1 | // |
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2 | // ******************************************************************** |
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3 | // * License and Disclaimer * |
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4 | // * * |
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5 | // * The Geant4 software is copyright of the Copyright Holders of * |
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6 | // * the Geant4 Collaboration. It is provided under the terms and * |
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7 | // * conditions of the Geant4 Software License, included in the file * |
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8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
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9 | // * include a list of copyright holders. * |
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10 | // * * |
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11 | // * Neither the authors of this software system, nor their employing * |
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12 | // * institutes,nor the agencies providing financial support for this * |
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13 | // * work make any representation or warranty, express or implied, * |
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14 | // * regarding this software system or assume any liability for its * |
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15 | // * use. Please see the license in the file LICENSE and URL above * |
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16 | // * for the full disclaimer and the limitation of liability. * |
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17 | // * * |
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18 | // * This code implementation is the result of the scientific and * |
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19 | // * technical work of the GEANT4 collaboration. * |
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20 | // * By using, copying, modifying or distributing the software (or * |
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21 | // * any work based on the software) you agree to acknowledge its * |
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22 | // * use in resulting scientific publications, and indicate your * |
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23 | // * acceptance of all terms of the Geant4 Software license. * |
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24 | // ******************************************************************** |
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25 | // |
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26 | // |
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27 | // $Id: G4ExcitedNucleonConstructor.cc,v 1.11 2006/06/29 19:27:08 gunter Exp $ |
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28 | // GEANT4 tag $Name: geant4-09-02-ref-02 $ |
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29 | // |
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30 | // |
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31 | // -------------------------------------------------------------- |
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32 | // GEANT 4 class implementation file |
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33 | // History: first implementation, based on object model of |
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34 | // 10 oct 1998 H.Kurashige |
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35 | // --------------------------------------------------------------- |
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36 | |
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37 | |
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38 | #include "G4ExcitedNucleonConstructor.hh" |
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39 | |
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40 | #include "G4ParticleDefinition.hh" |
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41 | #include "G4ParticleTable.hh" |
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42 | #include "G4ShortLivedTable.hh" |
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43 | #include "G4PhaseSpaceDecayChannel.hh" |
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44 | #include "G4VDecayChannel.hh" |
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45 | #include "G4DecayTable.hh" |
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46 | |
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47 | |
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48 | G4ExcitedNucleonConstructor::G4ExcitedNucleonConstructor(): |
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49 | G4ExcitedBaryonConstructor(NStates, NucleonIsoSpin) |
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50 | { |
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51 | |
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52 | } |
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53 | |
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54 | G4ExcitedNucleonConstructor::~G4ExcitedNucleonConstructor() |
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55 | { |
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56 | } |
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57 | |
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58 | G4int G4ExcitedNucleonConstructor::GetEncoding(G4int iIsoSpin3, G4int idxState) |
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59 | { |
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60 | G4int encoding; |
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61 | // Delta has exceptinal encoding |
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62 | if ((idxState==1)||(idxState==6)||(idxState==8)||(idxState==9)||(idxState==12) ) { |
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63 | encoding = GetEncodingOffset(idxState); |
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64 | if ((iIsoSpin3==3)||(iIsoSpin3==-3)) { |
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65 | // normal encoding |
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66 | encoding += 1000*GetQuarkContents(0, iIsoSpin3); |
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67 | encoding += 100*GetQuarkContents(1, iIsoSpin3); |
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68 | encoding += 10*GetQuarkContents(2, iIsoSpin3); |
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69 | } else if (iIsoSpin3== +1){ |
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70 | // 1st <--> 2nd quark |
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71 | encoding += 1000*GetQuarkContents(0, iIsoSpin3); |
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72 | encoding += 10*GetQuarkContents(1, iIsoSpin3); |
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73 | encoding += 100*GetQuarkContents(2, iIsoSpin3); |
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74 | } else if (iIsoSpin3== -1){ |
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75 | // 1st <--> 0th quark |
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76 | encoding += 100*GetQuarkContents(0, iIsoSpin3); |
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77 | encoding += 1000*GetQuarkContents(1, iIsoSpin3); |
