// // ******************************************************************** // * 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: G4LindhardPartition.cc,v 1.1 2009/11/05 11:42:24 vnivanch Exp $ // GEANT4 tag $Name: geant4-09-03-cand-01 $ // /* * G4LindhardPartition.cc * * Created by Marcus Mendenhall on 1/14/08. * Copyright 2008 Vanderbilt University, Nashville, TN, USA. All rights reserved. * */ #include "G4LindhardPartition.hh" #include "G4Material.hh" #include "G4Element.hh" /* for a first cut, we will compute NIEL from a Lindhard-Robinson partition based on the most abundant element in the material. this is from IEEE Trans. Nucl Science Vol. 48 No.1 February 2001 page 162++ Insoo Jun, "Effects of Secondary Particles on the Total Dose..." and, by reference, Lindhard, Nielsen, Scharff & Thompson, "Integral Equations Governing Radiation Efects...", Mat. Fys. Medd. Dan. Vid. Selsk. vol 33 #10, pp1-42, 1963 and Robinson, "The dependence of radiation effects on primary recoil energy", in Proc. Int. Conf. Radiation-Induced Voids in Metal, Albany, NY 1972 pp. 397-439 def lindhard_robinson(z1, a1, z2, a2, ke): el=30.724*z1*z2*math.sqrt(z1**0.6667+z2**0.6667)*(a1+a2)/a2 fl=0.0793*z1**0.6667*math.sqrt(z2)*(a1+a2)**1.5/ ((z1**0.6667+z2**0.6667)**0.75*a1**1.5*math.sqrt(a2)) eps=ke*(1.0/el) return 1.0/(1+fl*(3.4008*eps**0.16667+0.40244*eps**0.75+eps)) */ G4LindhardRobinsonPartition::G4LindhardRobinsonPartition() { max_z = 120; for(size_t i=1; iGetNumberOfElements(); const G4double *atomDensities=material->GetVecNbOfAtomsPerVolume(); G4double maxdens=0.0; size_t maxindex=0; for (size_t k=0 ; k < nMatElements ; k++ ) { if(atomDensities[k] > maxdens) { maxdens=atomDensities[k]; maxindex=k; } } const G4Element *element=material->GetElement(maxindex); G4int z2=G4int(element->GetZ()); G4double a2=element->GetA()/(Avogadro*amu); G4double zpow=z23[z1]+z23[z2]; G4double asum=a1+a2; G4double el=30.724*z1*z2*std::sqrt(zpow)*asum/a2; G4double fl=0.0793*z23[z1]*std::sqrt(z2*asum*asum*asum/(a1*a1*a1*a2))/std::pow(zpow, 0.75); G4double eps=(energy/eV)*(1.0/el); return 1.0/(1+fl*(3.4008*std::pow(eps, 0.16667)+0.40244*std::pow(eps, 0.75)+eps)); }