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26 ////////////////////////////////////////////// 26 ////////////////////////////////////////////////////////////////////////////////
27 // 27 // //
28 // File: G4ECDecay.cc 28 // File: G4ECDecay.cc //
29 // Author: D.H. Wright (SLAC) 29 // Author: D.H. Wright (SLAC) //
30 // Date: 25 November 2014 30 // Date: 25 November 2014 //
31 // 31 // //
32 ////////////////////////////////////////////// 32 ////////////////////////////////////////////////////////////////////////////////
33 33
34 #include "G4ECDecay.hh" 34 #include "G4ECDecay.hh"
35 #include "G4IonTable.hh" 35 #include "G4IonTable.hh"
36 #include "Randomize.hh" 36 #include "Randomize.hh"
37 #include "G4ThreeVector.hh" 37 #include "G4ThreeVector.hh"
38 #include "G4DynamicParticle.hh" 38 #include "G4DynamicParticle.hh"
39 #include "G4DecayProducts.hh" 39 #include "G4DecayProducts.hh"
40 #include "G4VAtomDeexcitation.hh" 40 #include "G4VAtomDeexcitation.hh"
41 #include "G4AtomicShells.hh" 41 #include "G4AtomicShells.hh"
42 #include "G4Electron.hh" 42 #include "G4Electron.hh"
43 #include "G4LossTableManager.hh" 43 #include "G4LossTableManager.hh"
44 #include "G4PhysicalConstants.hh" 44 #include "G4PhysicalConstants.hh"
45 #include "G4SystemOfUnits.hh" 45 #include "G4SystemOfUnits.hh"
46 46
47 G4ECDecay::G4ECDecay(const G4ParticleDefinitio 47 G4ECDecay::G4ECDecay(const G4ParticleDefinition* theParentNucleus,
48 const G4double& branch, c 48 const G4double& branch, const G4double& Qvalue,
49 const G4double& excitatio 49 const G4double& excitationE,
50 const G4Ions::G4FloatLeve 50 const G4Ions::G4FloatLevelBase& flb,
51 const G4RadioactiveDecayM 51 const G4RadioactiveDecayMode& mode)
52 : G4NuclearDecay("electron capture", mode, ex 52 : G4NuclearDecay("electron capture", mode, excitationE, flb), transitionQ(Qvalue),
53 applyARM(true) 53 applyARM(true)
54 { 54 {
55 SetParent(theParentNucleus); // Store name 55 SetParent(theParentNucleus); // Store name of parent nucleus, delete G4MT_parent
56 SetBR(branch); 56 SetBR(branch);
57 57
58 SetNumberOfDaughters(2); 58 SetNumberOfDaughters(2);
59 G4IonTable* theIonTable = 59 G4IonTable* theIonTable =
60 (G4IonTable*)(G4ParticleTable::GetParticle 60 (G4IonTable*)(G4ParticleTable::GetParticleTable()->GetIonTable());
61 G4int daughterZ = theParentNucleus->GetAtomi 61 G4int daughterZ = theParentNucleus->GetAtomicNumber() - 1;
62 G4int daughterA = theParentNucleus->GetAtomi 62 G4int daughterA = theParentNucleus->GetAtomicMass();
63 SetDaughter(0, theIonTable->GetIon(daughterZ 63 SetDaughter(0, theIonTable->GetIon(daughterZ, daughterA, excitationE, flb) );
64 SetDaughter(1, "nu_e"); 64 SetDaughter(1, "nu_e");
65 DefineSubshellProbabilities(daughterZ, daugh 65 DefineSubshellProbabilities(daughterZ, daughterZ);
66 } 66 }
67 67
68 68
69 G4ECDecay::~G4ECDecay() 69 G4ECDecay::~G4ECDecay()
70 {} 70 {}
71 71
72 72
73 G4DecayProducts* G4ECDecay::DecayIt(G4double) 73 G4DecayProducts* G4ECDecay::DecayIt(G4double)
74 { 74 {
75 // Fill G4MT_parent with theParentNucleus (s 75 // Fill G4MT_parent with theParentNucleus (stored by SetParent in ctor)
76 CheckAndFillParent(); 76 CheckAndFillParent();
77 77
78 // Fill G4MT_daughters with alpha and residu 78 // Fill G4MT_daughters with alpha and residual nucleus (stored by SetDaughter)
79 CheckAndFillDaughters(); 79 CheckAndFillDaughters();