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78 | encoding += 10*GetQuarkContents(2, iIsoSpin3); |
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79 | } |
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80 | encoding += GetiSpin(idxState) +1; |
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81 | } else { |
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82 | encoding = G4ExcitedBaryonConstructor::GetEncoding(iIsoSpin3, idxState); |
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83 | } |
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84 | return encoding; |
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85 | } |
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86 | |
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87 | G4DecayTable* G4ExcitedNucleonConstructor::CreateDecayTable( |
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88 | const G4String& parentName, |
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89 | G4int iIso3, |
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90 | G4int iState, |
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91 | G4bool fAnti) |
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92 | { |
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93 | // create decay table |
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94 | G4DecayTable* decayTable = new G4DecayTable(); |
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95 | |
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96 | G4double br; |
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97 | if ( (br=bRatio[iState][NGamma]) >0.0) { |
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98 | AddNGammaMode( decayTable, parentName, br, iIso3, fAnti); |
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99 | } |
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100 | |
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101 | if ( (br=bRatio[iState][NPi]) >0.0) { |
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102 | AddNPiMode( decayTable, parentName, br, iIso3, fAnti); |
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103 | } |
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104 | |
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105 | if ( (br=bRatio[iState][NEta]) >0.0) { |
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106 | AddNEtaMode( decayTable, parentName, br, iIso3, fAnti); |
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107 | } |
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108 | |
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109 | if ( (br=bRatio[iState][NOmega]) >0.0) { |
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110 | AddNOmegaMode( decayTable, parentName, br, iIso3, fAnti); |
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111 | } |
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112 | |
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113 | if ( (br=bRatio[iState][NRho]) >0.0) { |
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114 | AddNRhoMode( decayTable, parentName, br, iIso3, fAnti); |
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115 | } |
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116 | |
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117 | if ( (br=bRatio[iState][N2Pi]) >0.0) { |
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118 | AddN2PiMode( decayTable, parentName, br, iIso3, fAnti); |
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119 | } |
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120 | |
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121 | if ( (br=bRatio[iState][DeltaPi]) >0.0) { |
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122 | AddDeltaPiMode( decayTable, parentName, br, iIso3, fAnti); |
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123 | } |
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124 | |
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125 | if ( (br=bRatio[iState][NStarPi]) >0.0) { |
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126 | AddNStarPiMode( decayTable, parentName, br, iIso3, fAnti); |
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127 | } |
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128 | |
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129 | if ( (br=bRatio[iState][LambdaK]) >0.0) { |
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130 | AddLambdaKMode( decayTable, parentName, br, iIso3, fAnti); |
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131 | } |
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132 | |
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133 | return decayTable; |
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134 | } |
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135 | |
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136 | G4DecayTable* G4ExcitedNucleonConstructor::AddNGammaMode( |
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137 | G4DecayTable* decayTable, const G4String& nameParent, |
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138 | G4double br, G4int iIso3, G4bool fAnti) |
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139 | { |
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140 | G4VDecayChannel* mode; |
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141 | |
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142 | // |
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143 | G4String daughterN; |
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144 | if (iIso3 == +1) { |
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145 | daughterN = "proton"; |
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146 | } else { |
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147 | daughterN = "neutron"; |
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148 | } |
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149 | if (fAnti) daughterN = "anti_" + daughterN; |
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150 | |
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151 | // create decay channel [parent BR #daughters] |
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152 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2, |
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153 | daughterN,"gamma"); |
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154 | // add decay table |
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155 | decayTable->Insert(mode); |
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156 | |
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157 | return decayTable; |
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158 | } |
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159 | |
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160 | G4DecayTable* G4ExcitedNucleonConstructor::AddNPiMode( |
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161 | G4DecayTable* decayTable, const G4String& nameParent, |
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162 | G4double br, G4int iIso3, G4bool fAnti) |
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163 | { |
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164 | G4VDecayChannel* mode; |
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165 | |
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166 | G4String daughterN; |
