefficient:
// vomn G. Moliere, Z. Naturforsh A2 (1947), 133-145; A3 (1948), 78.
// 3) Nuclear Form Factor:
// A.V. Butkevich et al. Nucl. Instr. Meth. A488 (2002), 282-294.
//
// -----------------------------------------------------------------------------
//
#ifndef G4ScreeningMottCrossSection_h
#define G4ScreeningMottCrossSection_h 1
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
#include "globals.hh"
#include "G4ParticleDefinition.hh"
#include <vector>
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
static const G4int DIMMOTT = 750;
class G4NistManager;
class G4Pow;
class G4ScreeningMottCrossSection
{
public:
explicit G4ScreeningMottCrossSection();
~G4ScreeningMottCrossSection();
void Initialise(const G4ParticleDefinition*, G4double cosThetaLim);
void SetupKinematic(G4double kinEnergy, G4int Z);
G4double NuclearCrossSection(G4int form, G4int fast);
G4double GetScatteringAngle(G4int form, G4int fast);
G4double RatioMottRutherford(G4double tet);
G4double RatioMottRutherfordCosT(G4double sin2t2);
G4double McFcorrection(G4double sin2t2);
inline void SetupParticle(const G4ParticleDefinition*);
G4ScreeningMottCrossSection & operator=
(const G4ScreeningMottCrossSection &right) = delete;
G4ScreeningMottCrossSection(const G4ScreeningMottCrossSection&) = delete;
private:
G4double ComputeAngle(G4int idx, G4double& rand);
G4double FormFactor2ExpHof(G4double sin2t2);
G4double FormFactor2Gauss(G4double sin2t2);
G4double FormFactor2UniformHelm(G4double sin2t2);
G4double DifferentialXSection(G4int idx, G4int form);
G4double GetTransitionRandom();
G4NistManager* fNistManager;
G4Pow* fG4pow;
const G4ParticleDefinition* particle;
G4double fTotalCross;
//cost - min - max
G4double cosThetaMin;// def 1.0
G4double cosThetaMax;// def -1.0
G4double cosTetMinNuc;
G4double cosTetMaxNuc;
//energy cut
G4double ecut;
G4double etag;
G4double spin;
G4double mass;
//lab of incedent particle
G4double tkinLab;
G4double momLab2;
G4double invbetaLab2;
//relative system with nucleus
G4double mu_rel;
G4double tkin;
G4double mom2;
G4double invbeta2;
G4double beta;
G4double gamma;
//constants
G4double alpha;
G4double htc2;
G4double e2;
// target nucleus
G4double targetMass;
G4double As;
G4int targetZ;
G4int targetA;
// working array
std::vector<G4double> cross;
};
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
inline
void G4ScreeningMottCrossSection::SetupParticle(const G4ParticleDefinition* p)
{
particle = p;
mass = particle->GetPDGMass();
spin = particle->GetPDGSpin();
if(0.0 != spin) { spin = 0.5; }
tkin = 0.0;
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
#endif