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geant4/source/processes/electromagnetic/lowenergy/include/G4DNARutherfordTotalCrossSectionPolicy.icc
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//
// ********************************************************************
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//
// $Id: G4DNARutherfordTotalCrossSectionPolicy.icc,v 1.2 2006/06/29 19:35:21 gunter Exp $
// GEANT4 tag $Name: geant4-08-01 $
//
#ifdef G4DNARUTHERFORDTOTALCROSSSECTIONPOLICY_HH
#include "G4Electron.hh"
template <typename EnergyLimitsPolicy>
const G4ParticleDefinition *G4DNARutherfordTotalCrossSectionPolicy<EnergyLimitsPolicy> :: IncomingParticleDefinition(void) const
{
return G4Electron::Electron();
}
template <typename EnergyLimitsPolicy>
G4double G4DNARutherfordTotalCrossSectionPolicy<EnergyLimitsPolicy> :: TotalCrossSection(G4double k, G4int z) const
{
// pi * sigma_Ruth(K)
// sigma_el(K) = --------------------
// n(K) * (n(K) + 1)
//
// Where K is the electron non-relativistic kinetic energy
// Cross section per water molecule
if (k < EnergyLimitsPolicy::lowEnergyLimit)
{
if (EnergyLimitsPolicy::zeroBelowLowEnergyLimit)
return 0;
k=EnergyLimitsPolicy::lowEnergyLimit;
}
else if (k > EnergyLimitsPolicy::highEnergyLimit)
{
if (EnergyLimitsPolicy::zeroAboveHighEnergyLimit)
return 0;
k=EnergyLimitsPolicy::highEnergyLimit;
}
G4double n=ScreeningFactor(k,z);
return (pi * RutherfordTotalCrossSection(k, z))/(n*(n+1.));
}
template <typename EnergyLimitsPolicy>
G4double G4DNARutherfordTotalCrossSectionPolicy<EnergyLimitsPolicy> :: RutherfordTotalCrossSection(G4double k, G4int z) const
{
// e^4 / K + m_e c^2 \^2
// sigma_Ruth(K) = Z (Z+1) -------------------- | --------------------- |
// (4 pi epsilon_0)^2 \ K * (K + 2 m_e c^2) /
//
// Where K is the electron non-relativistic kinetic energy
//
// Nucl. Instr. Meth. 155 (1978) 145-156
G4double length;
length=(e_squared*(k+electron_mass_c2))/(4*pi*epsilon0*k*(k+2*electron_mass_c2));
return static_cast<G4double>(z*(z+1))*length*length;
}
template <typename EnergyLimitsPolicy>
G4double G4DNARutherfordTotalCrossSectionPolicy<EnergyLimitsPolicy> :: ScreeningFactor(G4double k, G4int z) const
{
//
// alpha_1 + beta_1 ln(K/eV) constK Z^(2/3)
// n(T) = -------------------------- -----------------
// K/(m_e c^2) 2 + K/(m_e c^2)
//
// Where K is the electron non-relativistic kinetic energy
//
// n(T) > 0 for T < ~ 400 MeV
//
// Nucl. Instr. Meth. 155 (1978) 145-156
const G4double alpha_1(1.64);
const G4double beta_1(-0.0825);
const G4double constK(1.7E-5);
G4double numerator;
numerator=(alpha_1+beta_1*std::log(k/eV))*constK*std::pow(static_cast<double>(z), 2./3.);
k/=electron_mass_c2;
G4double denominator;
denominator=k*(2+k);
return numerator/denominator;
}
#endif /* G4DNARUTHERFORDTOTALCROSSSECTIONPOLICY_HH */