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G4LindhardPartition.cc
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26 /*
27  * \file electromagnetic/TestEm7/src/G4LindhardPartition.cc
28  * \brief Implementation of the G4LindhardPartition class
29  *
30  * Created by Marcus Mendenhall on 1/14/08.
31  * 2008 Vanderbilt University, Nashville, TN, USA.
32  *
33  */
34 
35 //
36 // $Id: G4LindhardPartition.cc 68263 2013-03-20 10:16:46Z maire $
37 
38 #include "G4LindhardPartition.hh"
39 #include "G4Material.hh"
40 #include "G4Element.hh"
41 #include "G4PhysicalConstants.hh"
42 #include "G4SystemOfUnits.hh"
43 
44 /*
45 for a first cut, we will compute NIEL from a Lindhard-Robinson partition
46 based on the most abundant element in the material.
47 
48 this is from IEEE Trans. Nucl Science Vol. 48 No.1 February 2001 page 162++
49 Insoo Jun, "Effects of Secondary Particles on the Total Dose..."
50 and, by reference,
51 Lindhard, Nielsen, Scharff & Thompson,
52 "Integral Equations Governing Radiation Efects...",
53 Mat. Fys. Medd. Dan. Vid. Selsk. vol 33 #10, pp1-42, 1963
54 and
55 Robinson, "The dependence of radiation effects on primary recoil energy",
56 in Proc. Int. Conf. Radiation-Induced Voids in Metal,
57 Albany, NY 1972 pp. 397-439
58 def lindhard_robinson(z1, a1, z2, a2, ke):
59 el=30.724*z1*z2*math.sqrt(z1**0.6667+z2**0.6667)*(a1+a2)/a2
60 fl=0.0793*z1**0.6667*math.sqrt(z2)*(a1+a2)**1.5/
61 ((z1**0.6667+z2**0.6667)**0.75*a1**1.5*math.sqrt(a2))
62 eps=ke*(1.0/el)
63 return 1.0/(1+fl*(3.4008*eps**0.16667+0.40244*eps**0.75+eps))
64 */
65 
67 {
68  max_z = 120;
69  for(size_t i=1; i<max_z; i++) {z23[i]=std::pow((G4double)i, 2./3.);}
70 }
71 
73  G4int z1, G4double a1, const G4Material *material, G4double energy) const
74 {
75  size_t nMatElements = material->GetNumberOfElements();
76 
77  const G4double *atomDensities=material->GetVecNbOfAtomsPerVolume();
78  G4double maxdens=0.0;
79  size_t maxindex=0;
80  for (size_t k=0 ; k < nMatElements ; k++ )
81  {
82  if(atomDensities[k] > maxdens) {
83  maxdens=atomDensities[k];
84  maxindex=k;
85  }
86  }
87  const G4Element *element=material->GetElement(maxindex);
88 
89  G4int z2=G4int(element->GetZ());
90 
91  G4double a2=element->GetA()/(Avogadro*amu);
92 
93  G4double zpow=z23[z1]+z23[z2];
94  G4double asum=a1+a2;
95 
96  G4double el=30.724*z1*z2*std::sqrt(zpow)*asum/a2;
97  G4double fl=0.0793*z23[z1]*std::sqrt(z2*asum*asum*asum/(a1*a1*a1*a2))
98  /std::pow(zpow, 0.75);
99  G4double eps=(energy/eV)*(1.0/el);
100 
101  return
102  1.0/(1+fl*(3.4008*std::pow(eps, 0.16667)+0.40244*std::pow(eps, 0.75)+eps));
103 }
104 
virtual G4double PartitionNIEL(G4int z1, G4double a1, const G4Material *material, G4double energy) const
G4double GetZ() const
Definition: G4Element.hh:131
const G4Element * GetElement(G4int iel) const
Definition: G4Material.hh:200
G4double GetA() const
Definition: G4Element.hh:138
int G4int
Definition: G4Types.hh:78
float Avogadro
Definition: hepunit.py:253
string material
Definition: eplot.py:19
const G4double * GetVecNbOfAtomsPerVolume() const
Definition: G4Material.hh:204
double precision function energy(A, Z)
Definition: dpm25nuc6.f:4106
size_t GetNumberOfElements() const
Definition: G4Material.hh:184
double G4double
Definition: G4Types.hh:76