Geant4 10.7.0
Toolkit for the simulation of the passage of particles through matter
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G4PreCompoundTransitions Class Reference

#include <G4PreCompoundTransitions.hh>

+ Inheritance diagram for G4PreCompoundTransitions:

Public Member Functions

 G4PreCompoundTransitions ()
 
virtual ~G4PreCompoundTransitions ()
 
virtual G4double CalculateProbability (const G4Fragment &aFragment)
 
virtual void PerformTransition (G4Fragment &aFragment)
 
- Public Member Functions inherited from G4VPreCompoundTransitions
 G4VPreCompoundTransitions ()
 
virtual ~G4VPreCompoundTransitions ()
 
virtual G4double CalculateProbability (const G4Fragment &aFragment)=0
 
virtual void PerformTransition (G4Fragment &aFragment)=0
 
G4double GetTransitionProb1 () const
 
G4double GetTransitionProb2 () const
 
G4double GetTransitionProb3 () const
 
void UseNGB (G4bool use)
 
void UseCEMtr (G4bool use)
 

Additional Inherited Members

- Protected Attributes inherited from G4VPreCompoundTransitions
G4bool useNGB
 
G4bool useCEMtr
 
G4double TransitionProb1
 
G4double TransitionProb2
 
G4double TransitionProb3
 

Detailed Description

Definition at line 50 of file G4PreCompoundTransitions.hh.

Constructor & Destructor Documentation

◆ G4PreCompoundTransitions()

G4PreCompoundTransitions::G4PreCompoundTransitions ( )

Definition at line 58 of file G4PreCompoundTransitions.cc.

59{
60 proton = G4Proton::Proton();
62 G4DeexPrecoParameters* param = fNuclData->GetParameters();
63 FermiEnergy = param->GetFermiEnergy();
64 r0 = param->GetTransitionsR0();
65}
G4double GetTransitionsR0() const
G4DeexPrecoParameters * GetParameters()
static G4NuclearLevelData * GetInstance()
static G4Proton * Proton()
Definition: G4Proton.cc:92

◆ ~G4PreCompoundTransitions()

G4PreCompoundTransitions::~G4PreCompoundTransitions ( )
virtual

Definition at line 67 of file G4PreCompoundTransitions.cc.

68{}

Member Function Documentation

◆ CalculateProbability()

G4double G4PreCompoundTransitions::CalculateProbability ( const G4Fragment aFragment)
virtual

Implements G4VPreCompoundTransitions.

Definition at line 72 of file G4PreCompoundTransitions.cc.

