class AliAnaInsideClusterInvariantMass: public AliAnaCaloTrackCorrBaseClass
Split clusters with some criteria and calculate invariant mass to identify them as pi0 or conversion -- Author: Gustavo Conesa (LPSC-Grenoble)
Function Members (Methods)
public:
protected:
| virtual void | TObject::DoError(int level, const char* location, const char* fmt, va_list va) const |
| void | TObject::MakeZombie() |
private:
| AliAnaInsideClusterInvariantMass(const AliAnaInsideClusterInvariantMass& split) | |
| AliAnaInsideClusterInvariantMass& | operator=(const AliAnaInsideClusterInvariantMass& split) |
Data Members
public:
| enum mcTypes { | kmcPhoton | |
| kmcConversion | ||
| kmcPi0 | ||
| kmcPi0Conv | ||
| kmcEta | ||
| kmcHadron | ||
| }; | ||
| enum AliAnaCaloTrackCorrBaseClass::detector { | kEMCAL | |
| kPHOS | ||
| kCTS | ||
| kDCAL | ||
| kDCALPHOS | ||
| }; | ||
| enum TObject::EStatusBits { | kCanDelete | |
| kMustCleanup | ||
| kObjInCanvas | ||
| kIsReferenced | ||
| kHasUUID | ||
| kCannotPick | ||
| kNoContextMenu | ||
| kInvalidObject | ||
| }; | ||
| enum TObject::[unnamed] { | kIsOnHeap | |
| kNotDeleted | ||
| kZombie | ||
| kBitMask | ||
| kSingleKey | ||
| kOverwrite | ||
| kWriteDelete | ||
| }; |
private:
| Bool_t | fCheckSplitDistToBad | Check the distance to bad channel and to EMCal borders of split clusters |
| TLorentzVector | fClusterMomentum | ! Cluster momentum |
| Bool_t | fFillAngleHisto | Fill splitted clusters angle histograms |
| Bool_t | fFillArmenterosHisto | Fill armenteros type histo |
| Bool_t | fFillEbinHisto | Fill E bin histograms |
| Bool_t | fFillHighMultHisto | Fill centrality/event plane histograms |
| Bool_t | fFillIdConvHisto | Fill histograms for clusters identified as conversion |
| Bool_t | fFillIdEtaHisto | Fill histograms for clusters identified as Eta |
| Bool_t | fFillMCHisto | Fill MC energy fraction histos |
| Bool_t | fFillMCOverlapHisto | Fill MC particles overlap histograms |
| Bool_t | fFillNCellHisto | Fill n cells in cluster dependent histograms |
| Bool_t | fFillNLMDiffCutHisto | Fill NLM histograms for different settings |
| Bool_t | fFillSSExtraHisto | Fill shower shape extra histos |
| Bool_t | fFillSSWeightHisto | Fill weigth histograms |
| Bool_t | fFillTMHisto | Fill track matching histos, |
| Bool_t | fFillTMResidualHisto | Fill track matching histos, residuals |
| Bool_t | fFillThetaStarHisto | Fill cosThetaStar histos |
| TLorentzVector | fGrandMotherMom | ! Primary momentum |
| Float_t | fHistoECut | Fixed E cut for some histograms |
| TLorentzVector | fMCDaughMom1 | ! Primary momentum |
| TLorentzVector | fMCDaughMom2 | ! Primary momentum |
| Float_t | fMinBadDist | Minimal distance to bad channel to accept cluster |
| Int_t | fMinNCells | Study clusters with ncells larger than cut |
| Float_t | fNLMMinDiff[5] | List of local maxima min difference cell energy |
| Float_t | fNLMMinE[5] | List of local maxima min energy |
| Int_t | fNLMSettingN | Total number of NLM settings to test |
| TLorentzVector | fPrimaryMom | ! Primary momentum |
| TVector3 | fProdVertex | ! primary production vertex |
| Float_t | fSSECellCut[20] | List of cell min energy cuts to test |
| Int_t | fSSECellCutN | Total number of cell min energy cuts to test |
| Float_t | fSSWeight[20] | List of weights to test |
| Int_t | fSSWeightN | Total number of weights to test |