80 80
81 // Get shell number of captured electron 81 // Get shell number of captured electron
82 G4int shellIndex = -1; 82 G4int shellIndex = -1;
83 G4double ran; 83 G4double ran;
84 switch (theMode) 84 switch (theMode)
85 { 85 {
86 case KshellEC: 86 case KshellEC:
87 shellIndex = 0; 87 shellIndex = 0;
88 break; 88 break;
89 case LshellEC: // PL1+PL2+PL3=1 89 case LshellEC: // PL1+PL2+PL3=1
90 ran=G4UniformRand(); 90 ran=G4UniformRand();
91 if (ran <= PL1) shellIndex =1; 91 if (ran <= PL1) shellIndex =1;
92 else if (ran<= (PL1+PL2)) shellIndex =2; 92 else if (ran<= (PL1+PL2)) shellIndex =2;
93 else shellIndex =3; 93 else shellIndex =3;
94 break; 94 break;
95 case MshellEC: // PM1+PM2+PM3=1 95 case MshellEC: // PM1+PM2+PM3=1
96 ran=G4UniformRand(); 96 ran=G4UniformRand();
97 if (ran < PM1) shellIndex =4; 97 if (ran < PM1) shellIndex =4;
98 else if (ran< (PM1+PM2)) shellIndex =5; 98 else if (ran< (PM1+PM2)) shellIndex =5;
99 else shellIndex = 6; 99 else shellIndex = 6;
100 break; 100 break;
101 case NshellEC: // PN1+PN2+PN3=1 101 case NshellEC: // PN1+PN2+PN3=1
102 ran=G4UniformRand(); 102 ran=G4UniformRand();
103 if (ran < PN1) shellIndex = 9; 103 if (ran < PN1) shellIndex = 9;
104 else if (ran<= (PN1+PN2)) shellIndex =2; 104 else if (ran<= (PN1+PN2)) shellIndex =2;
105 else shellIndex =10; 105 else shellIndex =10;
106 break; 106 break;
107 default: 107 default:
108 G4Exception("G4ECDecay::DecayIt()", "HAD 108 G4Exception("G4ECDecay::DecayIt()", "HAD_RDM_009",
109 FatalException, "Invalid ele 109 FatalException, "Invalid electron shell selected");
110 } 110 }
111 111
112 // Initialize decay products with parent nuc 112 // Initialize decay products with parent nucleus at rest
113 G4DynamicParticle parentParticle(G4MT_parent 113 G4DynamicParticle parentParticle(G4MT_parent, G4ThreeVector(0,0,0), 0.0);
114 G4DecayProducts* products = new G4DecayProdu 114 G4DecayProducts* products = new G4DecayProducts(parentParticle);
115 G4double eBind = 0.0; 115 G4double eBind = 0.0;
116 116
117 // G4LossTableManager must already be initia 117 // G4LossTableManager must already be initialized with G4UAtomicDeexcitation
118 // This is currently done in G4RadioactiveDe 118 // This is currently done in G4RadioactiveDecay::BuildPhysicsTable
119 G4VAtomDeexcitation* atomDeex = 119 G4VAtomDeexcitation* atomDeex =
120 G4LossTableManager::Instance()->Atom 120 G4LossTableManager::Instance()->AtomDeexcitation();
121 std::vector<G4DynamicParticle*> armProducts; 121 std::vector<G4DynamicParticle*> armProducts;
122 122
123 if (applyARM) { 123 if (applyARM) {
124 if (nullptr != atomDeex) { 124 if (nullptr != atomDeex) {
125 G4int aZ = G4MT_daughters[0]->GetAtomicN 125 G4int aZ = G4MT_daughters[0]->GetAtomicNumber();
126 G4int nShells = G4AtomicShells::GetNumbe 126 G4int nShells = G4AtomicShells::GetNumberOfShells(aZ);
127 if (shellIndex >= nShells) shellIndex = 127 if (shellIndex >= nShells) shellIndex = nShells;
128 G4AtomicShellEnumerator as = G4AtomicShe 128 G4AtomicShellEnumerator as = G4AtomicShellEnumerator(shellIndex);
129 const G4AtomicShell* shell = atomDeex->G 129 const G4AtomicShell* shell = atomDeex->GetAtomicShell(aZ, as);
130 eBind = shell->BindingEnergy(); 130 eBind = shell->BindingEnergy();
131 if (atomDeex->IsFluoActive() && aZ > 5 & 131 if (atomDeex->IsFluoActive() && aZ > 5 && aZ < 105) {
