TObjString * GetAnalysisCuts();
TList * GetCreateOutputObjects();
-
+
+ void FillSSWeightHistograms(AliVCluster *clus, const Int_t nlm, const Int_t absId1, const Int_t absId2);
+
void Init();
void InitParameters();
void SetMinBadChannelDistance(Float_t cut) { fMinBadDist = cut ; }
+ void SetWCorrectionParameter(Float_t p = 0.07) { fWSimu = p ; }
+
void SwitchOnFillAngleHistograms() { fFillAngleHisto = kTRUE ; }
void SwitchOffFillAngleHistograms() { fFillAngleHisto = kFALSE ; }
void SwitchOnFillExtraSSHistograms() { fFillSSExtraHisto = kTRUE ; }
void SwitchOffFillExtraSSHistograms() { fFillSSExtraHisto = kFALSE ; }
+ void SwitchOnFillTMHistograms() { fFillTMHisto = kTRUE ; }
+ void SwitchOffFillTMHistograms() { fFillTMHisto = kFALSE ; }
+
void SwitchOnFillTMResidualHistograms() { fFillTMResidualHisto = kTRUE ; }
void SwitchOffFillTMResidualHistograms() { fFillTMResidualHisto = kFALSE ; }
+ void SwitchOnMCFractionHistograms() { fFillMCFractionHisto = kTRUE ; }
+ void SwitchOffMCFractionHistograms() { fFillMCFractionHisto = kFALSE ; }
+
+ void SwitchOnFillSSWeightHistograms() { fFillSSWeightHisto = kTRUE ; }
+ void SwitchOffFillSSWeightHistograms() { fFillSSWeightHisto = kFALSE ; }
+
+ void SwitchOnFillEbinHistograms() { fFillEbinHisto = kTRUE ; }
+ void SwitchOffFillEbinHistograms() { fFillEbinHisto = kFALSE ; }
+
+ void SetNWeightForShowerShape(Int_t n) { fSSWeightN = n ; }
+ void SetWeightForShowerShape(Int_t i, Float_t v) { if (i < 10) fSSWeight[i] = v ; }
+
+ void SetNECellCutForShowerShape(Int_t n) { fSSECellCutN = n ; }
+ void SetECellCutForShowerShape(Int_t i, Float_t v) { if (i < 10) fSSECellCut[i] = v ; }
+
+
+ void RecalculateClusterShowerShapeParametersWithCellCut(const AliEMCALGeometry * geom, AliVCaloCells* cells, AliVCluster * cluster,
+ Float_t & l0, Float_t & l1,
+ Float_t & disp, Float_t & dEta, Float_t & dPhi,
+ Float_t & sEta, Float_t & sPhi, Float_t & sEtaPhi,Float_t eCellMin = 0.);
+
+
//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:
Float_t fMinBadDist ; // Minimal distance to bad channel to accept cluster
Bool_t fFillAngleHisto; // Fill splitted clusters angle histograms
+ Bool_t fFillTMHisto ; // Fill track matching histos,
Bool_t fFillTMResidualHisto ; // Fill track matching histos, residuals
Bool_t fFillSSExtraHisto ; // Fill shower shape extra histos
+ Bool_t fFillMCFractionHisto ; // Fill MC energy fraction histos
+ Bool_t fFillSSWeightHisto ; // Fill weigth histograms
+ Bool_t fFillEbinHisto ; // Fill E bin histograms
+
+ Float_t fSSWeight[10]; // List of weights to test
+ Int_t fSSWeightN; // Total number of weights to test
+
+ Float_t fSSECellCut[10]; // List of cell min energy cuts to test
+ Int_t fSSECellCutN; // Total number of cell min energy cuts to test
+
+ Float_t fWSimu; // Slope of the linear correction factor for the shower
+ // shape weight in simulation, about 0.07
//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[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 * 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 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 * 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
- TH2F * fhMassM02NLocMaxN[7][2] ; //! Mass of >2 cells local maxima, vs M02, for E > 7 GeV, 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 * fhMassM02NLocMax1Ebin[4] ; //! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters
- TH2F * fhMassM02NLocMax2Ebin[4] ; //! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters
- TH2F * fhMassM02NLocMaxNEbin[4] ; //! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters
+ 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 * 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 * 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 * 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 * fhMassM02NLocMaxNEbin[4] ; //! Mass of splitted clusters when >2 local max vs M02, 4 E bins, neutral clusters
+
+ TH2F * fhMassAsyNLocMax1Ebin[4] ; //! Mass of Mass of splitted clusters when 1 local max vs asymmetry, 4 E bins, neutral clusters
+ TH2F * fhMassAsyNLocMax2Ebin[4] ; //! Mass of Mass of splitted clusters when 2 local max vs asymmetry, 4 E bins, neutral clusters
+ TH2F * fhMassAsyNLocMaxNEbin[4] ; //! Mass of Mass of splitted clusters when >2 local max vs asymmetry, 4 E bins, neutral clusters
+
+ TH2F * fhAsyMCGenRecoNLocMax1EbinPi0[4] ; //! Generated vs reconstructed asymmetry of splitted clusters from pi0 when 1 local max, 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 [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 [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[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 * 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 * 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[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[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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * fhM02Pi0NLocMax1[8][2] ; //! M02 for Mass around pi0, N Local Maxima = 1
+ TH2F * fhM02EtaNLocMax1[8][2] ; //! M02 for Mass around eta, N Local Maxima = 1
+ TH2F * fhM02ConNLocMax1[8][2] ; //! M02 for Mass around close to 0, N Local Maxima = 1
- 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 * fhM02Pi0NLocMax2[8][2] ; //! M02 for Mass around pi0, N Local Maxima = 2
+ TH2F * fhM02EtaNLocMax2[8][2] ; //! M02 for Mass around eta, N Local Maxima = 2
+ TH2F * fhM02ConNLocMax2[8][2] ; //! M02 for Mass around close to 0, N Local Maxima = 2
- 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 * fhM02Pi0NLocMaxN[8][2] ; //! M02 for Mass around pi0, N Local Maxima > 2
+ TH2F * fhM02EtaNLocMaxN[8][2] ; //! M02 for Mass around eta, N Local Maxima > 2
+ TH2F * fhM02ConNLocMaxN[8][2] ; //! M02 for Mass around close to 0, N Local Maxima > 2
- 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 * fhMassPi0NLocMax1[8][2] ; //! Mass for selected pi0, N Local Maxima = 1
+ TH2F * fhMassEtaNLocMax1[8][2] ; //! Mass for selected around eta, N Local Maxima = 1
+ TH2F * fhMassConNLocMax1[8][2] ; //! Mass for selected around close to 0, N Local Maxima = 1
+
+ TH2F * fhMassPi0NLocMax2[8][2] ; //! Mass for selected around pi0, N Local Maxima = 2
+ TH2F * fhMassEtaNLocMax2[8][2] ; //! Mass for selected around eta, N Local Maxima = 2
+ TH2F * fhMassConNLocMax2[8][2] ; //! Mass for selected around close to 0, N Local Maxima = 2
+
+ TH2F * fhMassPi0NLocMaxN[8][2] ; //! Mass for selected around pi0, N Local Maxima > 2
+ TH2F * fhMassEtaNLocMaxN[8][2] ; //! Mass for selected around eta, N Local Maxima > 2
+ TH2F * fhMassConNLocMaxN[8][2] ; //! Mass for selected 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 * fhMassAfterCutsNLocMax1[8][2] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 1