| TLorentzVector | fSubClusterMom1 | ! Sub-Cluster momentum |
| TLorentzVector | fSubClusterMom2 | ! Sub-Cluster momentum |
| TLorentzVector | fSubClusterMomBoost | ! Sub-Cluster momentum boosted, armenteros |
| TLorentzVector | fSubClusterMomSum | ! Sub-Cluster momentum sum, armenteros |
| Float_t | fWSimu[2] | Constant and slope of the linear correction factor for the shower |
| TH2F* | fhAnglePairAfterCutsNLocMax1[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairAfterCutsNLocMax2[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairAfterCutsNLocMaxN[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairM02NLocMax1[7][2] | ! pair opening angle vs M02 for E > 7 GeV |
| TH2F* | fhAnglePairM02NLocMax2[7][2] | ! pair opening angle vs M02 for E > 7 GeV |
| TH2F* | fhAnglePairM02NLocMaxN[7][2] | ! pair opening angle vs M02 for E > 7 GeV |
| TH2F* | fhAnglePairMassNLocMax1[7][2] | ! pair opening angle vs Mass for E > 7 GeV |
| TH2F* | fhAnglePairMassNLocMax2[7][2] | ! pair opening angle vs Mass for E > 7 GeV |
| TH2F* | fhAnglePairMassNLocMaxN[7][2] | ! pair opening angle vs Mass for E > 7 GeV |
| TH2F* | fhAnglePairNLocMax1[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairNLocMax2[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairNLocMaxN[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairOverM02NLocMax1[7][2] | ! pair opening angle / m02 vs E, NLM=1 |
| TH2F* | fhAnglePairOverM02NLocMax1Overlap0[7][2] | ! pair opening angle / m02 vs E, NLM=1 |
| TH2F* | fhAnglePairOverM02NLocMax2[7][2] | ! pair opening angle / m02 vs E, NLM=2 |
| TH2F* | fhAnglePairOverM02NLocMax2Overlap0[7][2] | ! pair opening angle / m02 vs E, NLM=2 |
| TH2F* | fhAnglePairOverM02NLocMaxN[7][2] | ! pair opening angle / m02 vs E, NLM=N |
| TH2F* | fhAnglePairOverM02NLocMaxNOverlap0[7][2] | ! pair opening angle / m02 vs E, NLM=N |
| TH2F* | fhAnglePairPi0NLocMax1[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairPi0NLocMax2[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairPi0NLocMaxN[7][2] | ! pair opening angle vs E |
| TH2F* | fhAnglePairPrimPi0OverM02NLocMax1 | ! pair opening angle / m02 vs E, NLM=1, prim pi0 |
| TH2F* | fhAnglePairPrimPi0OverM02NLocMax2 | ! pair opening angle / m02 vs E, NLM=2, prim pi0 |
| TH2F* | fhAnglePairPrimPi0OverM02NLocMaxN | ! pair opening angle / m02 vs E, NLM=N, prim pi0 |
| TH2F* | fhAnglePairPrimPi0RecoNLocMax1 | ! pair opening angle pi0 generated/reconstructed vs E |
| TH2F* | fhAnglePairPrimPi0RecoNLocMax2 | ! pair opening angle pi0 generated/reconstructed vs E |
| TH2F* | fhAnglePairPrimPi0RecoNLocMaxN | ! pair opening angle pi0 generated/reconstructed vs E |
| TH2F* | fhAnglePairPrimPi0vsRecoNLocMax1 | ! pair opening angle pi0 generated vs reconstructed |
| TH2F* | fhAnglePairPrimPi0vsRecoNLocMax2 | ! pair opening angle pi0 generated vs reconstructed |
| TH2F* | fhAnglePairPrimPi0vsRecoNLocMaxN | ! pair opening angle pi0 generated vs reconstructed |
| TH2F* | fhArmAfterCutsNLocMax1[7][4] | ! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima = 1 |
| TH2F* | fhArmAfterCutsNLocMax2[7][4] | ! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima = 2 |
| TH2F* | fhArmAfterCutsNLocMaxN[7][4] | ! Armenteros after M02, asymmetry cuts for pi0, N Local Maxima > 2 |
| TH2F* | fhArmNLocMax1[7][4] | ! Armenteros of 2 highest energy cells when 1 local max vs E, 1-6 for different MC particle types |
