//For histograms
enum mcTypes { kmcPhoton = 1, kmcConversion = 2, kmcPi0 = 3,
- kmcEta = 4, kmcElectron = 5, kmcHadron = 6 };
+ kmcEta = 4, kmcElectron = 5, kmcHadron = 6, kmcPi0Conv = 7 };
private:
//Histograms
- TH2F * fhMassNLocMax1[7][2] ; //! Mass of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
- TH2F * fhMassNLocMax2[7][2] ; //! Mass of 2 cells local maxima vs E, 1-6 for different MC particle types
- TH2F * fhMassNLocMaxN[7][2] ; //! Mass of >2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhMassNLocMax1[8][2] ; //! Mass of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
+ TH2F * fhMassNLocMax2[8][2] ; //! Mass of 2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhMassNLocMaxN[8][2] ; //! Mass of >2 cells local maxima vs E, 1-6 for different MC particle types
- TH2F * fhAsymNLocMax1[7][2] ; //! Asymmetry of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
- TH2F * fhAsymNLocMax2[7][2] ; //! Asymmetry of 2 cells local maxima vs E, 1-6 for different MC particle types
- TH2F * fhAsymNLocMaxN[7][2] ; //! Asymmetry of >2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhAsymNLocMax1[8][2] ; //! Asymmetry of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
+ TH2F * fhAsymNLocMax2[8][2] ; //! Asymmetry of 2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhAsymNLocMaxN[8][2] ; //! Asymmetry of >2 cells local maxima vs E, 1-6 for different MC particle types
TH2F * fhSplitEFractionvsAsyNLocMax1[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1 vs |A|
TH2F * fhSplitEFractionvsAsyNLocMax2[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2 vs |A|
TH2F * fhMassSplitECutNLocMax2 ; //! 85% of split energy, not matched, Mass of split clusters, NLM = 1
TH2F * fhMassSplitECutNLocMaxN ; //! 85% of split energy, not matched, Mass of split clusters, NLM > 2
- TH2F * fhMassM02NLocMax1[7][2] ; //! Mass of splitted clusters when 1 local max vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * fhMassM02NLocMax2[7][2] ; //! Mass of splitted clusters when 2 local max vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * fhMassM02NLocMaxN[7][2] ; //! Mass of splitted clusters when >2 local max vs M02, for E > 7 GeV, 1-6 for different MC particle types
+ TH2F * fhMassM02NLocMax1[8][2] ; //! Mass of splitted clusters when 1 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
+ TH2F * fhMassM02NLocMax2[8][2] ; //! Mass of splitted clusters when 2 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
+ TH2F * fhMassM02NLocMaxN[8][2] ; //! Mass of splitted clusters when >2 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types
TH2F * fhMassM02NLocMax1Ebin[4] ; //! Mass of splitted clusters when 1 local max vs M02, 4 E bins, neutral clusters
TH2F * fhMassM02NLocMax2Ebin[4] ; //! Mass of splitted clusters when 2 local max vs M02, 4 E bins, neutral clusters
TH2F * fhAsyMCGenRecoNLocMax2EbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when 2 local max, 4 E bins, neutral clusters
TH2F * fhAsyMCGenRecoNLocMaxNEbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when >2 local max, 4 E bins, neutral clusters
- TH2F * fhMassDispEtaNLocMax1[7][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * fhMassDispEtaNLocMax2[7][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * fhMassDispEtaNLocMaxN[7][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 7 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispEtaNLocMax1[8][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispEtaNLocMax2[8][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispEtaNLocMaxN[8][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