132 // Do atomic relaxation 132 // Do atomic relaxation
133 // VI, SI 133 // VI, SI
134 // Allows fixing of Bugzilla 1727 134 // Allows fixing of Bugzilla 1727
135 //const G4double deexLimit = 0.1*keV; 135 //const G4double deexLimit = 0.1*keV;
136 G4double deexLimit = 0.1*keV; 136 G4double deexLimit = 0.1*keV;
137 if (G4EmParameters::Instance()->Deexcitation 137 if (G4EmParameters::Instance()->DeexcitationIgnoreCut()) deexLimit = 0.;
138 138
139 atomDeex->GenerateParticles(&armProduc 139 atomDeex->GenerateParticles(&armProducts, shell, aZ, deexLimit, deexLimit);
140 } 140 }
141 141
142 G4double productEnergy = 0.; 142 G4double productEnergy = 0.;
143 for (std::size_t i = 0; i < armProducts. 143 for (std::size_t i = 0; i < armProducts.size(); ++i) {
144 productEnergy += armProducts[i]->GetKi 144 productEnergy += armProducts[i]->GetKineticEnergy();
145 } 145 }
146 G4double deficit = shell->BindingEnergy( 146 G4double deficit = shell->BindingEnergy() - productEnergy;
147 if (deficit > 0.0) { 147 if (deficit > 0.0) {
148 // Add a dummy electron to make up ext 148 // Add a dummy electron to make up extra energy
149 G4double cosTh = 1.-2.*G4UniformRand() 149 G4double cosTh = 1.-2.*G4UniformRand();
150 G4double sinTh = std::sqrt(1.- cosTh*c 150 G4double sinTh = std::sqrt(1.- cosTh*cosTh);
151 G4double phi = twopi*G4UniformRand(); 151 G4double phi = twopi*G4UniformRand();
152 152
153 G4ThreeVector electronDirection(sinTh* 153 G4ThreeVector electronDirection(sinTh*std::sin(phi),
154 sinTh* 154 sinTh*std::cos(phi), cosTh);
155 G4DynamicParticle* extra = 155 G4DynamicParticle* extra =
156 new G4DynamicParticle(G4Electron::El 156 new G4DynamicParticle(G4Electron::Electron(), electronDirection,
157 deficit); 157 deficit);
158 armProducts.push_back(extra); 158 armProducts.push_back(extra);
159 } 159 }
160 } // atomDeex 160 } // atomDeex
161 } // applyARM 161 } // applyARM
162 162
163 G4double daughterMass = G4MT_daughters[0]->G 163 G4double daughterMass = G4MT_daughters[0]->GetPDGMass();
164 164
165 // CM momentum using Q value corrected for b 165 // CM momentum using Q value corrected for binding energy of captured electron
166 G4double Q = transitionQ - eBind; 166 G4double Q = transitionQ - eBind;
167 167
168 // Negative transitionQ values for some rare 168 // Negative transitionQ values for some rare nuclides require this
169 // Absolute values in these cases are small 169 // Absolute values in these cases are small
170 if (Q < 0.0) Q = 0.0; 170 if (Q < 0.0) Q = 0.0;
171 171
172 G4double cmMomentum = Q*(Q + 2.*daughterMass 172 G4double cmMomentum = Q*(Q + 2.*daughterMass)/(Q + daughterMass)/2.;
173 173
174 G4double costheta = 2.*G4UniformRand() - 1.0 174 G4double costheta = 2.*G4UniformRand() - 1.0;
175 G4double sintheta = std::sqrt(1.0 - costheta 175 G4double sintheta = std::sqrt(1.0 - costheta*costheta);
176 G4double phi = twopi*G4UniformRand()*rad; 176 G4double phi = twopi*G4UniformRand()*rad;
177 G4ThreeVector direction(sintheta*std::cos(ph 177 G4ThreeVector direction(sintheta*std::cos(phi),sintheta*std::sin(phi),
178 costheta); 178 costheta);
179 G4double KE = cmMomentum; 179 G4double KE = cmMomentum;
180 G4DynamicParticle* daughterParticle = 180 G4DynamicParticle* daughterParticle =
181 new G4DynamicParticle(G4MT_daughters[1], d 181 new G4DynamicParticle(G4MT_daughters[1], direction, KE, 0.0);
