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2 | // ******************************************************************** |
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3 | // * License and Disclaimer * |
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11 | // * Neither the authors of this software system, nor their employing * |
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15 | // * use. Please see the license in the file LICENSE and URL above * |
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18 | // * This code implementation is the result of the scientific and * |
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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 | // HadrontherapyAnalysisManager.hh; May 2005 |
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27 | // See more at: http://g4advancedexamples.lngs.infn.it/Examples/hadrontherapy |
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28 | |
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29 | #ifndef HADRONTHERAPYANALYSISMANAGER_HH |
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30 | #define HADRONTHERAPYANALYSISMANAGER_HH 1 |
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31 | |
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32 | #include "globals.hh" |
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33 | |
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34 | |
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35 | #ifdef G4ANALYSIS_USE_ROOT ///< If analysis is done directly with ROOT |
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36 | #include "TROOT.h" |
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37 | #include "TFile.h" |
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38 | #include "TNtuple.h" |
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39 | #include "TH1F.h" |
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40 | #endif |
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41 | /** |
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42 | * Messenger class for analysis-settings for HadronTherapyAnalysisManager |
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43 | */ |
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44 | class HadrontherapyAnalysisFileMessenger; |
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45 | |
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46 | /** |
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47 | * A class for connecting the simulation to an analysis package. |
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48 | */ |
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49 | class HadrontherapyAnalysisManager |
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50 | { |
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51 | private: |
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52 | /** |
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53 | * Analysis manager is a singleton object (there is only one instance). |
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54 | * The pointer to this object is available through the use of the method GetInstance(); |
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55 | * |
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56 | * @see GetInstance |
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57 | */ |
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58 | HadrontherapyAnalysisManager(); |
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59 | |
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60 | public: |
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61 | ~HadrontherapyAnalysisManager(); |
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62 | |
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63 | /** |
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64 | * Get the pointer to the analysis manager. |
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65 | */ |
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66 | static HadrontherapyAnalysisManager* GetInstance(); |
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67 | |
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68 | #ifdef G4ANALYSIS_USE_ROOT |
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69 | /** |
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70 | * Clear analysis manager heap. |
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71 | */ |
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72 | void Clear(); |
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73 | |
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74 | /** |
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75 | * Book the histograms and ntuples in an AIDA or ROOT file. |
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76 | */ |
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77 | void book(); |
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78 | /** |
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79 | * Set name for the analysis file .root (used by macro) |
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80 | */ |
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81 | void SetAnalysisFileName(G4String); |
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82 | |
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83 | /** |
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84 | * Fill the ntuple with the energy deposit in the phantom |
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85 | */ |
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86 | void FillEnergyDeposit(G4int voxelXId, G4int voxelYId, G4int voxelZId, |
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87 | G4double energyDeposit); |
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88 | |
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89 | void BraggPeak(G4int, G4double); ///< Fill 1D histogram with the Bragg peak in the phantom |
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90 | |
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91 | void SecondaryProtonEnergyDeposit(G4int slice, G4double energy); |
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92 | ///< Fill 1D histogram with the energy deposit of secondary protons |
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93 | |
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94 | void SecondaryNeutronEnergyDeposit(G4int slice, G4double energy); |
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95 | ///< Fill 1D histogram with the energy deposit of secondary neutrons |
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96 | |
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97 | void SecondaryAlphaEnergyDeposit(G4int slice, G4double energy); |
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98 | ///< Fill 1D histogram with the energy deposit of secondary alpha particles |
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99 | |
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100 | void SecondaryGammaEnergyDeposit(G4int slice, G4double energy); |
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101 | ///< Fill 1D histogram with the energy deposit of secondary gamma |
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102 | |
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103 | void SecondaryElectronEnergyDeposit(G4int slice, G4double energy); |
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104 | ///< Fill 1D histogram with the energy deposit of secondary electrons |
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105 | |
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106 | void SecondaryTritonEnergyDeposit(G4int slice, G4double energy); |
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107 | ///< Fill 1D histogram with the energy deposit of secondary tritons |
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108 | |
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109 | void SecondaryDeuteronEnergyDeposit(G4int slice, G4double energy); |
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110 | ///< Fill 1D histogram with the energy deposit of secondary deuterons |
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111 | |
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112 | void SecondaryPionEnergyDeposit(G4int slice, G4double energy); |
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113 | ///< Fill 1D histogram with the energy deposit of secondary pions |
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114 | |
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115 | void electronEnergyDistribution(G4double secondaryParticleKineticEnergy); |
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116 | ///< Energy distribution of secondary electrons originated in the phantom |
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117 | |
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118 | void gammaEnergyDistribution(G4double secondaryParticleKineticEnergy); |
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119 | ///< Energy distribution of secondary gamma originated in the phantom |
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120 | |
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121 | void deuteronEnergyDistribution(G4double secondaryParticleKineticEnergy); |
