source: trunk/source/processes/electromagnetic/lowenergy/include/G4PenelopeCrossSection.hh

Last change on this file was 1350, checked in by garnier, 15 years ago

update to last version 4.9.4

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1//
2// ********************************************************************
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14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
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17// * *
18// * This code implementation is the result of the scientific and *
19// * technical work of the GEANT4 collaboration. *
20// * By using, copying, modifying or distributing the software (or *
21// * any work based on the software) you agree to acknowledge its *
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24// ********************************************************************
25//
26// $Id: G4PenelopeCrossSection.hh,v 1.1 2010/07/26 09:56:42 pandola Exp $
27// GEANT4 tag $Name: geant4-09-04-ref-00 $
28//
29// Author: Luciano Pandola
30//
31// History:
32// -----------
33// 18 Mar 2010 L. Pandola 1st implementation.
34//
35// -------------------------------------------------------------------
36//
37// Class description:
38// This class is a container for cross sections and transport momenta
39// calculated by Penelope models (ionisation, bremsstrahlung). It stores
40// PhysicsTables/PhysicsVectors of
41// a) the "hard quantities" (above the threshold), 0-th order (cross section)
42// 1-st order (= stopping XS), 2-nd order (= straggling XS)
43// b) the "soft quantities" (below threshold), 0-th order (cross section)
44// 1-st order (= stopping XS), 2-nd order (= straggling XS)
45// c) total hard cross sections for individual oscillators
46// vs. energy.
47//
48// The interface *always* uses energy and cross sections, while internally
49// log(energy) and log(XS) are used.
50//
51// One instance per each cut-material couple should be created by the
52// calling class.
53//
54// Public method to retrieve hard cross section, soft stopping power,
55// total cross section and hard shell cross sections.
56//
57// The method NormalizeShellCrossSections() normalizes the
58// shell cross sections by retrieving the total hard cross section.
59// Used for sampling.
60//
61// Notice: all quantities stored here are *per molecule*
62//
63// -------------------------------------------------------------------
64
65#ifndef G4PENELOPECROSSSECTION_HH
66#define G4PENELOPECROSSSECTION_HH 1
67
68#include "globals.hh"
69
70class G4PhysicsTable;
71class G4DataVector;
72
73class G4PenelopeCrossSection
74{
75
76public:
77 //constructor: one has to give the number of points in each PhysicsVector
78 //(= dimension of the energy grid) and the number of shells (0 is the
79 //default).
80 G4PenelopeCrossSection(size_t nOfEnergyPoints,size_t nOfShells=0);
81 //
82 ~G4PenelopeCrossSection();
83
84 G4double GetTotalCrossSection(G4double energy);
85 G4double GetHardCrossSection(G4double energy);
86 G4double GetSoftStoppingPower(G4double energy);
87 G4double GetShellCrossSection(size_t shellID,G4double energy);
88
89 size_t GetNumberOfShells(){return numberOfShells;};
90
91 void AddCrossSectionPoint(size_t binNumber,
92 G4double energy,G4double XH0, G4double XH1,
93 G4double XH2,
94 G4double XS0, G4double XS1, G4double XS2);
95
96 void AddShellCrossSectionPoint(size_t binNumber,
97 size_t shellID,G4double energy,G4double xs);
98
99 void NormalizeShellCrossSections();
100
101private:
102 G4PenelopeCrossSection & operator=(const G4PenelopeCrossSection &right);
103 G4PenelopeCrossSection(const G4PenelopeCrossSection&);
104
105 G4bool isNormalized;
106
107 size_t numberOfEnergyPoints;
108 size_t numberOfShells;
109
110 //all tables are log. XS vs. log E
111
112 //XS0, XS1, XS2 in Penelope nomenclature
113 G4PhysicsTable* softCrossSections;
114
115 //XH0, XH1, XH2 in Penelope nomenclature
116 G4PhysicsTable* hardCrossSections;
117
118 //XS for individual shells
119 G4PhysicsTable* shellCrossSections;
120
121};
122
123#endif
124
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