source: trunk/source/processes/hadronic/models/de_excitation/evaporation/include/G4EvaporationChannel.hh

Last change on this file was 1347, checked in by garnier, 14 years ago

geant4 tag 9.4

File size: 5.1 KB
Line 
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26// $Id: G4EvaporationChannel.hh,v 1.11 2010/11/17 12:19:08 vnivanch Exp $
27// GEANT4 tag $Name: geant4-09-04-ref-00 $
28//
29//
30//J.M. Quesada (August2008). Based on:
31//
32// Hadronic Process: Nuclear De-excitations
33// by V. Lara (Oct 1998)
34//
35// 17-11-2010 V.Ivanchenko in constructor replace G4VEmissionProbability by
36//            G4EvaporationProbability and do not new and delete probability
37//            object at each call; use G4Pow
38
39#ifndef G4EvaporationChannel_h
40#define G4EvaporationChannel_h 1
41
42#include "G4VEvaporationChannel.hh"
43#include "G4EvaporationProbability.hh"
44#include "G4VCoulombBarrier.hh"
45
46class G4EvaporationLevelDensityParameter;
47
48class G4EvaporationChannel : public G4VEvaporationChannel
49{
50public:
51  // constructor
52  G4EvaporationChannel(G4int theA, G4int theZ, const G4String & aName,
53                       G4EvaporationProbability * aEmissionStrategy,
54                       G4VCoulombBarrier * aCoulombBarrier);
55public:
56  // destructor
57  virtual ~G4EvaporationChannel();
58 
59  inline void SetEmissionStrategy(G4EvaporationProbability * aEmissionStrategy)
60  {theEvaporationProbabilityPtr = aEmissionStrategy;}
61
62  inline void SetCoulombBarrierStrategy(G4VCoulombBarrier * aCoulombBarrier)
63  {theCoulombBarrierPtr = aCoulombBarrier;} 
64   
65protected:
66  // default constructor
67  G4EvaporationChannel();
68 
69private:
70  // copy constructor
71  G4EvaporationChannel(const G4EvaporationChannel & right);
72 
73private:
74  const G4EvaporationChannel & operator=(const G4EvaporationChannel & right);
75 
76public:
77  G4bool operator==(const G4EvaporationChannel & right) const;
78  G4bool operator!=(const G4EvaporationChannel & right) const;
79
80public:
81  void Initialize(const G4Fragment & fragment);
82
83  G4FragmentVector * BreakUp(const G4Fragment & theNucleus);
84
85public:
86
87  inline G4double GetEmissionProbability(void) const 
88  {return EmissionProbability;}
89   
90  inline G4double GetMaximalKineticEnergy(void) const 
91  { return MaximalKineticEnergy; }
92 
93private: 
94 
95  // Calculate Binding Energy for separate fragment from nucleus
96  G4double CalcBindingEnergy(G4int anA, G4int aZ);
97
98  // Calculate maximal kinetic energy that can be carried by fragment (in MeV)
99  G4double CalcMaximalKineticEnergy(G4double U);
100
101  // Samples fragment kinetic energy.
102  G4double  GetKineticEnergy(const G4Fragment & aFragment);
103
104  // This has to be removed and put in Random Generator
105  G4ThreeVector IsotropicVector(G4double Magnitude  = 1.0);
106
107        // Data Members
108        // ************
109private:
110
111  // This data member define the channel.
112  // They are intializated at object creation (constructor) time.
113
114  // Atomic Number of ejectile
115  G4int theA;
116
117  // Charge of ejectile
118  G4int theZ;
119
120  G4double EvaporatedMass;
121  G4double ResidualMass;
122
123  // For evaporation probability calcualation
124  G4EvaporationProbability * theEvaporationProbabilityPtr;
125
126  // For Level Density calculation
127  // G4bool MyOwnLevelDensity;
128  G4VLevelDensityParameter * theLevelDensityPtr;
129
130  // For Coulomb Barrier calculation
131  G4VCoulombBarrier * theCoulombBarrierPtr;
132  G4double CoulombBarrier;
133   
134  //---------------------------------------------------
135
136  // These values depend on the nucleus that is being evaporated.
137  // They are calculated through the Initialize method which takes as parameters
138  // the atomic number, charge and excitation energy of nucleus.
139
140  // Residual Mass Number
141  G4int ResidualA;
142
143  // Residual Charge
144  G4int ResidualZ;
145       
146  // Emission Probability
147  G4double EmissionProbability;
148
149  // Maximal Kinetic Energy that can be carried by fragment
150  G4double MaximalKineticEnergy;
151
152};
153
154
155#endif
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