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122 | ///< Energy distribution of secondary deuterons originated in the phantom |
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123 | |
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124 | void tritonEnergyDistribution(G4double secondaryParticleKineticEnergy); |
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125 | ///< Energy distribution of secondary tritons originated in the phantom |
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126 | |
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127 | void alphaEnergyDistribution(G4double secondaryParticleKineticEnergy); |
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128 | ///< Energy distribution of secondary alpha originated in the phantom |
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129 | |
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130 | void heliumEnergy(G4double secondaryParticleKineticEnergy); |
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131 | ///< Energy distribution of the helium (He3 and alpha) particles after the phantom |
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132 | |
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133 | void hydrogenEnergy(G4double secondaryParticleKineticEnergy); |
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134 | ///< Energy distribution of the hydrogen (proton, d, t) particles after the phantom |
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135 | |
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136 | //Kinetic energy by voxel, mass number A and atomic number Z. |
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137 | void FillKineticFragmentTuple(G4int i, G4int j, G4int k, G4int A, G4double Z, G4double kinEnergy); |
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138 | |
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139 | //Kinetic energy by voxel, mass number A and atomic number Z of only primary particles |
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140 | void FillKineticEnergyPrimaryNTuple(G4int i, G4int j, G4int k, G4double kinEnergy); |
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141 | |
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142 | ///< Energy by voxel, mass number A and atomic number Z. |
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143 | void FillVoxelFragmentTuple(G4int i, G4int j, G4int k, G4int A, G4double Z, G4double energy, G4double fluence); |
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144 | |
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145 | void FillFragmentTuple(G4int A, G4double Z, G4double energy, G4double posX, G4double posY, G4double posZ); |
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146 | ///< Energy ntuple |
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147 | |
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148 | void FillLetFragmentTuple(G4int i, G4int j, G4int k, G4int A, G4double Z, G4double letT, G4double letD); |
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149 | ///< let ntuple |
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150 | |
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151 | void genericIonInformation(G4int, G4double, G4int, G4double); |
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152 | |
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153 | void ThintargetBeamDisp(G4double,G4double); |
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154 | |
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155 | void startNewEvent(); |
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156 | ///< Tell the analysis manager that a new event is starting |
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157 | |
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158 | void setGeometryMetaData(G4double, G4double, G4double); |
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159 | ///< from the detector construction information about the geometry can be written as metadata |
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160 | |
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161 | void setBeamMetaData(G4double, G4double); |
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162 | ///< metadata about the beam can be written this way |
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163 | |
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164 | void flush(); |
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165 | ///< Close the .hbk file with the histograms and the ntuples |
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166 | private: |
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167 | TH1F *createHistogram1D(const TString name, const TString title, int bins, double xmin, double xmax) { |
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168 | TH1F *histo = new TH1F(name, title, bins, xmin, xmax); |
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169 | histo->SetLineWidth(2); |
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170 | return histo; |
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171 | } |
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172 | |
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173 | private: |
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174 | #endif |
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175 | static HadrontherapyAnalysisManager* instance; |
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176 | HadrontherapyAnalysisFileMessenger* fMess; |
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177 | #ifdef G4ANALYSIS_USE_ROOT |
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178 | G4String analysisFileName; |
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179 | TFile *theTFile; |
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180 | TH1F *histo1; |
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181 | TH1F *histo2; |
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182 | TH1F *histo3; |
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183 | TH1F *histo4; |
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184 | TH1F *histo5; |
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185 | TH1F *histo6; |
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186 | TH1F *histo7; |
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187 | TH1F *histo8; |
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188 | TH1F *histo9; |
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189 | TH1F *histo10; |
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190 | TH1F *histo11; |
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191 | TH1F *histo12; |
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192 | TH1F *histo13; |
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193 | TH1F *histo14; |
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194 | TH1F *histo15; |
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195 | TH1F *histo16; |
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196 | |
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197 | TNtuple *kinFragNtuple; |
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198 | TNtuple *kineticEnergyPrimaryNtuple; |
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199 | |
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200 | // ntuple containing the fluence of all the particle in any voxel |
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201 | TNtuple *doseFragNtuple; |
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202 | |
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203 | // ntuple containing the fluence of all the particle in any voxel |
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204 | TNtuple *fluenceFragNtuple; |
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205 | |
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206 | // ntuple containing the fluence of all the particle in any voxel |
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207 | TNtuple *letFragNtuple; |
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208 | |
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209 | TNtuple *theROOTNtuple; |
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210 | TNtuple *theROOTIonTuple; |
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211 | TNtuple *fragmentNtuple; // fragments |
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212 | TNtuple *metaData; |
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213 | G4long eventCounter; // Simulation metadata |
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214 | G4double detectorDistance; |
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215 | G4double phantomDepth; |
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216 | G4double beamEnergy; |
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217 | G4double energyError; |
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218 | G4double phantomCenterDistance; |
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219 | #endif |
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220 | }; |
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221 | #endif |
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222 | |
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223 | |
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224 | |
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