#include <G4BertiniEvaporationChannel.hh>
Inheritance diagram for G4BertiniEvaporationChannel:
Definition at line 38 of file G4BertiniEvaporationChannel.hh.
| G4BertiniEvaporationChannel::G4BertiniEvaporationChannel | ( | ) |
Definition at line 46 of file G4BertiniEvaporationChannel.cc.
References verboseLevel.
00047 { 00048 verboseLevel = 0; 00049 }
| G4BertiniEvaporationChannel::~G4BertiniEvaporationChannel | ( | ) | [virtual] |
| virtual void G4BertiniEvaporationChannel::calculateProbability | ( | ) | [pure virtual] |
Implemented in G4BEChargedChannel, and G4BENeutronChannel.
Definition at line 353 of file G4BertiniEvaporationChannel.cc.
00354 { 00355 // Gives the binding energy correction depending in N 00356 // due to shell correction and pairing energies in MeV 00357 // 00358 // see Cameron, Canadian Journal of Physics, 00359 // vol. 35, 1957, p.1022 00360 G4double table[200] = { 00361 -0.83199997E+01, -0.15899999E+02, -0.11509999E+02, -0.14309999E+02, -0.11570000E+02, 00362 -0.15899999E+02, -0.13909999E+02, -0.16029999E+02, -0.12129999E+02, -0.13869999E+02, 00363 -0.12249998E+02, -0.14399999E+02, -0.13069999E+02, -0.15799998E+02, -0.13809999E+02, 00364 -0.14980000E+02, -0.12629999E+02, -0.13759999E+02, -0.11369999E+02, -0.12379998E+02, 00365 -0.92299995E+01, -0.96499996E+01, -0.76399994E+01, -0.91699991E+01, -0.80499992E+01, 00366 -0.97199993E+01, -0.88699989E+01, -0.10759999E+02, -0.86399994E+01, -0.88899994E+01, 00367 -0.65999994E+01, -0.71299992E+01, -0.47699995E+01, -0.53299990E+01, -0.30599995E+01, 00368 -0.37899990E+01, -0.17199993E+01, -0.27899990E+01, -0.92999995E+00, -0.21899996E+01, 00369 -0.51999998E+00, -0.18999996E+01, -0.44999999E+00, -0.21999998E+01, -0.12199993E+01, 00370 -0.30699997E+01, -0.24199991E+01, -0.43699999E+01, -0.39399996E+01, -0.60799999E+01, 00371 -0.44899998E+01, -0.45000000E+01, -0.31399994E+01, -0.29299994E+01, -0.10399990E+01, 00372 -0.13599997E+01, 0.69000000E+00, 0.20999998E+00, 0.21099997E+01, 0.13299990E+01, 00373 0.32900000E+01, 0.24599991E+01, 0.42999992E+01, 0.33199997E+01, 0.47899990E+01, 00374 0.36199999E+01, 0.49699993E+01, 0.36399994E+01, 0.46299992E+01, 0.30699997E+01, 00375 0.40599995E+01, 0.24899998E+01, 0.32999992E+01, 0.14599991E+01, 0.20599995E+01, 00376 0.50999999E+00, 0.73999995E+00, -0.11799994E+01, -0.12599993E+01, -0.35399990E+01, 00377 -0.39699993E+01, -0.52599993E+01, -0.41799994E+01, -0.37099991E+01, -0.20999994E+01, 00378 -0.16999998E+01, -0.79999983E-01, -0.17999995E+00, 0.94000000E+00, 0.26999998E+00, 00379 0.11299992E+01, 0.79999983E-01, 0.90999997E+00, -0.30999994E+00, 0.48999995E+00, 00380 -0.77999997E+00, 0.79999983E-01, -0.11499996E+01, -0.22999996E+00, -0.14099998E+01, 00381 -0.41999996E+00, -0.15499992E+01, -0.54999995E+00, -0.16599998E+01, -0.65999997E+00, 00382 -0.17299995E+01, -0.75000000E+00, -0.17399998E+01, -0.77999997E+00, -0.16899996E+01, 00383 -0.77999997E+00, -0.15999994E+01, -0.75000000E+00, -0.14599991E+01, -0.66999996E+00, 00384 -0.12599993E+01, -0.50999999E+00, -0.10399990E+01, -0.52999997E+00, -0.18399992E+01, 00385 -0.24199991E+01, -0.45199995E+01, -0.47599993E+01, -0.63299990E+01, -0.67599993E+01, 00386 -0.78099995E+01, -0.57999992E+01, -0.53699999E+01, -0.36299992E+01, -0.33499994E+01, 00387 -0.17500000E+01, -0.18799992E+01, -0.60999995E+00, -0.89999998E+00, 0.89999974E-01, 00388 -0.31999993E+00, 0.54999995E+00, -0.13000000E+00, 0.69999999E+00, -0.59999999E-01, 00389 0.48999995E+00, -0.19999999E+00, 0.39999998E+00, -0.21999997E+00, 0.35999995E+00, 00390 -0.89999974E-01, 0.57999998E+00, 0.11999995E+00, 0.75000000E+00, 0.14999998E+00, 00391 0.69999999E+00, 0.16999996E+00, 0.11099997E+01, 0.88999999E+00, 0.18499994E+01, 00392 0.16199999E+01, 0.25399990E+01, 0.22899990E+01, 0.31999998E+01, 0.29099998E+01, 00393 0.38399992E+01, 0.35299997E+01, 0.44799995E+01, 0.41499996E+01, 0.51199999E+01, 00394 0.47799997E+01, 0.57500000E+01, 0.53899994E+01, 0.63099995E+01, 0.59099998E+01, 00395 0.68699999E+01, 0.63299990E+01, 0.71299992E+01, 0.66099997E+01, 0.72999992E+01, 00396 0.63099995E+01, 0.62699995E+01, 0.48299999E+01, 0.44899998E+01, 0.28499994E+01, 00397 0.23199997E+01, 0.57999998E+00, -0.10999995E+00, -0.97999996E+00, 0.80999994E+00, 00398 0.17699995E+01, 0.33699999E+01, 0.41299992E+01, 0.55999994E+01, 0.61499996E+01, 00399 0.72899990E+01, 0.73499994E+01, 0.79499998E+01, 0.76699991E+01, 0.81599998E+01, 00400 0.78299990E+01, 0.83099995E+01, 0.80099993E+01, 0.85299997E+01, 0.82699995E+01 00401 }; 00402 if ( N > 130 ) throw G4HadronicException(__FILE__, __LINE__, " G4BertiniEvaporationChannel: shell correction for protons called with too large N " ); 00403 return table[ N-1 ]*MeV; 00404 }
Definition at line 313 of file G4BertiniEvaporationChannel.cc.
00314 { 00315 // Gives the binding energy correction depending in Z 00316 // due to shell correction and pairing energies in MeV 00317 // 00318 // see Cameron, Canadian Journal of Physics, 00319 // vol. 35, 1957, p.1022 00320 G4double table[130] = { 00321 0.26169998E+02, 0.19250000E+02, 0.24209991E+02, 0.20919998E+02, 0.23149994E+02, 00322 0.18009995E+02, 0.19549988E+02, 0.16939987E+02, 0.19729996E+02, 0.17069992E+02, 00323 0.18209991E+02, 0.14990000E+02, 0.16009995E+02, 0.12040000E+02, 0.13270000E+02, 00324 0.11089998E+02, 0.12169999E+02, 0.10259998E+02, 0.11040000E+02, 0.84099998E+01, 00325 0.97899990E+01, 0.73599997E+01, 0.81499996E+01, 0.56299992E+01, 0.58799992E+01, 00326 0.31699991E+01, 0.33199997E+01, 0.81999993E+00, 0.18299999E+01, 0.96999997E+00, 00327 0.23299999E+01, 0.12699995E+01, 0.29199991E+01, 0.16099997E+01, 0.29099998E+01, 00328 0.13499994E+01, 0.23999996E+01, 0.88999999E+00, 0.17399998E+01, 0.35999995E+00, 00329 0.94999999E+00, -0.64999998E+00, -0.39999995E-01, -0.17299995E+01, -0.95999998E+00, 00330 -0.28699999E+01, -0.20499992E+01, -0.40499992E+01, -0.33999996E+01, -0.57199993E+01, 00331 -0.37499990E+01, -0.41299992E+01, -0.24199991E+01, -0.28499994E+01, -0.10099993E+01, 00332 -0.13299990E+01, 0.53999996E+00, -0.20000000E-01, 0.17399998E+01, 0.75000000E+00, 00333 0.22399998E+01, 0.99999988E+00, 0.19799995E+01, 0.78999996E+00, 0.15399990E+01, 00334 0.38999999E+00, 0.10799999E+01, 0.00000000E+00, 0.77999997E+00, -0.34999996E+00, 00335 