TH2F * fhMassDispEtaNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
TH2F * fhMassDispEtaNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
TH2F * fhMassDispEtaNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
- TH2F * fhMassDispPhiNLocMax1[7][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * fhMassDispPhiNLocMax2[7][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * fhMassDispPhiNLocMaxN[7][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 7 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispPhiNLocMax1[8][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispPhiNLocMax2[8][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispPhiNLocMaxN[8][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
TH2F * fhMassDispPhiNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
TH2F * fhMassDispPhiNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
TH2F * fhMassDispPhiNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
- TH2F * fhMassDispAsyNLocMax1[7][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * fhMassDispAsyNLocMax2[7][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * fhMassDispAsyNLocMaxN[7][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 7 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispAsyNLocMax1[8][2] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, for E > 8 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispAsyNLocMax2[8][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
+ TH2F * fhMassDispAsyNLocMaxN[8][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types
TH2F * fhMassDispAsyNLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
TH2F * fhMassDispAsyNLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
TH2F * fhMassDispAsyNLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
- TH2F * fhNLocMax [7][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types
- TH2F * fhNLocMaxM02Cut[7][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut
+ TH2F * fhNLocMax [8][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types
+ TH2F * fhNLocMaxM02Cut[8][2] ; //! Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut
- TH2F * fhM02NLocMax1 [7][2] ; //! M02 vs E for N max in cluster = 1, 1-6 for different MC particle types
- TH2F * fhM02NLocMax2 [7][2] ; //! M02 vs E for N max in cluster = 2, 1-6 for different MC particle types
- TH2F * fhM02NLocMaxN [7][2] ; //! M02 vs E for N max in cluster > 2, 1-6 for different MC particle types
+ TH2F * fhM02NLocMax1 [8][2] ; //! M02 vs E for N max in cluster = 1, 1-6 for different MC particle types
+ TH2F * fhM02NLocMax2 [8][2] ; //! M02 vs E for N max in cluster = 2, 1-6 for different MC particle types
+ TH2F * fhM02NLocMaxN [8][2] ; //! M02 vs E for N max in cluster > 2, 1-6 for different MC particle types
TH2F * fhMCAsymM02NLocMax1MCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster = 1, for 4 energy bins
TH2F * fhMCAsymM02NLocMax2MCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster = 2, for 4 energy bins
TH2F * fhMCAsymM02NLocMaxNMCPi0Ebin[4] ; //! M02 vs decay asymmetry for N max in cluster > 2, for 4 energy bins
- TH2F * fhMCGenFracNLocMax1[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
- TH2F * fhMCGenFracNLocMax2[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
- TH2F * fhMCGenFracNLocMaxN[7][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
+ TH2F * fhMCGenFracNLocMax1[8][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
+ TH2F * fhMCGenFracNLocMax2[8][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
+ TH2F * fhMCGenFracNLocMaxN[8][2] ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