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167 | G4String daughterPi; |
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168 | |
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169 | // ------------ N pi0 ------------ |
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170 | // determine daughters |
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171 | if (iIso3 == +1) { |
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172 | daughterN = "proton"; |
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173 | daughterPi = "pi0"; |
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174 | } else { |
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175 | daughterN = "neutron"; |
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176 | daughterPi = "pi0"; |
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177 | } |
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178 | if (fAnti) daughterN = "anti_" + daughterN; |
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179 | // create decay channel [parent BR #daughters] |
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180 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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181 | daughterN,daughterPi); |
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182 | // add decay table |
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183 | decayTable->Insert(mode); |
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184 | |
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185 | // -------------N pi +/- -------------- |
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186 | // determine daughters |
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187 | if (iIso3 == +1) { |
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188 | daughterN = "neutron"; |
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189 | if (!fAnti) { |
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190 | daughterPi = "pi+"; |
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191 | } else { |
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192 | daughterPi = "pi-"; |
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193 | } |
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194 | } else { |
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195 | daughterN = "proton"; |
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196 | if (!fAnti) { |
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197 | daughterPi = "pi-"; |
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198 | } else { |
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199 | daughterPi = "pi+"; |
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200 | } |
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201 | } |
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202 | if (fAnti) daughterN = "anti_" + daughterN; |
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203 | |
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204 | // create decay channel [parent BR #daughters] |
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205 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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206 | daughterN,daughterPi); |
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207 | // add decay table |
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208 | decayTable->Insert(mode); |
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209 | |
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210 | return decayTable; |
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211 | } |
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212 | |
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213 | G4DecayTable* G4ExcitedNucleonConstructor::AddNEtaMode( |
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214 | G4DecayTable* decayTable, const G4String& nameParent, |
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215 | G4double br, G4int iIso3, G4bool fAnti) |
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216 | { |
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217 | G4VDecayChannel* mode; |
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218 | |
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219 | G4String daughterN; |
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220 | |
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221 | // ------------ N eta------------ |
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222 | // determine daughters |
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223 | if (iIso3 == +1) { |
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224 | daughterN = "proton"; |
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225 | } else { |
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226 | daughterN = "neutron"; |
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227 | } |
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228 | if (fAnti) daughterN = "anti_" + daughterN; |
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229 | // create decay channel [parent BR #daughters] |
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230 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2, |
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231 | daughterN, "eta"); |
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232 | // add decay table |
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233 | decayTable->Insert(mode); |
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234 | |
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235 | return decayTable; |
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236 | } |
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237 | |
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238 | G4DecayTable* G4ExcitedNucleonConstructor::AddNOmegaMode( |
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239 | G4DecayTable* decayTable, const G4String& nameParent, |
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240 | G4double br, G4int iIso3, G4bool fAnti) |
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241 | { |
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242 | G4VDecayChannel* mode; |
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243 | |
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244 | G4String daughterN; |
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245 | |
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246 | // ------------ N omega------------ |
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247 | // determine daughters |
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248 | if (iIso3 == +1) { |
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249 | daughterN = "proton"; |
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250 | } else { |
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251 | daughterN = "neutron"; |
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252 | } |
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253 | if (fAnti) daughterN = "anti_" + daughterN; |
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254 | // create decay channel [parent BR #daughters] |
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255 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2, |
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256 | daughterN, "omega"); |
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257 | // add decay table |