0.57999998E+00, -0.54999995E+00, 0.58999997E+00, -0.60999995E+00, 0.58999997E+00, 00336 -0.34999996E+00, 0.31999993E+00, -0.95999998E+00, -0.51999998E+00, -0.20799999E+01, 00337 -0.24599991E+01, -0.36399994E+01, -0.15499992E+01, -0.95999998E+00, 0.96999997E+00, 00338 0.88000000E+00, 0.23699999E+01, 0.17500000E+01, 0.27199993E+01, 0.18999996E+01, 00339 0.25499992E+01, 0.14599991E+01, 0.19299994E+01, 0.85999995E+00, 0.11699991E+01, 00340 0.79999983E-01, 0.38999999E+00, -0.75999999E+00, -0.38999999E+00, -0.15099993E+01, 00341 -0.11699991E+01, -0.23599997E+01, -0.19499998E+01, -0.30599995E+01, -0.26199999E+01, 00342 -0.35499992E+01, -0.29499998E+01, -0.37499990E+01, -0.30699997E+01, -0.37899990E+01, 00343 -0.30599995E+01, -0.37699995E+01, -0.30499992E+01, -0.37799997E+01, -0.31199999E+01, 00344 -0.38999996E+01, -0.33499994E+01, -0.42399998E+01, -0.38599997E+01, -0.49199991E+01, 00345 -0.50599995E+01, -0.67699995E+01, -0.74099998E+01, -0.91799994E+01, -0.10160000E+02, 00346 -0.11120000E+02, -0.97599993E+01, -0.92299995E+01, -0.79599991E+01, -0.76499996E+01, 00347 }; 00348 if ( Z > 130 ) throw G4HadronicException(__FILE__, __LINE__, " G4BertiniEvaporationChannel: shell correction for protons called with too large Z " ); 00349 return table[ Z-1 ]*MeV; 00350 }
| virtual G4DynamicParticle* G4BertiniEvaporationChannel::emit | ( | ) | [pure virtual] |
Implemented in G4BEChargedChannel, G4BEDeuteronChannel, G4BEHe3Channel, G4BEHe4Channel, G4BENeutronChannel, G4BEProtonChannel, and G4BETritonChannel.
Referenced by G4BertiniEvaporation::BreakItUp().
| G4double G4BertiniEvaporationChannel::getCoulomb | ( | ) | [virtual] |
Definition at line 159 of file G4BertiniEvaporationChannel.cc.
References correction, G4cout, G4endl, getQ(), nucleusA, nucleusZ, particleA, particleZ, qmFactor(), rho, and verboseLevel.
Referenced by getThresh(), and G4BEChargedChannel::sampleKineticEnergy().
00160 { 00161 G4int residualZ = nucleusZ - particleZ; 00162 G4int residualA = nucleusA - particleA; 00163 const G4double factor = 0.84696; // = e / ( 4 pi epsilon_0 r0 ) * 10^-6, r0=1.7E-15 00164 // In HETC88 this factor was 0.88235, perhaps due to different r0 00165 00166 G4double coulombBarrier = factor * particleZ * qmFactor() * residualZ / 00167 ( std::pow( G4double(residualA), 0.33333333 ) + rho ) * MeV; 00168 00169 if ( verboseLevel >= 10 ) 00170 G4cout << " G4BertiniEvaporationChannel::getThresh() " << G4endl 00171 << " residualZ " << residualZ << G4endl 00172 << " residualA " << residualA << G4endl 00173 << " qmFactor " << qmFactor() << G4endl 00174 << " Q " << getQ() << G4endl 00175 << " rho " << rho << G4endl 00176 << " part Z " << particleZ << G4endl 00177 << " (correction) " << correction << G4endl; 00178 00179 return coulombBarrier; 00180 }
| G4double G4BertiniEvaporationChannel::getLevelDensityParameter | ( | ) |
Definition at line 192 of file G4BertiniEvaporationChannel.cc.
References nucleusA, nucleusZ, particleA, and particleZ.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), G4BENeutronChannel::sampleKineticEnergy(), and G4BEChargedChannel::sampleKineticEnergy().