182 products->PushProducts(daughterParticle); 182 products->PushProducts(daughterParticle);
183 183
184 KE = std::sqrt(cmMomentum*cmMomentum + daugh 184 KE = std::sqrt(cmMomentum*cmMomentum + daughterMass*daughterMass) - daughterMass;
185 daughterParticle = 185 daughterParticle =
186 new G4DynamicParticle(G4MT_daughters[0], - 186 new G4DynamicParticle(G4MT_daughters[0], -1.0*direction, KE, daughterMass);
187 products->PushProducts(daughterParticle); 187 products->PushProducts(daughterParticle);
188 188
189 std::size_t nArm = armProducts.size(); 189 std::size_t nArm = armProducts.size();
190 if (nArm > 0) { 190 if (nArm > 0) {
191 G4ThreeVector bst = daughterParticle->Get4 191 G4ThreeVector bst = daughterParticle->Get4Momentum().boostVector();
192 for (std::size_t i = 0; i < nArm; ++i) { 192 for (std::size_t i = 0; i < nArm; ++i) {
193 G4DynamicParticle* dp = armProducts[i]; 193 G4DynamicParticle* dp = armProducts[i];
194 G4LorentzVector lv = dp->Get4Momentum(). 194 G4LorentzVector lv = dp->Get4Momentum().boost(bst);
195 dp->Set4Momentum(lv); 195 dp->Set4Momentum(lv);
196 products->PushProducts(dp); 196 products->PushProducts(dp);
197 } 197 }
198 } 198 }
199 199
200 // Energy conservation check 200 // Energy conservation check
201 /* 201 /*
202 G4int newSize = products->entries(); 202 G4int newSize = products->entries();
203 G4DynamicParticle* temp = 0; 203 G4DynamicParticle* temp = 0;
204 G4double KEsum = 0.0; 204 G4double KEsum = 0.0;
205 for (G4int i = 0; i < newSize; i++) { 205 for (G4int i = 0; i < newSize; i++) {
206 temp = products->operator[](i); 206 temp = products->operator[](i);
207 KEsum += temp->GetKineticEnergy(); 207 KEsum += temp->GetKineticEnergy();
208 } 208 }
209 209
210 G4double eCons = (transitionQ - KEsum)/keV; 210 G4double eCons = (transitionQ - KEsum)/keV;
211 G4cout << " EC check: Ediff (keV) = " << eCo 211 G4cout << " EC check: Ediff (keV) = " << eCons << G4endl;
212 */ 212 */
213 return products; 213 return products;
214 } 214 }
215 215
216 216
217 void G4ECDecay::DumpNuclearInfo() 217 void G4ECDecay::DumpNuclearInfo()
218 { 218 {
219 G4cout << " G4ECDecay of parent nucleus " << 219 G4cout << " G4ECDecay of parent nucleus " << GetParentName() << " from ";
220 if (theMode == 3) { 220 if (theMode == 3) {
221 G4cout << "K shell"; 221 G4cout << "K shell";
222 } else if (theMode == 4) { 222 } else if (theMode == 4) {
223 G4cout << "L shell"; 223 G4cout << "L shell";
224 } else if (theMode == 5) { 224 } else if (theMode == 5) {
225 G4cout << "M shell"; 225 G4cout << "M shell";
226 } 226 }
227 else if (theMode == 6) { 227 else if (theMode == 6) {
228 G4cout << "N shell"; 228 G4cout << "N shell";
229 } 229 }
230 G4cout << G4endl; 230 G4cout << G4endl;
231 G4cout << " to " << GetDaughterName(0) << " 231 G4cout << " to " << GetDaughterName(0) << " + " << GetDaughterName(1)
232 << " with branching ratio " << GetBR( 232 << " with branching ratio " << GetBR() << "% and Q value "
233 << transitionQ << G4endl; 233 << transitionQ << G4endl;
234 } 234 }
235 void G4ECDecay::DefineSubshellProbabilities(G4 235 void G4ECDecay::DefineSubshellProbabilities(G4int Z, G4int )
236 { //Implementation for the case of allowed tra 236 { //Implementation for the case of allowed transitions
237 //PL1+PL2=1. , PM1+PM2=1., PN1+PN2=1. 237 //PL1+PL2=1. , PM1+PM2=1., PN1+PN2=1.