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258 | decayTable->Insert(mode); |
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259 | |
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260 | return decayTable; |
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261 | } |
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262 | |
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263 | G4DecayTable* G4ExcitedNucleonConstructor::AddNRhoMode( |
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264 | G4DecayTable* decayTable, const G4String& nameParent, |
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265 | G4double br, G4int iIso3, G4bool fAnti) |
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266 | { |
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267 | G4VDecayChannel* mode; |
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268 | |
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269 | G4String daughterN; |
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270 | G4String daughterRho; |
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271 | |
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272 | // ------------ N rho0 ------------ |
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273 | // determine daughters |
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274 | if (iIso3 == +1) { |
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275 | daughterN = "proton"; |
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276 | daughterRho = "rho0"; |
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277 | } else { |
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278 | daughterN = "neutron"; |
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279 | daughterRho = "rho0"; |
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280 | } |
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281 | if (fAnti) daughterN = "anti_" + daughterN; |
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282 | // create decay channel [parent BR #daughters] |
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283 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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284 | daughterN,daughterRho); |
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285 | // add decay table |
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286 | decayTable->Insert(mode); |
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287 | |
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288 | // -------------N rho+/- -------------- |
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289 | // determine daughters |
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290 | if (iIso3 == +1) { |
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291 | daughterN = "neutron"; |
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292 | if (!fAnti) { |
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293 | daughterRho = "rho+"; |
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294 | } else { |
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295 | daughterRho = "rho-"; |
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296 | } |
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297 | } else { |
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298 | daughterN = "proton"; |
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299 | if (!fAnti) { |
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300 | daughterRho = "rho-"; |
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301 | } else { |
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302 | daughterRho = "rho+"; |
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303 | } |
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304 | } |
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305 | if (fAnti) daughterN = "anti_" + daughterN; |
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306 | |
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307 | // create decay channel [parent BR #daughters] |
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308 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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309 | daughterN,daughterRho); |
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310 | // add decay table |
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311 | decayTable->Insert(mode); |
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312 | |
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313 | return decayTable; |
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314 | } |
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315 | |
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316 | G4DecayTable* G4ExcitedNucleonConstructor::AddN2PiMode( |
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317 | G4DecayTable* decayTable, const G4String& nameParent, |
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318 | G4double br, G4int iIso3, G4bool fAnti) |
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319 | { |
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320 | // Decay Modes |
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321 | // N* --> N + pi + pi |
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322 | // Only I=0 states are included for 2-pi system |
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323 | |
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324 | G4VDecayChannel* mode; |
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325 | |
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326 | G4String daughterN; |
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327 | G4String daughterPi1; |
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328 | G4String daughterPi2; |
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329 | |
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330 | // -------------N pi+ pi- -------------- |
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331 | // determine daughters |
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332 | if (iIso3 == +1) { |
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333 | daughterN = "proton"; |
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334 | daughterPi1 = "pi+"; |
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335 | daughterPi2 = "pi-"; |
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336 | } else { |
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337 | daughterN = "neutron"; |
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338 | daughterPi1 = "pi+"; |
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339 | daughterPi2 = "pi-"; |
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340 | } |
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341 | if (fAnti) daughterN = "anti_" + daughterN; |
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342 | |
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343 | // create decay channel [parent BR #daughters] |
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344 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 3, |
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345 | daughterN,daughterPi1,daughterPi2); |
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346 | // add decay table |
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347 | decayTable->Insert(mode); |