00193 { 00194 G4int residualZ = nucleusZ - particleZ; 00195 G4int residualA = nucleusA - particleA; 00196 G4double b0 = 8; 00197 G4double y0 = 1.5; 00198 00199 G4double temp = ( residualA - 2.0 * residualZ ) / residualA; 00200 G4double smallA = residualA * ( 1.0 + y0 * std::pow( temp, 2. ) ) / b0 / MeV; 00201 00202 // In HETC98 b0 = b0(E). 00203 00204 return smallA; 00205 }
| G4String G4BertiniEvaporationChannel::getName | ( | ) |
Definition at line 116 of file G4BertiniEvaporationChannel.cc.
References name.
Referenced by G4BertiniEvaporation::BreakItUp(), and G4BEChargedChannel::calculateProbability().
00117 { 00118 return name; 00119 }
| G4int G4BertiniEvaporationChannel::getParticleA | ( | ) |
Definition at line 75 of file G4BertiniEvaporationChannel.cc.
References particleA.
Referenced by G4BertiniEvaporation::BreakItUp().
00076 { 00077 return particleA; 00078 }
| G4int G4BertiniEvaporationChannel::getParticleZ | ( | ) |
Definition at line 81 of file G4BertiniEvaporationChannel.cc.
References particleZ.
Referenced by G4BertiniEvaporation::BreakItUp().
00082 { 00083 return particleZ; 00084 }
| G4double G4BertiniEvaporationChannel::getProbability | ( | ) | [virtual] |
Definition at line 106 of file G4BertiniEvaporationChannel.cc.
References emissionProbability, G4cout, G4endl, name, and verboseLevel.
00107 { 00108 if ( verboseLevel >= 4 ) 00109 G4cout << "G4BerEvaporationChannel : probability of particle " << name 00110 << " is " << emissionProbability << G4endl; 00111 00112 return emissionProbability; 00113 }
| G4double G4BertiniEvaporationChannel::getQ | ( | ) | [virtual] |
Definition at line 129 of file G4BertiniEvaporationChannel.cc.
References G4NucleiProperties::GetMassExcess(), nucleusA, nucleusZ, particleA, and particleZ.
Referenced by G4BertiniEvaporation::BreakItUp(), getCoulomb(), and getThresh().
00130 { 00131 // The reaction Q is calculated by using the excess masses of the 00132 // secondary particle and the initial and residual nuclei 00133 G4int residualZ = nucleusZ - particleZ; 00134 G4int residualA = nucleusA - particleA; 00135 // G4int residualN = residualA - residualZ; 00136 // G4int nucleusN = nucleusA - nucleusZ; 00137 00138 // All the following are by default in MeV 00139 const G4double e1 = G4NucleiProperties::GetMassExcess( residualA, residualZ ); 00140 const G4double e2 = G4NucleiProperties::GetMassExcess( nucleusA, nucleusZ ); 00141 00142 return e1 - e2 + G4NucleiProperties::GetMassExcess( particleA, particleZ ); 00143 // In HETC88 : Mass excesses were calculated with the Cameron mass excess formula, 00144 // see Cameron, Canadian Journal of Physics, 00145 // vol. 35, 1957, p.1022 00146 // Also mass excesses of particles were 00147 // 8.3675, 7.5851, 13.7279, 15.8381, 15.8195, 3.6092 for 00148 // n, p, D, T, 3He, 4He 00149 }
| G4double G4BertiniEvaporationChannel::getThresh | ( | ) | [virtual] |
Definition at line 152 of file G4BertiniEvaporationChannel.cc.
References getCoulomb(), and getQ().
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), G4BENeutronChannel::sampleKineticEnergy(), and G4BEChargedChannel::sampleKineticEnergy().
00153 { 00154 G4double threshold = getQ() + getCoulomb(); 00155 return threshold; 00156 }
| void G4BertiniEvaporationChannel::isotropicCosines | ( | G4double & | , | |
| G4double & | , | |||
| G4double & | ||||
| ) | [protected] |
Definition at line 208 of file G4BertiniEvaporationChannel.cc.
References G4UniformRand.
Referenced by G4BETritonChannel::emit(), G4BEProtonChannel::emit(), G4BENeutronChannel::emit(), G4BEHe4Channel::emit(), G4BEHe3Channel::emit(), and G4BEDeuteronChannel::emit().