74{
75 // Number of holes
76 G4int H = aFragment.GetNumberOfHoles();
77 // Number of Particles
78 G4int P = aFragment.GetNumberOfParticles();
79 // Number of Excitons
80 G4int N = P+H;
81 // Nucleus
82 G4int A = aFragment.GetA_asInt();
83 G4int Z = aFragment.GetZ_asInt();
84 G4double U = aFragment.GetExcitationEnergy();
85 TransitionProb2 = 0.0;
86 TransitionProb3 = 0.0;
87 /*
88 G4cout << "G4PreCompoundTransitions::CalculateProbability H/P/N/Z/A= "
89 << H << " " << P << " " << N << " " << Z << " " << A <<G4endl;
90 G4cout << aFragment << G4endl;
91 */
92 if(U < 10*eV || 0==N) { return 0.0; }
93
94 //J. M. Quesada (Feb. 08) new physics
95 // OPT=1 Transitions are calculated according to Gudima's paper
96 // (original in G4PreCompound from VL)
97 // OPT=2 Transitions are calculated according to Gupta's formulae
98 //
99 static const G4double sixdpi2 = 6.0/CLHEP::pi2;
100 G4double GE = sixdpi2*U*fNuclData->GetLevelDensity(Z,A,U);
101 if (useCEMtr) {
102 // Relative Energy (T_{rel})
103 G4double RelativeEnergy = 1.6*FermiEnergy + U/G4double(N);
104
105 // Sample kind of nucleon-projectile
106 G4bool ChargedNucleon(false);
107 if(G4int(P*G4UniformRand()) <= aFragment.GetNumberOfCharged()) {
108 ChargedNucleon = true;
109 }
110
111 // Relative Velocity:
112 // <V_{rel}>^2
113 G4double RelativeVelocitySqr;
114 if (ChargedNucleon) {
115 RelativeVelocitySqr = 2*RelativeEnergy/CLHEP::proton_mass_c2;
116 } else {
117 RelativeVelocitySqr = 2*RelativeEnergy/CLHEP::neutron_mass_c2;
118 }
119 // <V_{rel}>
120 G4double RelativeVelocity = std::sqrt(RelativeVelocitySqr);
121
122 // Proton-Proton Cross Section
123 G4double ppXSection =
124 (10.63/RelativeVelocitySqr - 29.92/RelativeVelocity + 42.9)
125 * CLHEP::millibarn;
126 // Proton-Neutron Cross Section
127 G4double npXSection =
128 (34.10/RelativeVelocitySqr - 82.20/RelativeVelocity + 82.2)
129 * CLHEP::millibarn;
130
131 // Averaged Cross Section: \sigma(V_{rel})
132 G4double AveragedXSection;
133 if (ChargedNucleon)
134 {
135 //JMQ: small bug fixed
136 AveragedXSection = ((Z-1)*ppXSection + (A-Z)*npXSection)/G4double(A-1);
137 }
138 else
139 {
140 AveragedXSection = ((A-Z-1)*ppXSection + Z*npXSection)/G4double(A-1);
141 }
142
143 // Fermi relative energy ratio
144 G4double FermiRelRatio = FermiEnergy/RelativeEnergy;
145
146 // This factor is introduced to take into account the Pauli principle
147 G4double PauliFactor = 1.0 - 1.4*FermiRelRatio;
148 if (FermiRelRatio > 0.5) {
149 G4double x = 2.0 - 1.0/FermiRelRatio;
150 PauliFactor += 0.4*FermiRelRatio*x*x*std::sqrt(x);
151 }
152 // Interaction volume
153 G4double xx = 2*r0 + CLHEP::hbarc/(CLHEP::proton_mass_c2*RelativeVelocity);
154 G4double Vint = CLHEP::pi*xx*xx*xx/0.75;
155
156 // Transition probability for \Delta n = +2
157
158 TransitionProb1 = std::max(0.0, AveragedXSection*PauliFactor
159 *std::sqrt(2.0*RelativeEnergy/CLHEP::proton_mass_c2)/Vint);
160
161 //JMQ 281009 phenomenological factor in order to increase
162 // equilibrium contribution
163 // G4double factor=5.0;
164 // TransitionProb1 *= factor;
165
166 // GE = g*E where E is Excitation Energy
167 G4double Fph = G4double(P*P+H*H+P-3*H)*0.25;
168
169 if(!useNGB) {
170
171 // F(p+1,h+1)
172 G4double Fph1 = Fph + N*0.5;
173
174 static const G4double plimit = 100;
175
176 //JMQ/AH bug fixed: if (U-Fph < 0.0)
177 if (GE > Fph1) {
178 G4double x0 = GE-Fph;
179 G4double x1 = (N+1)*G4Log(x0/(GE-Fph1));
180 if(x1 < plimit) {
181 x1 = G4Exp(x1)*TransitionProb1/x0;
182
183 // Transition probability for \Delta n = -2 (at F(p,h) = 0)
184 TransitionProb2 = std::max(0.0, (P*H*(N+1)*(N-2))*x1/x0);
185
186 // Transition probability for \Delta n = 0 (at F(p,h) = 0)
187 TransitionProb3 = std::max(0.0,((N+1)*(P*(P-1) + 4*P*H + H*(H-1)))*x1
188 /G4double(N));
189 }
190 }
191 }
192
193 } else {
194 //JMQ: Transition probabilities from Gupta's work
195 // GE = g*E where E is Excitation Energy
196 TransitionProb1 = std::max(0.0, U*(4.2e+12 - 3.6e+10*U/G4double(N+1)))
197 /(16*CLHEP::c_light);
198
199 if (!useNGB && N > 1) {
200 TransitionProb2 = ((N-1)*(N-2)*P*H)*TransitionProb1/(GE*GE);
201 }
202 }
203 // G4cout<<"U = "<<U<<G4endl;
204 // G4cout<<"N="<<N<<" P="<<P<<" H="<<H<<G4endl;
205 // G4cout<<"l+ ="<<TransitionProb1<<" l- ="<< TransitionProb2
206 // <<" l0 ="<< TransitionProb3<<G4endl;
208}
@ GE
Definition: Evaluator.cc:65
double A(double temperature)
G4double G4Exp(G4double initial_x)
Exponential Function double precision.
Definition: G4Exp.hh:179
G4double G4Log(G4double x)
Definition: G4Log.hh:226
double G4double
Definition: G4Types.hh:83
bool G4bool
Definition: G4Types.hh:86
int G4int
Definition: G4Types.hh:85
#define G4UniformRand()
Definition: Randomize.hh:52
G4int GetNumberOfParticles() const
Definition: G4Fragment.hh:337
G4int GetNumberOfHoles() const
Definition: G4Fragment.hh:357
G4double GetExcitationEnergy() const
Definition: G4Fragment.hh:275
G4int GetZ_asInt() const
Definition: G4Fragment.hh:263
G4int GetNumberOfCharged() const
Definition: G4Fragment.hh:342
G4int GetA_asInt() const
Definition: G4Fragment.hh:258
G4double GetLevelDensity(G4int Z, G4int A, G4double U)