+ TH2F * fhMassAfterCutsNLocMax2[8][2] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima = 2
+ TH2F * fhMassAfterCutsNLocMaxN[8][2] ; //! Mass after M02, asymmetry cuts for pi0, N Local Maxima > 2
- TH2F * fhAnglePairLocMax1[2] ; //! pair opening angle vs E
- TH2F * fhAnglePairLocMax2[2] ; //! pair opening angle vs E
- TH2F * fhAnglePairLocMaxN[2] ; //! pair opening angle vs E
+ TH2F * fhAsyPi0NLocMax1[8][2] ; //! Asy for Mass around pi0, N Local Maxima = 1
+ TH2F * fhAsyEtaNLocMax1[8][2] ; //! Asy for Mass around eta, N Local Maxima = 1
+ TH2F * fhAsyConNLocMax1[8][2] ; //! Asy for Mass around close to 0, N Local Maxima = 1
- TH2F * fhAnglePairMassLocMax1[2] ; //! pair opening angle vs Mass for E > 7 GeV
- 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 * fhAsyPi0NLocMax2[8][2] ; //! Asy for Mass around pi0, N Local Maxima = 2
+ TH2F * fhAsyEtaNLocMax2[8][2] ; //! Asy for Mass around eta, N Local Maxima = 2
+ TH2F * fhAsyConNLocMax2[8][2] ; //! Asy for Mass around close to 0, N Local Maxima = 2
- 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 * fhAsyPi0NLocMaxN[8][2] ; //! Asy for Mass around pi0, N Local Maxima > 2
+ TH2F * fhAsyEtaNLocMaxN[8][2] ; //! Asy for Mass around eta, N Local Maxima > 2
+ TH2F * fhAsyConNLocMaxN[8][2] ; //! Asy for Mass around close to 0, 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[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 1, after M02 and asymmetry cut
+ TH2F * fhSplitEFractionAfterCutsNLocMax2[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima = 2, after M02 and asymmetry cut
+ TH2F * fhSplitEFractionAfterCutsNLocMaxN[8][2] ; //! sum of splitted cluster energy / cluster energy for N Local Maxima > 2, after M02 and asymmetry cut
+
+ 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 * fhAnglePairNLocMax1[2] ; //! pair opening angle vs E
+ TH2F * fhAnglePairNLocMax2[2] ; //! pair opening angle vs E
+ TH2F * fhAnglePairNLocMaxN[2] ; //! pair opening angle vs E
+
+ TH2F * fhAnglePairMassNLocMax1[2] ; //! pair opening angle vs Mass for E > 7 GeV
+ TH2F * fhAnglePairMassNLocMax2[2] ; //! pair opening angle vs Mass for E > 7 GeV
+ TH2F * fhAnglePairMassNLocMaxN[2] ; //! pair opening angle vs Mass for E > 7 GeV
+
+ TH2F * fhTrackMatchedDEtaNLocMax1[8] ; //! Eta distance between track and cluster vs cluster E, 1 local maximum
+ TH2F * fhTrackMatchedDPhiNLocMax1[8] ; //! Phi distance between track and cluster vs cluster E, 1 local maximum
+ TH2F * fhTrackMatchedDEtaNLocMax2[8] ; //! Eta distance between track and cluster vs cluster E, 2 local maximum
+ TH2F * fhTrackMatchedDPhiNLocMax2[8] ; //! Phi distance between track and cluster vs cluster E, 2 local maximum
+ TH2F * fhTrackMatchedDEtaNLocMaxN[8] ; //! Eta distance between track and cluster vs cluster E, more than 2 local maximum
+ TH2F * fhTrackMatchedDPhiNLocMaxN[8] ; //! Phi distance between track and cluster vs cluster E, more than 2 local maximum
+
+ TH2F * fhCentralityPi0NLocMax1[8][2] ; //! Centrality for selected pi0, N Local Maxima = 1
+ TH2F * fhCentralityEtaNLocMax1[8][2] ; //! Centrality for selected eta, N Local Maxima = 1
+ TH2F * fhCentralityPi0NLocMax2[8][2] ; //! Centrality for selected pi0, N Local Maxima = 2