00209 { 00210 // Samples isotropic random direction cosines. 00211 G4double CosTheta = 1.0 - 2.0 * G4UniformRand(); 00212 G4double SinTheta = std::sqrt( 1.0 - CosTheta * CosTheta ); 00213 G4double Phi = twopi * G4UniformRand(); 00214 00215 u = std::cos( Phi ) * SinTheta; 00216 v = std::cos( Phi ) * CosTheta, 00217 w = std::sin( Phi ); 00218 00219 return; 00220 }
Definition at line 261 of file G4BertiniEvaporationChannel.cc.
Referenced by setPairingCorrection().
00262 { 00263 // Pairing energy for neutrons P(N), see 00264 // Cameron, Nuclear Level Spacings, p. 1040 00265 // Canadian Journal of Physics, vol 36, 1958 00266 G4double table[200] = { 00267 0.00000000E+00, 0.59799995E+01, 0.00000000E+00, 0.27699995E+01, 0.00000000E+00, 00268 0.31599998E+01, 0.00000000E+00, 0.30099993E+01, 0.00000000E+00, 0.16799994E+01, 00269 0.00000000E+00, 0.17299995E+01, 0.00000000E+00, 0.21699991E+01, 0.00000000E+00, 00270 0.17399998E+01, 0.00000000E+00, 0.17500000E+01, 0.00000000E+00, 0.17199993E+01, 00271 0.00000000E+00, 0.16299992E+01, 0.00000000E+00, 0.14099998E+01, 0.00000000E+00, 00272 0.12899990E+01, 0.00000000E+00, 0.14699993E+01, 0.00000000E+00, 0.13199997E+01, 00273 0.00000000E+00, 0.14599991E+01, 0.00000000E+00, 0.14399996E+01, 0.00000000E+00, 00274 0.14599991E+01, 0.00000000E+00, 0.15199995E+01, 0.00000000E+00, 0.15099993E+01, 00275 0.00000000E+00, 0.14699993E+01, 0.00000000E+00, 0.14499998E+01, 0.00000000E+00, 00276 0.12799997E+01, 0.00000000E+00, 0.12299995E+01, 0.00000000E+00, 0.12699995E+01, 00277 0.00000000E+00, 0.61999995E+00, 0.00000000E+00, 0.75999999E+00, 0.00000000E+00, 00278 0.12299995E+01, 0.00000000E+00, 0.12199993E+01, 0.00000000E+00, 0.13999996E+01, 00279 0.00000000E+00, 0.13599997E+01, 0.00000000E+00, 0.12999992E+01, 0.00000000E+00, 00280 0.12899990E+01, 0.00000000E+00, 0.12399998E+01, 0.00000000E+00, 0.12799997E+01, 00281 0.00000000E+00, 0.12399998E+01, 0.00000000E+00, 0.11999998E+01, 0.00000000E+00, 00282 0.94000000E+00, 0.00000000E+00, 0.99999988E+00, 0.00000000E+00, 0.10499992E+01, 00283 0.00000000E+00, 0.53999996E+00, 0.00000000E+00, 0.59999996E+00, 0.00000000E+00, 00284 0.75000000E+00, 0.00000000E+00, 0.75000000E+00, 0.00000000E+00, 0.84999996E+00, 00285 0.00000000E+00, 0.96999997E+00, 0.00000000E+00, 0.10199995E+01, 0.00000000E+00, 00286 0.10499992E+01, 0.00000000E+00, 0.10599995E+01, 0.00000000E+00, 0.10699997E+01, 00287 0.00000000E+00, 0.10599995E+01, 0.00000000E+00, 0.10499992E+01, 0.00000000E+00, 00288 0.10199995E+01, 0.00000000E+00, 0.96999997E+00, 0.00000000E+00, 0.90999997E+00, 00289 0.00000000E+00, 0.82999998E+00, 0.00000000E+00, 0.73999995E+00, 0.00000000E+00, 00290 0.65999997E+00, 0.00000000E+00, 0.60999995E+00, 0.00000000E+00, 0.60999995E+00, 00291 0.00000000E+00, 0.89999998E+00, 0.00000000E+00, 0.51999998E+00, 0.00000000E+00, 00292 0.80999994E+00, 0.00000000E+00, 0.67999995E+00, 0.00000000E+00, 0.71999997E+00, 00293 0.00000000E+00, 0.76999998E+00, 0.00000000E+00, 0.67999995E+00, 0.00000000E+00, 00294 0.66999996E+00, 0.00000000E+00, 0.79999995E+00, 0.00000000E+00, 0.67999995E+00, 00295 0.00000000E+00, 