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geant4_9_6_p02
source
processes
electromagnetic
lowenergy
include
G4AtomicTransitionManager.hh
Go to the documentation of this file.
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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//
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// $Id: G4AtomicTransitionManager.hh,v 1.2 ????
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// GEANT4 tag $Name: not supported by cvs2svn $
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//
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// Authors: Elena Guardincerri (Elena.Guardincerri@ge.infn.it)
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// Alfonso Mantero (Alfonso.Mantero@ge.infn.it)
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//
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// History:
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// -----------
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//
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// 16 Sept 2001 EG Modified according to a design iteration in the
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// LowEnergy category
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//
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// -------------------------------------------------------------------
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// Class description:
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// Low Energy Electromagnetic Physics: create or fills and manages G4AtomicShell,
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// G4FluoTransition, G4AugerTransition objects.
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// Further documentation available from http://www.ge.infn.it/geant4/lowE
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// -------------------------------------------------------------------
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#ifndef G4AtomicTransitionManager_h
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#define G4AtomicTransitionManager_h 1
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#include "
G4ShellData.hh
"
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#include "
G4FluoData.hh
"
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#include "
G4AugerData.hh
"
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#include "
G4FluoTransition.hh
"
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#include "
G4AtomicShell.hh
"
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// #include "g4std/map"
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#include <vector>
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#include "
globals.hh
"
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// This class is a singleton
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class
G4AtomicTransitionManager
{
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public
:
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// The only way to get an instance of this class is to call the
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// function Instance()
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static
G4AtomicTransitionManager
*
Instance
();
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// Z is the atomic number of the element, shellIndex is the
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// index (in EADL) of the shell
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G4AtomicShell
*
Shell
(
G4int
Z
,
size_t
shellIndex)
const
;
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// Z is the atomic number of the element, shellIndex is the
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// index (in EADL) of the final shell for the transition
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// This function gives, upon Z and the Index of the initial shell where te vacancy is,
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// the radiative transition that can happen (originating shell, energy, probability)
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const
G4FluoTransition
*
ReachableShell
(
G4int
Z,
size_t
shellIndex)
const
;
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// This function gives, upon Z and the Index of the initial shell where te vacancy is,
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// the NON-radiative transition that can happen with originating shell for the transition, and the
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// data for the possible auger electrons emitted (originating vacancy, energy amnd probability)
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const
G4AugerTransition
*
ReachableAugerShell
(
G4int
Z,
G4int
shellIndex)
const
;
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// This function returns the number of shells of the element
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// whose atomic number is Z
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G4int
NumberOfShells
(
G4int
Z)
const
;
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// This function returns the number of those shells of the element
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// whose atomic number is Z which are reachable through a radiative
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// transition
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// This function returns the number of possible radiative transitions for the atom with atomic number Z
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// i.e. the number of shell in wich a vacancy can be filled with a radiative transition
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G4int
NumberOfReachableShells
(
G4int
Z)
const
;
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// This function returns the number of possible NON-radiative transitions for the atom with atomic number Z
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// i.e. the number of shell in wich a vacancy can be filled by a NON-radiative transition
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G4int
NumberOfReachableAugerShells
(
G4int
Z)
const
;
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// Gives the sum of the probabilities of radiative transition towards the
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// shell whose index is shellIndex
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G4double
TotalRadiativeTransitionProbability
(
G4int
Z,
size_t
shellIndex);
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// Gives the sum of the probabilities of non radiative transition from the
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// shell whose index is shellIndex
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G4double
TotalNonRadiativeTransitionProbability
(
G4int
Z,
size_t
shellIndex);
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protected
:
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G4AtomicTransitionManager
(
G4int
minZ = 1,
G4int
maxZ = 100,
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G4int
limitInfTable = 6,
G4int
limitSupTable=100 );
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~G4AtomicTransitionManager
();
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private
:
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// Hide copy constructor and assignment operator
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G4AtomicTransitionManager
& operator=(
const
G4AtomicTransitionManager
&
right
);
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G4AtomicTransitionManager
(
const
G4AtomicTransitionManager
&);
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static
G4AtomicTransitionManager
* instance;
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// the first element of the map is the atomic number Z.
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// the second element is a vector of G4AtomicShell*.
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std::map<G4int,std::vector<G4AtomicShell*>,std::less<G4int> > shellTable;
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// the first element of the map is the atomic number Z.
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// the second element is a vector of G4AtomicTransition*.
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std::map<G4int,std::vector<G4FluoTransition*>,std::less<G4int> > transitionTable;
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// since Augereffect data r stored as a table in G4AugerData, we have here a pointer to an element of that class itself.
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G4AugerData
* augerData;
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// Minimum and maximum Z in EADL table containing identities and binding
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// energies of shells
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G4int
zMin;
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G4int
zMax;
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// Minimum and maximum Z in EADL table containing identities, transition
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// energies and transition probabilities of shells
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G4int
infTableLimit;
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G4int
supTableLimit;
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};
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#endif
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