+ TH2F * fhCentralityEtaNLocMax2[8][2] ; //! Centrality for selected eta, N Local Maxima = 2
+ TH2F * fhCentralityPi0NLocMaxN[8][2] ; //! Centrality for selected pi0, N Local Maxima > 2
+ TH2F * fhCentralityEtaNLocMaxN[8][2] ; //! Centrality for selected eta, N Local Maxima > 2
+
+ TH2F * fhEventPlanePi0NLocMax1 ; //! Event plane for selected pi0, N Local Maxima = 1
+ TH2F * fhEventPlaneEtaNLocMax1 ; //! Event plane for selected eta, N Local Maxima = 1
+ TH2F * fhEventPlanePi0NLocMax2 ; //! Event plane for selected pi0, N Local Maxima = 2
+ TH2F * fhEventPlaneEtaNLocMax2 ; //! Event plane for selected eta, N Local Maxima = 2
+ TH2F * fhEventPlanePi0NLocMaxN ; //! Event plane for selected pi0, N Local Maxima > 2
+ TH2F * fhEventPlaneEtaNLocMaxN ; //! Event plane for selected eta, N Local Maxima > 2
+
+ TH2F * fhClusterEtaPhiNLocMax1 ; //! Eta vs Phi of clusters with N Local Maxima = 1, E > 8 GeV
+ TH2F * fhClusterEtaPhiNLocMax2 ; //! Eta vs Phi of clusters with N Local Maxima = 2, E > 8 GeV
+ TH2F * fhClusterEtaPhiNLocMaxN ; //! Eta vs Phi of clusters with N Local Maxima > 2, E > 8 GeV
+ TH2F * fhPi0EtaPhiNLocMax1 ; //! Eta vs Phi of pi0's with N Local Maxima = 1, E > 8 GeV
+ TH2F * fhPi0EtaPhiNLocMax2 ; //! Eta vs Phi of pi0's with N Local Maxima = 2, E > 8 GeV
+ TH2F * fhPi0EtaPhiNLocMaxN ; //! Eta vs Phi of pi0's with N Local Maxima > N, E > 8 GeV
+ TH2F * fhEtaEtaPhiNLocMax1 ; //! Eta vs Phi of eta's with N Local Maxima = 1, E > 8 GeV
+ TH2F * fhEtaEtaPhiNLocMax2 ; //! Eta vs Phi of eta's with N Local Maxima = 2, E > 8 GeV
+ TH2F * fhEtaEtaPhiNLocMaxN ; //! Eta vs Phi of eta's with N Local Maxima > N, E > 8 GeV
+
+ TH2F * fhPi0CellE[3] ; //! pi0's energy vs cluster cell energy with NLM = 1, = 2, > 2
+ TH2F * fhPi0CellEFrac[3] ; //! pi0's energy vs cluster cell energy fraction with NLM = 1, = 2, > 2
+ TH2F * fhPi0CellLogEFrac[3] ; //! pi0's energy vs cluster log cell energy fraction with NLM = 1, = 2, > 2
+ TH2F * fhPi0CellEMaxEMax2Frac [3]; //! pi0's energy vs fraction of 2 main maxima energy with NLM = 1, = 2, > 2
+ TH2F * fhPi0CellEMaxClusterFrac [3]; //! pi0's energy vs energy fraction of main LM and cluster energy with NLM = 1, = 2, > 2
+ TH2F * fhPi0CellEMax2ClusterFrac[3]; //! pi0's energy vs energy fraction of second LM and cluster energy with NLM = 1, = 2, > 2
+ TH2F * fhPi0CellEMaxFrac [3]; //! pi0's energy vs energy fraction of main LM and cluster cell energy with NLM = 1, = 2, > 2
+ TH2F * fhPi0CellEMax2Frac [3]; //! pi0's energy vs energy fraction of second LM and cluster cell energy with NLM = 1, = 2, > 2
+
+ TH2F * fhM02WeightPi0[3][10] ; //! M02 for selected pi0 with different weight, with NLM = 1, = 2, > 2
+ TH2F * fhM02ECellCutPi0[3][10] ; //! M02 for selected pi0 with different cut on cell energy, with NLM = 1, = 2, > 2
+
- AliAnaInsideClusterInvariantMass( const AliAnaInsideClusterInvariantMass & g) ; // cpy ctor
- AliAnaInsideClusterInvariantMass & operator = (const AliAnaInsideClusterInvariantMass & g) ; // cpy assignment
+ AliAnaInsideClusterInvariantMass( const AliAnaInsideClusterInvariantMass & split) ; // cpy ctor
+ AliAnaInsideClusterInvariantMass & operator = (const AliAnaInsideClusterInvariantMass & split) ; // cpy assignment
- ClassDef(AliAnaInsideClusterInvariantMass,14)
+ ClassDef(AliAnaInsideClusterInvariantMass,20)
} ;
git://git.uio.no / u / mrichter / AliRoot.git / blobdiff