238 PL1 = 1./(1+PL2overPL1[Z-1]); 238 PL1 = 1./(1+PL2overPL1[Z-1]);
239 PL2 = PL1*PL2overPL1[Z-1]; 239 PL2 = PL1*PL2overPL1[Z-1];
240 PM1 = 1./(1+PM2overPM1[Z-1]); 240 PM1 = 1./(1+PM2overPM1[Z-1]);
241 PM2 = PM1*PM2overPM1[Z-1]; 241 PM2 = PM1*PM2overPM1[Z-1];
242 PN1 = 1./(1+PN2overPN1[Z-1]); 242 PN1 = 1./(1+PN2overPN1[Z-1]);
243 PN2 = PN1*PN2overPN1[Z-1]; 243 PN2 = PN1*PN2overPN1[Z-1];
244 } 244 }
245 ////////////////////////////////////////////// 245 ////////////////////////////////////////////////////////////////////////////
246 // Table of subshell ratio probability PL2/PL1 246 // Table of subshell ratio probability PL2/PL1 in function of Z
247 // PL2/PL1 = (fL2/gL1)^2 247 // PL2/PL1 = (fL2/gL1)^2
248 // with gL1 and fL2 the bound electron radial 248 // with gL1 and fL2 the bound electron radial wave amplitudes taken from
249 // Bambynek et al., Rev. Modern Phy 249 // Bambynek et al., Rev. Modern Physics, vol. 49, 1971, table IX
250 // For Z=18 interpolation between Z=17 and Z= 250 // For Z=18 interpolation between Z=17 and Z=19 to avoid a jump in PL2/Pl1
251 ////////////////////////////////////////////// 251 ////////////////////////////////////////////////////////////////////////////
252 const G4double G4ECDecay::PL2overPL1[100] = { 252 const G4double G4ECDecay::PL2overPL1[100] = {
253 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.00 253 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 1.8722e-04,
254 2.6438e-04, 3.5456e-04, 4.5790e-04, 6.15 254 2.6438e-04, 3.5456e-04, 4.5790e-04, 6.1588e-04, 7.8944e-04, 9.8530e-04, 1.2030e-03,
255 1.4361e-03, 1.6886e-03, 1.9609e-03, 2.26 255 1.4361e-03, 1.6886e-03, 1.9609e-03, 2.2641e-03, 2.5674e-03, 2.9019e-03, 3.2577e-03,
256 3.6338e-03, 4.0310e-03, 4.4541e-03, 4.89 256 3.6338e-03, 4.0310e-03, 4.4541e-03, 4.8943e-03, 5.3620e-03, 5.8523e-03, 6.3650e-03,
257 6.9061e-03, 7.4607e-03, 8.0398e-03, 8.64 257 6.9061e-03, 7.4607e-03, 8.0398e-03, 8.6417e-03, 9.2665e-03, 9.9150e-03, 1.0588e-02,
258 1.1284e-02, 1.2004e-02, 1.2744e-02, 1.35 258 1.1284e-02, 1.2004e-02, 1.2744e-02, 1.3518e-02, 1.4312e-02, 1.5136e-02, 1.5981e-02,
259 1.6857e-02, 1.7764e-02, 1.8696e-02, 1.96 259 1.6857e-02, 1.7764e-02, 1.8696e-02, 1.9682e-02, 2.0642e-02, 2.1661e-02, 2.2708e-02,
260 2.3788e-02, 2.4896e-02, 2.6036e-02, 2.72 260 2.3788e-02, 2.4896e-02, 2.6036e-02, 2.7217e-02, 2.8409e-02, 2.9646e-02, 3.0917e-02,
261 3.2220e-02, 3.3561e-02, 3.4937e-02, 3.63 261 3.2220e-02, 3.3561e-02, 3.4937e-02, 3.6353e-02, 3.7805e-02, 3.9297e-02, 4.0826e-02,
262 4.2399e-02, 4.4010e-02, 4.5668e-02, 4.73 262 4.2399e-02, 4.4010e-02, 4.5668e-02, 4.7368e-02, 4.9115e-02, 5.0896e-02, 5.2744e-02,
263 5.4625e-02, 5.6565e-02, 5.8547e-02, 6.05 263 5.4625e-02, 5.6565e-02, 5.8547e-02, 6.0593e-02, 6.2690e-02, 6.4844e-02, 6.7068e-02,
264 6.9336e-02, 7.1667e-02, 7.4075e-02, 7.65 264 6.9336e-02, 7.1667e-02, 7.4075e-02, 7.6544e-02, 7.9085e-02, 8.1688e-02, 8.4371e-02,