0.63999999E+00, 0.00000000E+00, 0.57999998E+00, 0.00000000E+00, 00296 0.54999995E+00, 0.00000000E+00, 0.56999993E+00, 0.00000000E+00, 0.56999993E+00, 00297 0.00000000E+00, 0.54999995E+00, 0.00000000E+00, 0.59999996E+00, 0.00000000E+00, 00298 0.57999998E+00, 0.00000000E+00, 0.57999998E+00, 0.00000000E+00, 0.60999995E+00, 00299 0.00000000E+00, 0.63000000E+00, 0.00000000E+00, 0.64999998E+00, 0.00000000E+00, 00300 0.65999997E+00, 0.00000000E+00, 0.64999998E+00, 0.00000000E+00, 0.64999998E+00, 00301 0.00000000E+00, 0.63999999E+00, 0.00000000E+00, 0.63999999E+00, 0.00000000E+00, 00302 0.63000000E+00, 0.00000000E+00, 0.60999995E+00, 0.00000000E+00, 0.58999997E+00, 00303 0.00000000E+00, 0.54999995E+00, 0.00000000E+00, 0.38999999E+00, 0.00000000E+00, 00304 0.35999995E+00, 0.00000000E+00, 0.39999998E+00, 0.00000000E+00, 0.39999998E+00, 00305 0.00000000E+00, 0.39999998E+00, 0.00000000E+00, 0.39999998E+00, 0.00000000E+00, 00306 0.39999998E+00, 0.00000000E+00, 0.39999998E+00, 0.00000000E+00, 0.39999998E+00 00307 }; 00308 if ( N > 200 ) throw G4HadronicException(__FILE__, __LINE__, " G4BertiniEvaporationChannel: pairing energy for neutrons called with too large Z " ); 00309 return table[ N-1 ]*MeV; 00310 }
Definition at line 223 of file G4BertiniEvaporationChannel.cc.
Referenced by setPairingCorrection().
00224 { 00225 // Pairing energy for protons P(Z), see 00226 // Cameron, Nuclear Level Spacings, p. 1040 00227 // Canadian Journal of Physics, vol 36, 1958 00228 G4double table [130] = { 00229 0.00000000E+00, 0.54399996E+01, 0.00000000E+00, 0.27599993E+01, 0.00000000E+00, 00230 0.33399992E+01, 0.00000000E+00, 0.26999998E+01, 0.00000000E+00, 0.18999996E+01, 00231 0.00000000E+00, 0.21199999E+01, 0.00000000E+00, 0.21299992E+01, 0.00000000E+00, 00232 0.15399990E+01, 0.00000000E+00, 0.14199991E+01, 0.00000000E+00, 0.15099993E+01, 00233 0.00000000E+00, 0.17299995E+01, 0.00000000E+00, 0.14399996E+01, 0.00000000E+00, 00234 0.14499998E+01, 0.00000000E+00, 0.13699999E+01, 0.00000000E+00, 0.10899992E+01, 00235 0.00000000E+00, 0.13599997E+01, 0.00000000E+00, 0.14199991E+01, 0.00000000E+00, 00236 0.13299990E+01, 0.00000000E+00, 0.11999998E+01, 0.00000000E+00, 0.99999988E+00, 00237 0.00000000E+00, 0.11599998E+01, 0.00000000E+00, 0.12799997E+01, 0.00000000E+00, 00238 0.13799992E+01, 0.00000000E+00, 0.13799992E+01, 0.00000000E+00, 0.13199997E+01, 00239 0.00000000E+00, 0.10399990E+01, 0.00000000E+00, 0.11099997E+01, 0.00000000E+00, 00240 0.11299992E+01, 0.00000000E+00, 0.12099991E+01, 0.00000000E+00, 0.14299994E+01, 00241 0.00000000E+00, 0.11499996E+01, 0.00000000E+00, 0.98999995E+00, 0.00000000E+00, 00242 0.90999997E+00, 0.00000000E+00, 0.91999996E+00, 0.00000000E+00, 0.99999988E+00, 00243 0.00000000E+00, 0.11099997E+01, 0.00000000E+00, 0.12299995E+01, 0.00000000E+00, 00244 0.84999996E+00, 0.00000000E+00, 0.97999996E+00, 0.00000000E+00, 0.71999997E+00, 00245 0.00000000E+00, 0.79999995E+00, 0.00000000E+00, 0.76999998E+00, 0.00000000E+00, 00246 0.88999999E+00, 0.00000000E+00, 0.91999996E+00, 0.00000000E+00, 0.79999995E+00, 00247 0.00000000E+00, 0.80999994E+00, 0.00000000E+00, 