◆ PerformTransition()

void G4PreCompoundTransitions::PerformTransition ( G4Fragment aFragment)
virtual

Implements G4VPreCompoundTransitions.

Definition at line 210 of file G4PreCompoundTransitions.cc.

211{
212 G4double ChosenTransition =
214 G4int deltaN = 0;
215 G4int Npart = result.GetNumberOfParticles();
216 G4int Ncharged = result.GetNumberOfCharged();
217 G4int Nholes = result.GetNumberOfHoles();
218 if (ChosenTransition <= TransitionProb1)
219 {
220 // Number of excitons is increased on \Delta n = +2
221 deltaN = 2;
222 }
223 else if (ChosenTransition <= TransitionProb1+TransitionProb2)
224 {
225 // Number of excitons is increased on \Delta n = -2
226 deltaN = -2;
227 }
228
229 // AH/JMQ: Randomly decrease the number of charges if deltaN is -2 and
230 // in proportion to the number charges w.r.t. number of particles,
231 // PROVIDED that there are charged particles
232 deltaN /= 2;
233
234 //G4cout << "deltaN= " << deltaN << G4endl;
235
236 // JMQ the following lines have to be before SetNumberOfCharged,
237 // otherwise the check on number of charged vs. number of particles fails
238 result.SetNumberOfParticles(Npart+deltaN);
239 result.SetNumberOfHoles(Nholes+deltaN);
240
241 if(deltaN < 0) {
242 if( (Ncharged == Npart) ||
243 (Ncharged >= 1 && G4int(Npart*G4UniformRand()) <= Ncharged))
244 {
245 result.SetNumberOfCharged(Ncharged+deltaN); // deltaN is negative!
246 }
247
248 } else if ( deltaN > 0 ) {
249 // With weight Z/A, number of charged particles is increased with +1
250 G4int A = result.GetA_asInt() - Npart;
251 G4int Z = result.GetZ_asInt() - Ncharged;
252 if((Z == A) || (Z > 0 && G4int(A*G4UniformRand()) <= Z))
253 {
254 result.SetNumberOfCharged(Ncharged+deltaN);
255 }
256 }
257
258 // Number of charged can not be greater that number of particles
259 if ( Npart < Ncharged )
260 {
261 result.SetNumberOfCharged(Npart);
262 }
263 //G4cout << "### After transition" << G4endl;
264 //G4cout << result << G4endl;
265}

The documentation for this class was generated from the following files: