Geant4 9.6.0
Toolkit for the simulation of the passage of particles through matter
Loading...
Searching...
No Matches
G4QLowEnergy.hh
Go to the documentation of this file.
1//
2// ********************************************************************
3// * License and Disclaimer *
4// * *
5// * The Geant4 software is copyright of the Copyright Holders of *
6// * the Geant4 Collaboration. It is provided under the terms and *
7// * conditions of the Geant4 Software License, included in the file *
8// * LICENSE and available at http://cern.ch/geant4/license . These *
9// * include a list of copyright holders. *
10// * *
11// * Neither the authors of this software system, nor their employing *
12// * institutes,nor the agencies providing financial support for this *
13// * work make any representation or warranty, express or implied, *
14// * regarding this software system or assume any liability for its *
15// * use. Please see the license in the file LICENSE and URL above *
16// * for the full disclaimer and the limitation of liability. *
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 *
22// * use in resulting scientific publications, and indicate your *
23// * acceptance of all terms of the Geant4 Software license. *
24// ********************************************************************
25//
26// $Id$
27//
28// ---------------- G4QLowEnergy header ----------------
29// by Mikhail Kossov, Aug 2007.
30// Header of G4QLowEnergy class (A+A) of the CHIPS Simulation Branch in GEANT4
31// -------------------------------------------------------------------------------
32// This is a unique CHIPS class for the Ion-Ion Low Energy Inelastic Interactions
33// -------------------------------------------------------------------------------
34// At present (Aug-07) it is not tested.
35// The normalization is based on the temporary G4QIonIonCrossSection class
36// -------------------------------------------------------------------------------
37// Short description: This is a fast low energy algorithm for the
38// inelastic interactions of nucleons and nuclei (ions) with nuclei.
39// This is a fase-space algorithm, but not quark level. Provides
40// nuclear fragments upto alpha only. Never was tumed (but can be).
41// ---------------------------------------------------------------
42
43#ifndef G4QLowEnergy_hh
44#define G4QLowEnergy_hh
45
46// GEANT4 Headers
47#include "globals.hh"
48#include "G4ios.hh"
49#include "Randomize.hh"
50#include "G4VDiscreteProcess.hh"
51#include "G4Track.hh"
52#include "G4Step.hh"
53#include "G4ParticleTypes.hh"
54#include "G4ParticleTable.hh"
55#include "G4VParticleChange.hh"
57#include "G4DynamicParticle.hh"
58#include "G4ThreeVector.hh"
59#include "G4LorentzVector.hh"
60
61// CHIPS Headers
62#include "G4QNucleus.hh"
67#include "G4QIsotope.hh"
68#include "G4QCHIPSWorld.hh"
69#include "G4QHadronVector.hh"
70#include <vector>
71
73{
74public:
75
76 // Constructor
77 G4QLowEnergy(const G4String& processName ="CHIPS_LowEnergyIonIonInelastic");
78
79 // Destructor
81
83
84 G4double GetMeanFreePath(const G4Track& aTrack, G4double previousStepSize,
86 // It returns the MeanFreePath of the process for the current track :
87 // (energy, material)
88 // The previousStepSize and G4ForceCondition* are not used.
89 // This function overloads a virtual function of the base class.
90 // It is invoked by the ProcessManager of the Particle.
91
92
93 G4VParticleChange* PostStepDoIt(const G4Track& aTrack, const G4Step& aStep);
94 // It computes the final state of the process (at end of step),
95 // returned as a ParticleChange object.
96 // This function overloads a virtual function of the base class.
97 // It is invoked by the ProcessManager of the Particle.
98
100
102
103 void SwitchOnEvaporation() {evaporate=true;} // Evaporation instead of gammas (default)
104
105 void SwitchOffEvaporation() {evaporate=false;} // Gammas instead of evaporation
106
107private:
108
109 // Hide assignment operator as private
110 G4QLowEnergy& operator=(const G4QLowEnergy &right);
111
112 // Copy constructor
114
115 // Calculate Cross-Section of the Diffraction Reaction (p is in GeV @@ units)
116 G4double CalculateXS(G4double p, G4int Z, G4int N, G4int pPDG);
117
118 // BODY
119 // Static Parameters --------------------------------------------------------------------
120 static G4int nPartCWorld; // The#of particles for hadronization (limit of A of fragm.)
121 //--------------------------------- End of static parameters ---------------------------
122 // Working parameters
123 G4bool evaporate;
124 G4VQCrossSection* theCS;
125 G4LorentzVector EnMomConservation; // Residual of Energy/Momentum Cons.
126 G4int nOfNeutrons; // #of neutrons in the target nucleus
127
128 // Modifires for the reaction
129 G4double Time; // Time shift of the capture reaction
130 G4double EnergyDeposition; // Energy deposited in the reaction
131 static std::vector <G4int> ElementZ; // Z of the element(i) in theLastCalc
132 static std::vector <G4double> ElProbInMat; // SumProbabilityElements in Material
133 static std::vector <std::vector<G4int>*> ElIsoN; // N of isotope(j) of Element(i)
134 static std::vector <std::vector<G4double>*> IsoProbInEl;// SumProbabIsotopes in Element i
135};
136#endif
G4double condition(const G4ErrorSymMatrix &m)
G4ForceCondition
double G4double
Definition: G4Types.hh:64
int G4int
Definition: G4Types.hh:66
bool G4bool
Definition: G4Types.hh:67
G4LorentzVector GetEnegryMomentumConservation()
Definition: G4QLowEnergy.cc:76
G4double GetMeanFreePath(const G4Track &aTrack, G4double previousStepSize, G4ForceCondition *condition)
Definition: G4QLowEnergy.cc:83
G4VParticleChange * PostStepDoIt(const G4Track &aTrack, const G4Step &aStep)
G4bool IsApplicable(const G4ParticleDefinition &particle)
G4int GetNumberOfNeutronsInTarget()
Definition: G4QLowEnergy.cc:78
void SwitchOffEvaporation()
void SwitchOnEvaporation()
Definition: G4Step.hh:78