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348 | |
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349 | // -------------N pi0 pi0 -------------- |
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350 | // determine daughters |
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351 | if (iIso3 == +1) { |
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352 | daughterN = "proton"; |
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353 | daughterPi1 = "pi0"; |
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354 | daughterPi2 = "pi0"; |
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355 | } else { |
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356 | daughterN = "neutron"; |
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357 | daughterPi1 = "pi0"; |
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358 | daughterPi2 = "pi0"; |
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359 | } |
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360 | if (fAnti) daughterN = "anti_" + daughterN; |
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361 | |
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362 | // create decay channel [parent BR #daughters] |
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363 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 3, |
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364 | daughterN,daughterPi1,daughterPi2); |
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365 | // add decay table |
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366 | decayTable->Insert(mode); |
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367 | |
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368 | return decayTable; |
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369 | } |
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370 | |
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371 | G4DecayTable* G4ExcitedNucleonConstructor::AddNStarPiMode( |
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372 | G4DecayTable* decayTable, const G4String& nameParent, |
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373 | G4double br, G4int iIso3, G4bool fAnti) |
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374 | { |
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375 | G4VDecayChannel* mode; |
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376 | |
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377 | G4String daughterN; |
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378 | G4String daughterPi; |
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379 | |
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380 | // ------------ N pi0 ------------ |
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381 | // determine daughters |
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382 | if (iIso3 == +1) { |
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383 | daughterN = "N(1440)+"; |
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384 | daughterPi = "pi0"; |
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385 | } else { |
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386 | daughterN = "N(1440)0"; |
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387 | daughterPi = "pi0"; |
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388 | } |
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389 | if (fAnti) daughterN = "anti_" + daughterN; |
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390 | // create decay channel [parent BR #daughters] |
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391 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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392 | daughterN,daughterPi); |
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393 | // add decay table |
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394 | decayTable->Insert(mode); |
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395 | |
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396 | // -------------N pi +/- -------------- |
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397 | // determine daughters |
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398 | if (iIso3 == +1) { |
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399 | daughterN = "N(1440)0"; |
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400 | if (!fAnti) { |
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401 | daughterPi = "pi+"; |
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402 | } else { |
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403 | daughterPi = "pi-"; |
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404 | } |
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405 | } else { |
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406 | daughterN = "N(1440)+"; |
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407 | if (!fAnti) { |
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408 | daughterPi = "pi-"; |
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409 | } else { |
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410 | daughterPi = "pi+"; |
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411 | } |
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412 | } |
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413 | if (fAnti) daughterN = "anti_" + daughterN; |
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414 | |
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415 | // create decay channel [parent BR #daughters] |
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416 | mode = new G4PhaseSpaceDecayChannel(nameParent, br/2.0, 2, |
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417 | daughterN,daughterPi); |
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418 | // add decay table |
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419 | decayTable->Insert(mode); |
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420 | |
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421 | return decayTable; |
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422 | } |
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423 | |
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424 | G4DecayTable* G4ExcitedNucleonConstructor::AddDeltaPiMode( |
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425 | G4DecayTable* decayTable, const G4String& nameParent, |
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426 | G4double br, G4int iIso3, G4bool fAnti) |
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427 | { |
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428 | G4VDecayChannel* mode; |
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429 | |
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430 | G4String daughterDelta; |
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431 | G4String daughterPi; |
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432 | G4double r; |
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433 | |
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434 | // ------------ Delta pi+/- ------------ |
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435 | // determine daughters |
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436 | if (iIso3 == +1) { |
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437 | daughterDelta = "delta0"; |