TH2F * fhMCGenFracAfterCutsNLocMax1MCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, MCPi0 after M02 and asymmetry cut
TH2F * fhMCGenFracAfterCutsNLocMax2MCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, MCPi0, after M02 and asymmetry cut
TH2F * fhMCGenFracAfterCutsNLocMaxNMCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, MCPi0, after M02 and asymmetry cut
- TH2F * fhMCGenSplitEFracNLocMax1[7][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
- TH2F * fhMCGenSplitEFracNLocMax2[7][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
- TH2F * fhMCGenSplitEFracNLocMaxN[7][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
+ TH2F * fhMCGenSplitEFracNLocMax1[8][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
+ TH2F * fhMCGenSplitEFracNLocMax2[8][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
+ TH2F * fhMCGenSplitEFracNLocMaxN[8][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
TH2F * fhMCGenSplitEFracAfterCutsNLocMax1MCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
TH2F * fhMCGenSplitEFracAfterCutsNLocMax2MCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types
TH2F * fhMCGenSplitEFracAfterCutsNLocMaxNMCPi0; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types
- TH2F * fhMCGenEFracvsSplitEFracNLocMax1[7][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster = 1, MC pi0
- TH2F * fhMCGenEFracvsSplitEFracNLocMax2[7][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster = 2, MC pi0
- TH2F * fhMCGenEFracvsSplitEFracNLocMaxN[7][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster > 2, MC pi0
+ TH2F * fhMCGenEFracvsSplitEFracNLocMax1[8][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster = 1, MC pi0
+ TH2F * fhMCGenEFracvsSplitEFracNLocMax2[8][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster = 2, MC pi0
+ TH2F * fhMCGenEFracvsSplitEFracNLocMaxN[8][2] ; //! E generated particle / E reconstructed vs E1+E2 reconstructed / E reconstructed for N max in cluster > 2, MC pi0
- TH2F * fhMCGenEvsSplitENLocMax1[7][2] ; //! E generated particle vs E1+E2 for N max in cluster = 1, 1-6 for different MC particle types
- TH2F * fhMCGenEvsSplitENLocMax2[7][2] ; //! E generated particle vs E1+E2 for N max in cluster = 2, 1-6 for different MC particle types
- TH2F * fhMCGenEvsSplitENLocMaxN[7][2] ; //! E generated particle vs E1+E2 for N max in cluster > 2, 1-6 for different MC particle types
+ TH2F * fhMCGenEvsSplitENLocMax1[8][2] ; //! E generated particle vs E1+E2 for N max in cluster = 1, 1-6 for different MC particle types
+ TH2F * fhMCGenEvsSplitENLocMax2[8][2] ; //! E generated particle vs E1+E2 for N max in cluster = 2, 1-6 for different MC particle types
+ TH2F * fhMCGenEvsSplitENLocMaxN[8][2] ; //! E generated particle vs E1+E2 for N max in cluster > 2, 1-6 for different MC particle types
- TH2F * fhMCGenFracNLocMaxEbin[7][4] ; //! NLM vs E generated particle / E reconstructed vs E reconstructed 1-6 for different MC particle types, not matched to track
- TH2F * fhMCGenFracNLocMaxEbinMatched[7][4] ; //! NLM vs E generated particle / E reconstructed vs E reconstructed 1-6 for different MC particle types, matched to track
+ TH2F * fhMCGenFracNLocMaxEbin[8][4] ; //! NLM vs E generated particle / E reconstructed vs E reconstructed 1-6 for different MC particle types, not matched to track
+ TH2F * fhMCGenFracNLocMaxEbinMatched[8][4] ; //! NLM vs E generated particle / E reconstructed vs E reconstructed 1-6 for different MC particle types, matched to track
- TH2F * fhM02MCGenFracNLocMax1Ebin[7][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, not track matched
- TH2F * fhM02MCGenFracNLocMax2Ebin[7][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, not track matched