265 8.7135e-02, 8.9995e-02, 9.2919e-02, 9.59 265 8.7135e-02, 8.9995e-02, 9.2919e-02, 9.5949e-02, 9.9036e-02, 1.0226e-01, 1.0555e-01,
266 1.0899e-01, 1.1249e-01, 1.1613e-01, 1.19 266 1.0899e-01, 1.1249e-01, 1.1613e-01, 1.1989e-01, 1.2379e-01, 1.2780e-01, 1.3196e-01,
267 1.3627e-01, 1.4071e-01}; 267 1.3627e-01, 1.4071e-01};
268 ////////////////////////////////////////////// 268 ////////////////////////////////////////////////////////////////////////////
269 // Table of subshell ratio probability PM2/PM1 269 // Table of subshell ratio probability PM2/PM1 in function of Z
270 // PM2/PM1 = (fM2/gM1)^2 270 // PM2/PM1 = (fM2/gM1)^2
271 // with gM1 and fM2 the bound electron radial 271 // with gM1 and fM2 the bound electron radial wave amplitudes taken from
272 // Bambynek et al., Rev. Modern Phy 272 // Bambynek et al., Rev. Modern Physics, vol. 49, 1971, table IX
273 ////////////////////////////////////////////// 273 ////////////////////////////////////////////////////////////////////////////
274 const G4double G4ECDecay::PM2overPM1[100] = { 274 const G4double G4ECDecay::PM2overPM1[100] = {
275 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.00 275 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00,
276 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.00 276 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00,
277 1.0210e-03, 1.2641e-03, 1.5231e-03, 1.79 277 1.0210e-03, 1.2641e-03, 1.5231e-03, 1.7990e-03, 2.1938e-03, 2.5863e-03, 2.9621e-03,
278 3.3637e-03, 3.7909e-03, 4.2049e-03, 4.70 278 3.3637e-03, 3.7909e-03, 4.2049e-03, 4.7021e-03, 5.1791e-03, 5.6766e-03, 6.1952e-03,
279 6.7045e-03, 7.2997e-03, 7.9438e-03, 8.62 279 6.7045e-03, 7.2997e-03, 7.9438e-03, 8.6271e-03, 9.3294e-03, 1.0058e-02, 1.0813e-02,
280 1.1594e-02, 1.2408e-02, 1.3244e-02, 1.41 280 1.1594e-02, 1.2408e-02, 1.3244e-02, 1.4118e-02, 1.5023e-02, 1.5962e-02, 1.6919e-02,
281 1.7910e-02, 1.8934e-02, 1.9986e-02, 2.10 281 1.7910e-02, 1.8934e-02, 1.9986e-02, 2.1072e-02, 2.2186e-02, 2.3336e-02, 2.4524e-02,
282 2.5750e-02, 2.7006e-02, 2.8302e-02, 2.96 282 2.5750e-02, 2.7006e-02, 2.8302e-02, 2.9629e-02, 3.0994e-02, 3.2399e-02, 3.3845e-02,
283 3.5328e-02, 3.6852e-02, 3.8414e-02, 4.00 283 3.5328e-02, 3.6852e-02, 3.8414e-02, 4.0025e-02, 4.1673e-02, 4.3368e-02, 4.5123e-02,
284 4.6909e-02, 4.8767e-02, 5.0662e-02, 5.26 284 4.6909e-02, 4.8767e-02, 5.0662e-02, 5.2612e-02, 5.4612e-02, 5.6662e-02, 5.8773e-02,
285 6.0930e-02, 6.3141e-02, 6.5413e-02, 6.77 285 6.0930e-02, 6.3141e-02, 6.5413e-02, 6.7752e-02, 7.0139e-02, 7.2603e-02, 7.5127e-02,
286 7.7721e-02, 8.0408e-02, 8.3128e-02, 8.59 286 7.7721e-02, 8.0408e-02, 8.3128e-02, 8.5949e-02, 8.8843e-02, 9.1824e-02, 9.4888e-02,
287 9.8025e-02, 1.0130e-01, 1.0463e-01, 1.08 287 9.8025e-02, 1.0130e-01, 1.0463e-01, 1.0806e-01, 1.1159e-01, 1.1526e-01, 1.1900e-01,
288 1.2290e-01, 1.2688e-01, 1.3101e-01, 1.35 288 1.2290e-01, 1.2688e-01, 1.3101e-01, 1.3528e-01, 1.3969e-01, 1.4425e-01, 1.4896e-01,