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438 | if (!fAnti) { |
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439 | daughterPi = "pi+"; |
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440 | } else { |
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441 | daughterPi = "pi-"; |
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442 | } |
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443 | r = br/6.0; |
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444 | } else { |
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445 | daughterDelta = "delta+"; |
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446 | if (!fAnti) { |
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447 | daughterPi = "pi-"; |
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448 | } else { |
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449 | daughterPi = "pi+"; |
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450 | } |
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451 | r = br/6.0; |
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452 | } |
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453 | if (fAnti) daughterDelta = "anti_" + daughterDelta; |
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454 | // create decay channel [parent BR #daughters] |
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455 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2, |
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456 | daughterDelta,daughterPi); |
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457 | // add decay table |
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458 | decayTable->Insert(mode); |
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459 | |
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460 | // ------------ Delta pi+/- ------------ |
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461 | // determine daughters |
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462 | if (iIso3 == +1) { |
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463 | daughterDelta = "delta++"; |
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464 | if (!fAnti) { |
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465 | daughterPi = "pi-"; |
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466 | } else { |
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467 | daughterPi = "pi+"; |
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468 | } |
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469 | r = br/2.0; |
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470 | } else { |
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471 | daughterDelta = "delta-"; |
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472 | if (!fAnti) { |
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473 | daughterPi = "pi+"; |
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474 | } else { |
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475 | daughterPi = "pi-"; |
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476 | } |
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477 | r = br/2.0; |
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478 | } |
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479 | if (fAnti) daughterDelta = "anti_" + daughterDelta; |
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480 | // create decay channel [parent BR #daughters] |
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481 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2, |
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482 | daughterDelta,daughterPi); |
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483 | // add decay table |
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484 | decayTable->Insert(mode); |
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485 | |
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486 | // ------------ Delta pi0 ------------ |
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487 | // determine daughters |
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488 | if (iIso3 == +1) { |
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489 | daughterDelta = "delta+"; |
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490 | daughterPi = "pi0"; |
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491 | r = br/3.0; |
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492 | } else { |
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493 | daughterDelta = "delta0"; |
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494 | daughterPi = "pi0"; |
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495 | r = br/3.0; |
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496 | } |
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497 | if (fAnti) daughterDelta = "anti_" + daughterDelta; |
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498 | // create decay channel [parent BR #daughters] |
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499 | mode = new G4PhaseSpaceDecayChannel(nameParent, r, 2, |
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500 | daughterDelta,daughterPi); |
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501 | // add decay table |
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502 | decayTable->Insert(mode); |
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503 | |
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504 | |
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505 | return decayTable; |
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506 | } |
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507 | |
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508 | G4DecayTable* G4ExcitedNucleonConstructor::AddLambdaKMode( |
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509 | G4DecayTable* decayTable, const G4String& nameParent, |
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510 | G4double br, G4int iIso3, G4bool fAnti) |
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511 | { |
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512 | G4VDecayChannel* mode; |
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513 | |
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514 | G4String lambda = "lambda"; |
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515 | G4String daughterK; |
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516 | |
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517 | // ------------ N pi0 ------------ |
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518 | // determine daughters |
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519 | if (iIso3 == +1) { |
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520 | if (!fAnti) { |
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521 | daughterK = "kaon+"; |
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522 | } else { |
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523 | daughterK = "kaon-"; |
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524 | } |
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525 | } else { |
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526 | if (!fAnti) { |
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527 | daughterK = "kaon0"; |
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528 | } else { |
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529 | daughterK = "anti_kaon0"; |
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530 | } |