- TH2F * fhM02MCGenFracNLocMaxNEbin[7][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, not track matched
+ TH2F * fhM02MCGenFracNLocMax1Ebin[8][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, not track matched
+ TH2F * fhM02MCGenFracNLocMax2Ebin[8][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, not track matched
+ TH2F * fhM02MCGenFracNLocMaxNEbin[8][4] ; //! M02 vs E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, not track matched
- TH2F * fhMassMCGenFracNLocMax1Ebin[7][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, not track matched
- TH2F * fhMassMCGenFracNLocMax2Ebin[7][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, not track matched
- TH2F * fhMassMCGenFracNLocMaxNEbin[7][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, not track matched
+ TH2F * fhMassMCGenFracNLocMax1Ebin[8][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, not track matched
+ TH2F * fhMassMCGenFracNLocMax2Ebin[8][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, not track matched
+ TH2F * fhMassMCGenFracNLocMaxNEbin[8][4] ; //! Mass vs E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, not track matched
- TH2F * fhNCellNLocMax1[7][2] ; //! n cells in cluster vs E for N max in cluster = 1, 1-6 for different MC particle types
- TH2F * fhNCellNLocMax2[7][2] ; //! n cells in cluster vs E for N max in cluster = 2, 1-6 for different MC particle types
- TH2F * fhNCellNLocMaxN[7][2] ; //! n cells in cluster vs E for N max in cluster > 2, 1-6 for different MC particle types
+ TH2F * fhNCellNLocMax1[8][2] ; //! n cells in cluster vs E for N max in cluster = 1, 1-6 for different MC particle types
+ TH2F * fhNCellNLocMax2[8][2] ; //! n cells in cluster vs E for N max in cluster = 2, 1-6 for different MC particle types
+ TH2F * fhNCellNLocMaxN[8][2] ; //! n cells in cluster vs E for N max in cluster > 2, 1-6 for different MC particle types
- TH2F * fhM02Pi0LocMax1[7][2] ; //! M02 for Mass around pi0, N Local Maxima = 1
- TH2F * fhM02EtaLocMax1[7][2] ; //! M02 for Mass around eta, N Local Maxima = 1
- TH2F * fhM02ConLocMax1[7][2] ; //! M02 for Mass around close to 0, N Local Maxima = 1
+ TH2F * fhM02Pi0LocMax1[8][2] ; //! M02 for Mass around pi0, N Local Maxima = 1
+ TH2F * fhM02EtaLocMax1[8][2] ; //! M02 for Mass around eta, N Local Maxima = 1
+ TH2F * fhM02ConLocMax1[8][2] ; //! M02 for Mass around close to 0, N Local Maxima = 1
- TH2F * fhM02Pi0LocMax2[7][2] ; //! M02 for Mass around pi0, N Local Maxima = 2
- TH2F * fhM02EtaLocMax2[7][2] ; //! M02 for Mass around eta, N Local Maxima = 2
- TH2F * fhM02ConLocMax2[7][2] ; //! M02 for Mass around close to 0, N Local Maxima = 2
+ TH2F * fhM02Pi0LocMax2[8][2] ; //! M02 for Mass around pi0, N Local Maxima = 2
+ TH2F * fhM02EtaLocMax2[8][2] ; //! M02 for Mass around eta, N Local Maxima = 2
+ TH2F * fhM02ConLocMax2[8][2] ; //! M02 for Mass around close to 0, N Local Maxima = 2
- TH2F * fhM02Pi0LocMaxN[7][2] ; //! M02 for Mass around pi0, N Local Maxima > 2
- TH2F * fhM02EtaLocMaxN[7][2] ; //! M02 for Mass around eta, N Local Maxima > 2
- TH2F * fhM02ConLocMaxN[7][2] ; //! M02 for Mass around close to 0, N Local Maxima > 2
+ TH2F * fhM02Pi0LocMaxN[8][2] ; //! M02 for Mass around pi0, N Local Maxima > 2
+ TH2F * fhM02EtaLocMaxN[8][2] ; //! M02 for Mass around eta, N Local Maxima > 2
+ TH2F * fhM02ConLocMaxN[8][2] ; //! M02 for Mass around close to 0, N Local Maxima > 2
- TH2F * fhMassPi0LocMax1[7][2] ; //! Mass for selected pi0, N Local Maxima = 1
- TH2F * fhMassEtaLocMax1[7][2] ; //! Mass for selected around eta, N Local Maxima = 1
- TH2F * fhMassConLocMax1[7][2] ; //! Mass for selected around close to 0, N Local Maxima = 1
