source: trunk/source/processes/hadronic/models/de_excitation/multifragmentation/src/G4StatMFMicroManager.cc @ 1337

Last change on this file since 1337 was 1337, checked in by garnier, 14 years ago

tag geant4.9.4 beta 1 + modifs locales

File size: 6.4 KB
Line 
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27// $Id: G4StatMFMicroManager.cc,v 1.6 2008/07/25 11:20:47 vnivanch Exp $
28// GEANT4 tag $Name: geant4-09-04-beta-01 $
29//
30// Hadronic Process: Nuclear De-excitations
31// by V. Lara
32
33
34#include "G4StatMFMicroManager.hh"
35#include "G4HadronicException.hh"
36
37
38// Copy constructor
39G4StatMFMicroManager::G4StatMFMicroManager(const G4StatMFMicroManager & )
40{
41    throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMicroManager::copy_constructor meant to not be accessable");
42}
43
44// Operators
45
46G4StatMFMicroManager & G4StatMFMicroManager::
47operator=(const G4StatMFMicroManager & )
48{
49    throw G4HadronicException(__FILE__, __LINE__, "G4StatMFMicroManager::operator= meant to not be accessable");
50    return *this;
51}
52
53
54G4bool G4StatMFMicroManager::operator==(const G4StatMFMicroManager & ) const
55{
56    return false;
57}
58 
59
60G4bool G4StatMFMicroManager::operator!=(const G4StatMFMicroManager & ) const
61{
62    return true;
63}
64
65
66
67// constructor
68G4StatMFMicroManager::G4StatMFMicroManager(const G4Fragment & theFragment, const G4int multiplicity,
69                                           const G4double FreeIntE, const G4double SCompNuc) : 
70    _Normalization(0.0)
71{
72    // Perform class initialization
73    Initialize(theFragment,multiplicity,FreeIntE,SCompNuc);
74}
75
76
77// destructor
78G4StatMFMicroManager::~G4StatMFMicroManager() 
79{
80  if (!_Partition.empty()) 
81    {
82      std::for_each(_Partition.begin(),_Partition.end(),
83                      DeleteFragment());
84    }
85}
86
87
88
89// Initialization method
90
91void G4StatMFMicroManager::Initialize(const G4Fragment & theFragment, const G4int m, 
92                                      const G4double FreeIntE, const G4double SCompNuc) 
93{
94    G4int i;
95
96    G4double U = theFragment.GetExcitationEnergy();
97
98    G4double A = theFragment.GetA();
99    G4double Z = theFragment.GetZ();
100       
101    // Statistical weights
102    _WW = 0.0;
103
104    // Mean breakup multiplicity
105    _MeanMultiplicity = 0.0;
106
107    // Mean channel temperature
108    _MeanTemperature = 0.0;
109
110    // Mean channel entropy
111    _MeanEntropy = 0.0; 
112       
113    // Keep fragment atomic numbers
114//      G4int * FragmentAtomicNumbers = new G4int(static_cast<G4int>(A+0.5));
115//      G4int * FragmentAtomicNumbers = new G4int(m);
116    G4int FragmentAtomicNumbers[4];
117       
118    // We distribute A nucleons between m fragments mantaining the order
119    // FragmentAtomicNumbers[m-1]>FragmentAtomicNumbers[m-2]>...>FragmentAtomicNumbers[0]
120    // Our initial distribution is
121    // FragmentAtomicNumbers[m-1]=A, FragmentAtomicNumbers[m-2]=0, ..., FragmentAtomicNumbers[0]=0
122    FragmentAtomicNumbers[m-1] = static_cast<G4int>(A);
123    for (i = 0; i <  (m - 1); i++) FragmentAtomicNumbers[i] = 0;
124
125    // We try to distribute A nucleons in partitions of m fragments
126    // MakePartition return true if it is possible
127    // and false if it is not   
128    while (MakePartition(m,FragmentAtomicNumbers)) {
129        // Allowed partitions are stored and its probability calculated
130                       
131        G4StatMFMicroPartition * aPartition = new G4StatMFMicroPartition(static_cast<G4int>(A),
132                                                                         static_cast<G4int>(Z));
133        G4double PartitionProbability = 0.0;
134                       
135        for (i = m-1; i >= 0; i--) aPartition->SetPartitionFragment(FragmentAtomicNumbers[i]);
136        PartitionProbability = aPartition->CalcPartitionProbability(U,FreeIntE,SCompNuc);
137        _Partition.push_back(aPartition);
138                       
139        _WW += PartitionProbability;
140        _MeanMultiplicity += m*PartitionProbability;
141        _MeanTemperature += aPartition->GetTemperature() * PartitionProbability;
142        if (PartitionProbability > 0.0) 
143            _MeanEntropy += PartitionProbability * aPartition->GetEntropy();
144                       
145    }
146               
147       
148    // garbage collection
149//      delete [] FragmentAtomicNumbers;
150       
151}
152
153
154G4bool G4StatMFMicroManager::MakePartition(const G4int k, G4int * ANumbers)
155    // Distributes A nucleons between k fragments
156    // mantaining the order ANumbers[k-1] > ANumbers[k-2] > ... > ANumbers[0]
157    // If it is possible returns true. In other case returns false
158{
159    G4int l = 1;
160    while (l < k) {
161        G4int tmp = ANumbers[l-1] + ANumbers[k-1];
162        ANumbers[l-1] += 1;
163        ANumbers[k-1] -= 1;
164        if (ANumbers[l-1] > ANumbers[l] || ANumbers[k-2] > ANumbers[k-1]) {
165            ANumbers[l-1] = 1;
166            ANumbers[k-1] = tmp - 1;
167            l++;
168        } else return true;
169    }
170    return false;
171}
172
173
174
175void G4StatMFMicroManager::Normalize(const G4double Norm)
176{
177    _Normalization = Norm;
178    _WW /= Norm;
179    _MeanMultiplicity /= Norm;
180    _MeanTemperature /= Norm;
181    _MeanEntropy /= Norm; 
182       
183    return;
184}
185
186G4StatMFChannel * G4StatMFMicroManager::ChooseChannel(const G4double A0, const G4double Z0, 
187                                                      const G4double MeanT)
188{
189    G4double RandNumber = _Normalization * _WW * G4UniformRand();
190    G4double AccumWeight = 0.0;
191       
192    for (std::vector<G4StatMFMicroPartition*>::iterator i = _Partition.begin();
193         i != _Partition.end(); ++i)
194    {
195        AccumWeight += (*i)->GetProbability();
196        if (RandNumber < AccumWeight)
197            return (*i)->ChooseZ(A0,Z0,MeanT);
198    }
199
200    throw G4HadronicException(__FILE__, __LINE__, 
201        "G4StatMFMicroCanonical::ChooseChannel: Couldn't find a channel.");
202    return 0;
203}
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