289 1.5384e-01, 1.5887e-01}; 289 1.5384e-01, 1.5887e-01};
290 ////////////////////////////////////////////// 290 ////////////////////////////////////////////////////////////////////////////
291 // Table of subshell ratio probability PN2/PN1 291 // Table of subshell ratio probability PN2/PN1 in function of Z
292 // PN2/PN1 = (fN2/gN1)^2 292 // PN2/PN1 = (fN2/gN1)^2
293 // with gN1 and fN2 are the bound electron rad 293 // with gN1 and fN2 are the bound electron radial wave amplitude taken from
294 // Bambynek et al., Rev. Modern Phy 294 // Bambynek et al., Rev. Modern Physics, vol. 49, 1971, table IX
295 // For Z=44 interpolation between Z=43 and Z= 295 // For Z=44 interpolation between Z=43 and Z=45 to avoid a jump in PN2/PN1
296 ////////////////////////////////////////////// 296 ////////////////////////////////////////////////////////////////////////////
297 const G4double G4ECDecay::PN2overPN1[100] = { 297 const G4double G4ECDecay::PN2overPN1[100] = {
298 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.00 298 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00,
299 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.00 299 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00,
300 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.00 300 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00,
301 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.00 301 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00,
302 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.00 302 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00, 0.0000e+00,
303 0.0000e+00, 9.6988e-03, 1.0797e-02, 1.17 303 0.0000e+00, 9.6988e-03, 1.0797e-02, 1.1706e-02, 1.2603e-02, 1.3408e-02, 1.4352e-02,
304 1.5511e-02, 1.6579e-02, 1.7646e-02, 1.87 304 1.5511e-02, 1.6579e-02, 1.7646e-02, 1.8731e-02, 1.9886e-02, 2.1069e-02, 2.2359e-02,
305 2.3710e-02, 2.5058e-02, 2.6438e-02, 2.78 305 2.3710e-02, 2.5058e-02, 2.6438e-02, 2.7843e-02, 2.9283e-02, 3.0762e-02, 3.2275e-02,
306 3.3843e-02, 3.5377e-02, 3.6886e-02, 3.85 306 3.3843e-02, 3.5377e-02, 3.6886e-02, 3.8502e-02, 4.0159e-02, 4.1867e-02, 4.3617e-02,
307 4.5470e-02, 4.7247e-02, 4.9138e-02, 5.10 307 4.5470e-02, 4.7247e-02, 4.9138e-02, 5.1065e-02, 5.3049e-02, 5.5085e-02, 5.7173e-02,
308 5.9366e-02, 6.1800e-02, 6.3945e-02, 6.63 308 5.9366e-02, 6.1800e-02, 6.3945e-02, 6.6333e-02, 6.8785e-02, 7.1303e-02, 7.3801e-02,
309 7.6538e-02, 7.9276e-02, 8.2070e-02, 8.49 309 7.6538e-02, 7.9276e-02, 8.2070e-02, 8.4959e-02, 8.7940e-02, 9.0990e-02, 9.4124e-02,
310 9.7337e-02, 1.0069e-01, 1.0410e-01, 1.07 310 9.7337e-02, 1.0069e-01, 1.0410e-01, 1.0761e-01, 1.1122e-01, 1.1499e-01, 1.1882e-01,
311 1.2282e-01, 1.2709e-01, 1.3114e-01, 1.35 311 1.2282e-01, 1.2709e-01, 1.3114e-01, 1.3549e-01, 1.4001e-01, 1.4465e-01, 1.4946e-01,
312 1.5443e-01, 1.5954e-01}; 312 1.5443e-01, 1.5954e-01};
313 313
314 314