0.69000000E+00, 0.00000000E+00, 00248 0.69999999E+00, 0.00000000E+00, 0.75999999E+00, 0.00000000E+00, 0.72999996E+00, 00249 0.00000000E+00, 0.79999995E+00, 0.00000000E+00, 0.73999995E+00, 0.00000000E+00, 00250 0.72999996E+00, 0.00000000E+00, 0.71999997E+00, 0.00000000E+00, 0.71999997E+00, 00251 0.00000000E+00, 0.71999997E+00, 0.00000000E+00, 0.70999998E+00, 0.00000000E+00, 00252 0.69000000E+00, 0.00000000E+00, 0.67999995E+00, 0.00000000E+00, 0.65999997E+00, 00253 0.00000000E+00, 0.60999995E+00, 0.00000000E+00, 0.41999996E+00, 0.00000000E+00, 00254 0.35999995E+00, 0.00000000E+00, 0.40999997E+00, 0.00000000E+00, 0.48999995E+00 00255 }; 00256 if ( Z>130 ) throw G4HadronicException(__FILE__, __LINE__, " G4BertiniEvaporationChannel: pairing energy for protons called with too large Z " ); 00257 return table[ Z-1 ]*MeV; 00258 }
| G4double G4BertiniEvaporationChannel::qmFactor | ( | ) | [virtual] |
Reimplemented in G4BEDeuteronChannel, G4BEHe3Channel, G4BEHe4Channel, G4BEProtonChannel, and G4BETritonChannel.
Definition at line 183 of file G4BertiniEvaporationChannel.cc.
Referenced by G4BEChargedChannel::calculateProbability(), and getCoulomb().
00184 { 00185 // Coefficient k_p for empirical cross section 00186 // formula presented in Dostrovsky, Phys. Rev., 00187 // vol. 116, 1959 00188 return 0; 00189 }
| void G4BertiniEvaporationChannel::setExcitationEnergy | ( | G4double | inputE | ) |
Definition at line 87 of file G4BertiniEvaporationChannel.cc.
References excitationEnergy.
00088 { 00089 excitationEnergy = energy; 00090 }
| void G4BertiniEvaporationChannel::setNucleusA | ( | G4int | inputA | ) |
Definition at line 63 of file G4BertiniEvaporationChannel.cc.
References nucleusA.
00064 { 00065 nucleusA = a; 00066 }
| void G4BertiniEvaporationChannel::setNucleusZ | ( | G4int | inputZ | ) |
Definition at line 69 of file G4BertiniEvaporationChannel.cc.
References nucleusZ.
00070 { 00071 nucleusZ = z; 00072 }
| void G4BertiniEvaporationChannel::setPairingCorrection | ( | G4int | isCorrection | ) |
Definition at line 93 of file G4BertiniEvaporationChannel.cc.
References correction, nucleusA, nucleusZ, pairingEnergyNeutrons(), pairingEnergyProtons(), particleA, and particleZ.
00094 { 00095 G4int residualZ = nucleusZ - particleZ; 00096 G4int residualA = nucleusA - particleA; 00097 00098 // Note: pairing energy is zero for odd nucleon number. 00099 00100 if ( isCorrection ) correction = pairingEnergyProtons( residualZ ) 00101 + pairingEnergyNeutrons( residualA - residualZ ); 00102 else correction = 0; 00103 }
| void G4BertiniEvaporationChannel::setProbability | ( | G4double | newProb | ) | [virtual] |
Definition at line 122 of file G4BertiniEvaporationChannel.cc.
References emissionProbability.
Referenced by G4BertiniEvaporation::BreakItUp().
00123 { 00124 emissionProbability = newProb; 00125 return; 00126 }
| void G4BertiniEvaporationChannel::setQ | ( | G4double | inputQ | ) |
| void G4BertiniEvaporationChannel::setVerboseLevel | ( | G4int | verbose | ) |
Definition at line 57 of file G4BertiniEvaporationChannel.cc.
References verboseLevel.
