// // ******************************************************************** // * License and Disclaimer * // * * // * The Geant4 software is copyright of the Copyright Holders of * // * the Geant4 Collaboration. It is provided under the terms and * // * conditions of the Geant4 Software License, included in the file * // * LICENSE and available at http://cern.ch/geant4/license . These * // * include a list of copyright holders. * // * * // * Neither the authors of this software system, nor their employing * // * institutes,nor the agencies providing financial support for this * // * work make any representation or warranty, express or implied, * // * regarding this software system or assume any liability for its * // * use. Please see the license in the file LICENSE and URL above * // * for the full disclaimer and the limitation of liability. * // * * // * This code implementation is the result of the scientific and * // * technical work of the GEANT4 collaboration. * // * By using, copying, modifying or distributing the software (or * // * any work based on the software) you agree to acknowledge its * // * use in resulting scientific publications, and indicate your * // * acceptance of all terms of the Geant4 Software license. * // ******************************************************************** // // // $Id: G4DNARutherfordTotalCrossSectionPolicy.icc,v 1.2 2006/06/29 19:35:21 gunter Exp $ // GEANT4 tag $Name: geant4-08-02 $ // #ifdef G4DNARUTHERFORDTOTALCROSSSECTIONPOLICY_HH #include "G4Electron.hh" template const G4ParticleDefinition *G4DNARutherfordTotalCrossSectionPolicy :: IncomingParticleDefinition(void) const { return G4Electron::Electron(); } template G4double G4DNARutherfordTotalCrossSectionPolicy :: 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 G4double G4DNARutherfordTotalCrossSectionPolicy :: 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(z*(z+1))*length*length; } template G4double G4DNARutherfordTotalCrossSectionPolicy :: 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(z), 2./3.); k/=electron_mass_c2; G4double denominator; denominator=k*(2+k); return numerator/denominator; } #endif /* G4DNARUTHERFORDTOTALCROSSSECTIONPOLICY_HH */