Geant4-11
G4PenelopeCrossSection.hh
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25//
26//
27// Author: Luciano Pandola
28//
29// History:
30// -----------
31// 18 Mar 2010 L. Pandola 1st implementation.
32// 09 Mar 2012 L. Pandola Add public method (and machinery) to return
33// the absolute and the normalized shell cross
34// sections independently.
35//
36// -------------------------------------------------------------------
37//
38// Class description:
39// This class is a container for cross sections and transport momenta
40// calculated by Penelope models (ionisation, bremsstrahlung). It stores
41// PhysicsTables/PhysicsVectors of
42// a) the "hard quantities" (above the threshold), 0-th order (cross section)
43// 1-st order (= stopping XS), 2-nd order (= straggling XS)
44// b) the "soft quantities" (below threshold), 0-th order (cross section)
45// 1-st order (= stopping XS), 2-nd order (= straggling XS)
46// c) total hard cross sections for individual oscillators
47// vs. energy. Two versions are available, one with normalized values
48// (good for sampling) and one with absolute values.
49//
50// The interface *always* uses energy and cross sections, while internally
51// log(energy) and log(XS) are used.
52//
53// One instance per each cut-material couple should be created by the
54// calling class.
55//
56// Public method to retrieve hard cross section, soft stopping power,
57// total cross section and hard shell cross sections.
58//
59// Notice: all quantities stored here are *per molecule*
60//
61// -------------------------------------------------------------------
62
63#ifndef G4PENELOPECROSSSECTION_HH
64#define G4PENELOPECROSSSECTION_HH 1
65
66#include "globals.hh"
67
68class G4PhysicsTable;
69class G4DataVector;
70
72{
73
74public:
75 //constructor: one has to give the number of points in each PhysicsVector
76 //(= dimension of the energy grid) and the number of shells (0 is the
77 //default).
78 explicit G4PenelopeCrossSection(size_t nOfEnergyPoints,size_t nOfShells=0);
79 //
81
89 G4double GetShellCrossSection(size_t shellID,G4double energy) const;
92
93 size_t GetNumberOfShells() const {return fNumberOfShells;};
94
98 void AddCrossSectionPoint(size_t binNumber,
100 G4double XH2,
101 G4double XS0, G4double XS1, G4double XS2);
102 void AddShellCrossSectionPoint(size_t binNumber,
103 size_t shellID,G4double energy,G4double xs);
105
108
109private:
110 //all tables are log. XS vs. log E
111
112 //XS0, XS1, XS2 in Penelope nomenclature
114
115 //XH0, XH1, XH2 in Penelope nomenclature
117
118 //XS for individual shells
121
125};
126
127#endif
128
double G4double
Definition: G4Types.hh:83
bool G4bool
Definition: G4Types.hh:86
void AddShellCrossSectionPoint(size_t binNumber, size_t shellID, G4double energy, G4double xs)
G4PhysicsTable * fShellNormalizedCrossSections
G4double GetTotalCrossSection(G4double energy) const
Returns total cross section at the given energy.
G4double GetSoftStoppingPower(G4double energy) const
Returns the total stopping power due to soft collisions.
G4double GetShellCrossSection(size_t shellID, G4double energy) const
Returns the hard cross section for the given shell (per molecule)
G4PhysicsTable * fShellCrossSections
G4double GetHardCrossSection(G4double energy) const
Returns hard cross section at the given energy.
G4PenelopeCrossSection(const G4PenelopeCrossSection &)=delete
G4double GetNormalizedShellCrossSection(size_t shellID, G4double energy) const
Returns the hard cross section for the given shell (normalized to 1)
void AddCrossSectionPoint(size_t binNumber, G4double energy, G4double XH0, G4double XH1, G4double XH2, G4double XS0, G4double XS1, G4double XS2)
G4PenelopeCrossSection & operator=(const G4PenelopeCrossSection &right)=delete
G4PenelopeCrossSection(size_t nOfEnergyPoints, size_t nOfShells=0)
G4double energy(const ThreeVector &p, const G4double m)