+ TH2F * fhMassPi0LocMax1[8][2] ; //! Mass for selected pi0, N Local Maxima = 1
+ TH2F * fhMassEtaLocMax1[8][2] ; //! Mass for selected around eta, N Local Maxima = 1
+ TH2F * fhMassConLocMax1[8][2] ; //! Mass for selected around close to 0, N Local Maxima = 1
- TH2F * fhMassPi0LocMax2[7][2] ; //! Mass for selected around pi0, N Local Maxima = 2
- TH2F * fhMassEtaLocMax2[7][2] ; //! Mass for selected around eta, N Local Maxima = 2
- TH2F * fhMassConLocMax2[7][2] ; //! Mass for selected around close to 0, N Local Maxima = 2
+ TH2F * fhMassPi0LocMax2[8][2] ; //! Mass for selected around pi0, N Local Maxima = 2
+ TH2F * fhMassEtaLocMax2[8][2] ; //! Mass for selected around eta, N Local Maxima = 2
+ TH2F * fhMassConLocMax2[8][2] ; //! Mass for selected around close to 0, N Local Maxima = 2
- TH2F * fhMassPi0LocMaxN[7][2] ; //! Mass for selected around pi0, N Local Maxima > 2
- TH2F * fhMassEtaLocMaxN[7][2] ; //! Mass for selected around eta, N Local Maxima > 2
- TH2F * fhMassConLocMaxN[7][2] ; //! Mass for selected around close to 0, N Local Maxima > 2
+ TH2F * fhMassPi0LocMaxN[8][2] ; //! Mass for selected around pi0, N Local Maxima > 2
+ TH2F * fhMassEtaLocMaxN[8][2] ; //! Mass for selected around eta, N Local Maxima > 2
+ TH2F * fhMassConLocMaxN[8][2] ; //! Mass for selected around close to 0, N Local Maxima > 2
- TH2F * fhMassAfterCutsNLocMax1[7] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 1, not matched
- TH2F * fhMassAfterCutsNLocMax2[7] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 2, not matched
- TH2F * fhMassAfterCutsNLocMaxN[7] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima > 2, not matched
+ TH2F * fhMassAfterCutsNLocMax1[8] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 1, not matched
+ TH2F * fhMassAfterCutsNLocMax2[8] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 2, not matched
+ TH2F * fhMassAfterCutsNLocMaxN[8] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima > 2, not matched
- TH2F * fhAsyPi0LocMax1[7][2] ; //! Asy for Mass around pi0, N Local Maxima = 1
- TH2F * fhAsyEtaLocMax1[7][2] ; //! Asy for Mass around eta, N Local Maxima = 1
- TH2F * fhAsyConLocMax1[7][2] ; //! Asy for Mass around close to 0, N Local Maxima = 1
+ TH2F * fhAsyPi0LocMax1[8][2] ; //! Asy for Mass around pi0, N Local Maxima = 1
+ TH2F * fhAsyEtaLocMax1[8][2] ; //! Asy for Mass around eta, N Local Maxima = 1
+ TH2F * fhAsyConLocMax1[8][2] ; //! Asy for Mass around close to 0, N Local Maxima = 1
- TH2F * fhAsyPi0LocMax2[7][2] ; //! Asy for Mass around pi0, N Local Maxima = 2
- TH2F * fhAsyEtaLocMax2[7][2] ; //! Asy for Mass around eta, N Local Maxima = 2
- TH2F * fhAsyConLocMax2[7][2] ; //! Asy for Mass around close to 0, N Local Maxima = 2
+ TH2F * fhAsyPi0LocMax2[8][2] ; //! Asy for Mass around pi0, N Local Maxima = 2
+ TH2F * fhAsyEtaLocMax2[8][2] ; //! Asy for Mass around eta, N Local Maxima = 2
+ TH2F * fhAsyConLocMax2[8][2] ; //! Asy for Mass around close to 0, N Local Maxima = 2
- TH2F * fhAsyPi0LocMaxN[7][2] ; //! Asy for Mass around pi0, N Local Maxima > 2
- TH2F * fhAsyEtaLocMaxN[7][2] ; //! Asy for Mass around eta, N Local Maxima > 2
- TH2F * fhAsyConLocMaxN[7][2] ; //! Asy for Mass around close to 0, N Local Maxima > 2
+ TH2F * fhAsyPi0LocMaxN[8][2] ; //! Asy for Mass around pi0, N Local Maxima > 2
+ TH2F * fhAsyEtaLocMaxN[8][2] ; //! Asy for Mass around eta, N Local Maxima > 2
+ TH2F * fhAsyConLocMaxN[8][2] ; //! Asy for Mass around close to 0, N Local Maxima > 2
- TH2F * fhSplitEFractionNLocMax1[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1
- TH2F * fhSplitEFractionNLocMax2[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2