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531 | } |
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532 | if (fAnti) lambda = "anti_" + lambda; |
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533 | // create decay channel [parent BR #daughters] |
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534 | mode = new G4PhaseSpaceDecayChannel(nameParent, br, 2, |
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535 | lambda, daughterK); |
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536 | // add decay table |
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537 | decayTable->Insert(mode); |
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538 | |
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539 | return decayTable; |
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540 | } |
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541 | |
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542 | // PDG2005 |
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543 | // N(2090) is renamed to N(2080) |
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544 | // but keep unchanged temporalily Apr 06 |
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545 | |
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546 | const char* G4ExcitedNucleonConstructor::name[] = { |
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547 | "N(1440)", "N(1520)", "N(1535)", "N(1650)", "N(1675)", |
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548 | "N(1680)", "N(1700)", "N(1710)", "N(1720)", "N(1900)", |
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549 | "N(1990)", "N(2090)", "N(2190)", "N(2220)", "N(2250)" |
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550 | }; |
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551 | |
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552 | const G4double G4ExcitedNucleonConstructor::mass[] = { |
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553 | 1.440*GeV, 1.520*GeV, 1.535*GeV, 1.655*GeV, 1.675*GeV, |
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554 | 1.685*GeV, 1.700*GeV, 1.710*GeV, 1.720*GeV, 1.900*GeV, |
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555 | 1.950*GeV, 2.080*GeV, 2.190*GeV, 2.250*GeV, 2.275*GeV |
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556 | }; |
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557 | |
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558 | const G4double G4ExcitedNucleonConstructor::width[] = { |
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559 | 300.0*MeV, 115.0*MeV, 150.0*MeV, 165.0*MeV, 150.0*MeV, |
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560 | 130.0*MeV, 100.0*MeV, 100.0*MeV, 200.0*MeV, 500.0*MeV, |
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561 | 555.0*MeV, 350.0*MeV, 500.0*MeV, 400.0*MeV, 500.0*MeV |
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562 | }; |
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563 | |
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564 | const G4int G4ExcitedNucleonConstructor::iSpin[] = { |
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565 | 1, 3, 1, 1, 5, |
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566 | 5, 3, 1, 3, 3, |
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567 | 7, 3, 7, 9, 9 |
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568 | }; |
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569 | |
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570 | const G4int G4ExcitedNucleonConstructor::iParity[] = { |
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571 | +1, -1, -1, -1, -1, |
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572 | +1, -1, +1, +1, +1, |
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573 | +1, -1, +1, -1, -1 |
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574 | }; |
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575 | |
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576 | const G4int G4ExcitedNucleonConstructor::encodingOffset[] = { |
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577 | 10000, 0, 20000, 30000, 0, |
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578 | 10000, 20000, 40000, 30000, 40000, |
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579 | 10000, 50000, 0, 0, 10000 |
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580 | }; |
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581 | |
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582 | const G4double G4ExcitedNucleonConstructor::bRatio[ G4ExcitedNucleonConstructor::NStates ][ G4ExcitedNucleonConstructor::NumberOfDecayModes] = |
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583 | { |
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584 | { 0.0, 0.70, 0.0, 0.0, 0.0, 0.05, 0.25, 0.0, 0.0}, |
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585 | { 0.0, 0.60, 0.0, 0.0, 0.0, 0.15, 0.25, 0.0, 0.0}, |
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586 | {0.001, 0.55, 0.35, 0.0, 0.0, 0.05, 0.00, 0.05, 0.0}, |
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587 | { 0.0, 0.65, 0.05, 0.0, 0.0, 0.05, 0.10, 0.05, 0.10}, |
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588 | { 0.0, 0.45, 0.0, 0.0, 0.0, 0.00, 0.55, 0.0, 0.0}, |
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589 | { 0.0, 0.65, 0.0, 0.0, 0.0, 0.20, 0.15, 0.0, 0.0}, |
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590 | { 0.0, 0.10, 0.05, 0.0, 0.05, 0.45, 0.35, 0.0, 0.0}, |
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591 | { 0.0, 0.15, 0.20, 0.0, 0.05, 0.20, 0.20, 0.10, 0.10}, |
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592 | { 0.0, 0.15, 0.00, 0.0, 0.25, 0.45, 0.10, 0.00, 0.05}, |
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593 | { 0.0, 0.35, 0.0, 0.55, 0.05, 0.00, 0.05, 0.0, 0.0}, |
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594 | { 0.0, 0.05, 0.0, 0.0, 0.15, 0.25, 0.30, 0.15, 0.10}, |
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595 | { 0.0, 0.60, 0.05, 0.0, 0.25, 0.05, 0.05, 0.0, 0.0}, |
---|
596 | { 0.0, 0.35, 0.0, 0.00, 0.30, 0.15, 0.15, 0.05, 0.0}, |
---|
597 | { 0.0, 0.35, 0.0, 0.0, 0.25, 0.20, 0.20, 0.0, 0.0}, |
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598 | { 0.0, 0.30, 0.0, 0.00, 0.25, 0.20, 0.20, 0.05, 0.0} |
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599 | }; |
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600 | |
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601 | |
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602 | |
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603 | |
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604 | |
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605 | |
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606 | |
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607 | |
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608 | |
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609 | |
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610 | |
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611 | |
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612 | |
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613 | |
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614 | |
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615 | |
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