00058 { 00059 verboseLevel = level; 00060 }
G4double G4BertiniEvaporationChannel::correction [protected] |
Definition at line 75 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), getCoulomb(), G4BENeutronChannel::sampleKineticEnergy(), G4BEChargedChannel::sampleKineticEnergy(), and setPairingCorrection().
Definition at line 73 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), getProbability(), and setProbability().
Definition at line 76 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), G4BENeutronChannel::sampleKineticEnergy(), G4BEChargedChannel::sampleKineticEnergy(), and setExcitationEnergy().
G4double G4BertiniEvaporationChannel::exmass [protected] |
Definition at line 72 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BEDeuteronChannel::G4BEDeuteronChannel().
G4String G4BertiniEvaporationChannel::name [protected] |
Definition at line 66 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BEDeuteronChannel::G4BEDeuteronChannel(), G4BEHe3Channel::G4BEHe3Channel(), G4BEHe4Channel::G4BEHe4Channel(), G4BENeutronChannel::G4BENeutronChannel(), G4BEProtonChannel::G4BEProtonChannel(), G4BETritonChannel::G4BETritonChannel(), getName(), and getProbability().
G4int G4BertiniEvaporationChannel::nucleusA [protected] |
Definition at line 68 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), getCoulomb(), getLevelDensityParameter(), getQ(), setNucleusA(), and setPairingCorrection().
G4int G4BertiniEvaporationChannel::nucleusZ [protected] |
Definition at line 69 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), G4BEChargedChannel::coulombFactorForProton(), getCoulomb(), getLevelDensityParameter(), getQ(), G4BEChargedChannel::qmFactorForAlpha(), G4BEChargedChannel::qmFactorForProton(), setNucleusZ(), and setPairingCorrection().
G4int G4BertiniEvaporationChannel::particleA [protected] |
Definition at line 70 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), G4BEDeuteronChannel::G4BEDeuteronChannel(), G4BEHe3Channel::G4BEHe3Channel(), G4BEHe4Channel::G4BEHe4Channel(), G4BENeutronChannel::G4BENeutronChannel(), G4BEProtonChannel::G4BEProtonChannel(), G4BETritonChannel::G4BETritonChannel(), getCoulomb(), getLevelDensityParameter(), getParticleA(), getQ(), and setPairingCorrection().
G4int G4BertiniEvaporationChannel::particleZ [protected] |
Definition at line 71 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), G4BEChargedChannel::coulombFactorForProton(), G4BEDeuteronChannel::G4BEDeuteronChannel(), G4BEHe3Channel::G4BEHe3Channel(), G4BEHe4Channel::G4BEHe4Channel(), G4BENeutronChannel::G4BENeutronChannel(), G4BEProtonChannel::G4BEProtonChannel(), G4BETritonChannel::G4BETritonChannel(), getCoulomb(), getLevelDensityParameter(), getParticleZ(), getQ(), G4BEChargedChannel::qmFactorForAlpha(), G4BEChargedChannel::qmFactorForProton(), and setPairingCorrection().
G4double G4BertiniEvaporationChannel::rho [protected] |
Definition at line 74 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BEDeuteronChannel::G4BEDeuteronChannel(), G4BEHe3Channel::G4BEHe3Channel(), G4BEHe4Channel::G4BEHe4Channel(), G4BENeutronChannel::G4BENeutronChannel(), G4BEProtonChannel::G4BEProtonChannel(), G4BETritonChannel::G4BETritonChannel(), and getCoulomb().
G4int G4BertiniEvaporationChannel::spin [protected] |
G4int G4BertiniEvaporationChannel::verboseLevel [protected] |
Definition at line 67 of file G4BertiniEvaporationChannel.hh.
Referenced by G4BENeutronChannel::calculateProbability(), G4BEChargedChannel::calculateProbability(), G4BEChargedChannel::G4BEChargedChannel(), G4BEDeuteronChannel::G4BEDeuteronChannel(), G4BEHe3Channel::G4BEHe3Channel(), G4BEHe4Channel::G4BEHe4Channel(), G4BENeutronChannel::G4BENeutronChannel(), G4BEProtonChannel::G4BEProtonChannel(), G4BertiniEvaporationChannel(), G4BETritonChannel::G4BETritonChannel(), getCoulomb(), getProbability(), G4BENeutronChannel::sampleKineticEnergy(), G4BEChargedChannel::sampleKineticEnergy(), and setVerboseLevel().
1.4.7