- TH2F * fhSplitEFractionNLocMaxN[7][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2
+ TH2F * fhSplitEFractionNLocMax1[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1
+ TH2F * fhSplitEFractionNLocMax2[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2
+ TH2F * fhSplitEFractionNLocMaxN[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2
TH2F * fhSplitEFractionAfterCutsNLocMax1 ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1, after M02 and asymmetry cut
TH2F * fhSplitEFractionAfterCutsNLocMax2 ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2, after M02 and asymmetry cut
TH2F * fhSplitEFractionAfterCutsNLocMaxN ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2, after M02 and asymmetry cut
- TH2F * fhMassSplitEFractionNLocMax1Ebin[7][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster = 1, 1-6 for different MC particle types, not track matched
- TH2F * fhMassSplitEFractionNLocMax2Ebin[7][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster = 2, 1-6 for different MC particle types, not track matched
- TH2F * fhMassSplitEFractionNLocMaxNEbin[7][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster > 2, 1-6 for different MC particle types, not track matched
+ TH2F * fhMassSplitEFractionNLocMax1Ebin[8][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster = 1, 1-6 for different MC particle types, not track matched
+ TH2F * fhMassSplitEFractionNLocMax2Ebin[8][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster = 2, 1-6 for different MC particle types, not track matched
+ TH2F * fhMassSplitEFractionNLocMaxNEbin[8][4] ; //! Mass vs sum of splitted cluster energy / cluster energy for N max in cluster > 2, 1-6 for different MC particle types, not track matched
TH2F * fhAnglePairLocMax1[2] ; //! pair opening angle vs E
TH2F * fhAnglePairLocMax2[2] ; //! pair opening angle vs E
TH2F * fhAnglePairMassLocMax2[2] ; //! pair opening angle vs Mass for E > 7 GeV
TH2F * fhAnglePairMassLocMaxN[2] ; //! pair opening angle vs Mass for E > 7 GeV
- TH2F * fhTrackMatchedDEtaLocMax1[7] ; //! Eta distance between track and cluster vs cluster E, 1 local maximum
- TH2F * fhTrackMatchedDPhiLocMax1[7] ; //! Phi distance between track and cluster vs cluster E, 1 local maximum
- TH2F * fhTrackMatchedDEtaLocMax2[7] ; //! Eta distance between track and cluster vs cluster E, 2 local maximum
- TH2F * fhTrackMatchedDPhiLocMax2[7] ; //! Phi distance between track and cluster vs cluster E, 2 local maximum
- TH2F * fhTrackMatchedDEtaLocMaxN[7] ; //! Eta distance between track and cluster vs cluster E, more than 2 local maximum
- TH2F * fhTrackMatchedDPhiLocMaxN[7] ; //! Phi distance between track and cluster vs cluster E, more than 2 local maximum
+ TH2F * fhTrackMatchedDEtaLocMax1[8] ; //! Eta distance between track and cluster vs cluster E, 1 local maximum
+ TH2F * fhTrackMatchedDPhiLocMax1[8] ; //! Phi distance between track and cluster vs cluster E, 1 local maximum
+ TH2F * fhTrackMatchedDEtaLocMax2[8] ; //! Eta distance between track and cluster vs cluster E, 2 local maximum
+ TH2F * fhTrackMatchedDPhiLocMax2[8] ; //! Phi distance between track and cluster vs cluster E, 2 local maximum
+ TH2F * fhTrackMatchedDEtaLocMaxN[8] ; //! Eta distance between track and cluster vs cluster E, more than 2 local maximum
+ TH2F * fhTrackMatchedDPhiLocMaxN[8] ; //! Phi distance between track and cluster vs cluster E, more than 2 local maximum
AliAnaInsideClusterInvariantMass( const AliAnaInsideClusterInvariantMass & split) ; // cpy ctor
AliAnaInsideClusterInvariantMass & operator = (const AliAnaInsideClusterInvariantMass & split) ; // cpy assignment