TH2F * fhSplitEFractionvsAsyNLocMax2[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2 vs |A|
TH2F * fhSplitEFractionvsAsyNLocMaxN[2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2 vs |A|
- TH2F * fhMassM02CutNLocMax1 ; //! M02(E) selection, not matched, Mass of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
- TH2F * fhMassM02CutNLocMax2 ; //! M02(E) selection, not matched, Mass of 2 cells local maxima vs E, 1-6 for different MC particle types
- TH2F * fhMassM02CutNLocMaxN ; //! M02(E) selection, not matched, Mass of >2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhMassM02CutNLocMax1 ; //! M02(E) selection, not matched, Mass of split clusters, NLM = 1
+ TH2F * fhMassM02CutNLocMax2 ; //! M02(E) selection, not matched, Mass of split clusters, NLM = 1
+ TH2F * fhMassM02CutNLocMaxN ; //! M02(E) selection, not matched, Mass of split clusters, NLM > 2
- TH2F * fhMassSplitECutNLocMax1 ; //! 85% of split energy, not matched, Mass of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
- TH2F * fhMassSplitECutNLocMax2 ; //! 85% of split energy, not matched, Mass of 2 cells local maxima vs E, 1-6 for different MC particle types
- TH2F * fhMassSplitECutNLocMaxN ; //! 85% of split energy, not matched, Mass of >2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhAsymM02CutNLocMax1 ; //! M02(E) selection, not matched, energy asymmetry of split clusters, NLM = 1
+ TH2F * fhAsymM02CutNLocMax2 ; //! M02(E) selection, not matched, energy asymmetry of split clusters, NLM = 2
+ TH2F * fhAsymM02CutNLocMaxN ; //! M02(E) selection, not matched, energy asymmetry of split clusters, NLM > 2
- TH2F * fhMassAsyCutNLocMax1 ; //! |A|>0.8 selection, not matched, Mass of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types
- TH2F * fhMassAsyCutNLocMax2 ; //! |A|>0.8 selection, not matched, Mass of 2 cells local maxima vs E, 1-6 for different MC particle types
- TH2F * fhMassAsyCutNLocMaxN ; //! |A|>0.8 selection, not matched, Mass of >2 cells local maxima vs E, 1-6 for different MC particle types
+ TH2F * fhMassSplitECutNLocMax1 ; //! 85% of split energy, not matched, Mass of split clusters, NLM = 1
+ 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 * fhMassAsyCutNLocMax1 ; //! |A|>0.8 selection, Mass of split clusters, NLM = 1
+ TH2F * fhMassAsyCutNLocMax2 ; //! |A|>0.8 selection, Mass of split clusters, NLM = 1
+ TH2F * fhMassAsyCutNLocMaxN ; //! |A|>0.8 selection, Mass of split clusters, NLM > 2
TH2F * fhMassM02NLocMax1[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 * fhMassM02NLocMax2[7][2] ; //! Mass of 2 cells local maxima, vs M02, for E > 7 GeV, 1-6 for different MC particle types
AliAnaInsideClusterInvariantMass( const AliAnaInsideClusterInvariantMass & split) ; // cpy ctor
AliAnaInsideClusterInvariantMass & operator = (const AliAnaInsideClusterInvariantMass & split) ; // cpy assignment
- ClassDef(AliAnaInsideClusterInvariantMass,17)
+ ClassDef(AliAnaInsideClusterInvariantMass,18)
} ;