| TH2F* | fhArmNLocMax2[7][4] | ! Armenteros of 2 cells local maxima vs E, 1-6 for different MC particle types |
| TH2F* | fhArmNLocMaxN[7][4] | ! Armenteros of >2 cells local maxima vs E, 1-6 for different MC particle types |
| TH2F* | fhArmPi0NLocMax1[7][4] | ! Armenteros for selected pi0, N Local Maxima = 1 |
| TH2F* | fhArmPi0NLocMax2[7][4] | ! Armenteros for selected pi0, N Local Maxima = 2 |
| TH2F* | fhArmPi0NLocMaxN[7][4] | ! Armenteros for selected pi0, N Local Maxima > 2 |
| TH2F* | fhAsyConNLocMax1[7][2] | ! Asy for Mass around close to 0, N Local Maxima = 1 |
| TH2F* | fhAsyConNLocMax2[7][2] | ! Asy for Mass around close to 0, N Local Maxima = 2 |
| TH2F* | fhAsyConNLocMaxN[7][2] | ! Asy for Mass around close to 0, N Local Maxima > 2 |
| TH2F* | fhAsyEtaNLocMax1[7][2] | ! Asy for Mass around eta, N Local Maxima = 1 |
| TH2F* | fhAsyEtaNLocMax2[7][2] | ! Asy for Mass around eta, N Local Maxima = 2 |
| TH2F* | fhAsyEtaNLocMaxN[7][2] | ! Asy for Mass around eta, N Local Maxima > 2 |
| TH2F* | fhAsyMCGenRecoDiffMCPi0[3] | ! reconstructed-generated asymmetry of splitted clusters vs E from pi0, for 3 NLM cases |
| TH2F* | fhAsyMCGenRecoDiffMCPi0Conv[3] | ! reconstructed-generated asymmetry of splitted clusters vs E from converted pi0, for 3 NLM cases |
| 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* | fhAsyPi0NLocMax1[7][2] | ! Asy for Mass around pi0, N Local Maxima = 1 |
| TH2F* | fhAsyPi0NLocMax2[7][2] | ! Asy for Mass around pi0, N Local Maxima = 2 |
| TH2F* | fhAsyPi0NLocMaxN[7][2] | ! Asy for Mass around pi0, N Local Maxima > 2 |
| TH2F* | fhAsymEnCutNLocMax1 | ! Asym(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhAsymEnCutNLocMax2 | ! Asym(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhAsymEnCutNLocMaxN | ! Asym(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM > 2 |
| TH2F* | fhAsymM02CutNLocMax1 | ! Asym(E) M02 selection, not matched, energy asymmetry of split clusters, NLM = 1 |
| TH2F* | fhAsymM02CutNLocMax2 | ! Asym(E) M02 selection, not matched, energy asymmetry of split clusters, NLM = 2 |
| TH2F* | fhAsymM02CutNLocMaxN | ! Asym(E) M02 selection, not matched, energy asymmetry of split clusters, NLM > 2 |
| 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* | fhCentralityEtaNLocMax1 | ! Centrality for selected eta, N Local Maxima = 1 |
| TH2F* | fhCentralityEtaNLocMax2 | ! Centrality for selected eta, N Local Maxima = 2 |
| TH2F* | fhCentralityEtaNLocMaxN | ! Centrality for selected eta, N Local Maxima > 2 |
| TH2F* | fhCentralityPi0NLocMax1 | ! Centrality for selected pi0, N Local Maxima = 1 |
| TH2F* | fhCentralityPi0NLocMax2 | ! Centrality for selected pi0, N Local Maxima = 2 |
| TH2F* | fhCentralityPi0NLocMaxN | ! Centrality for selected pi0, 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* | fhCosThStarAfterCutsNLocMax1[7][2] | ! cos(theta^star) vs E, after M02, asymmetry cuts, NLM=1 |
| TH2F* | fhCosThStarAfterCutsNLocMax2[7][2] | ! cos(theta^star) vs E, after M02, asymmetry cuts, NLM=2 |
| TH2F* | fhCosThStarAfterCutsNLocMaxN[7][2] | ! cos(theta^star) vs E, after M02, asymmetry cuts, NLM>2 |
| TH2F* | fhCosThStarNLocMax1[7][2] | ! cos(theta^star) vs E, NLM=1 |
| TH2F* | fhCosThStarNLocMax2[7][2] | ! cos(theta^star) vs E, NLM=2 |
| TH2F* | fhCosThStarNLocMaxN[7][2] | ! cos(theta^star) vs E, NLM>2 |
| TH2F* | fhCosThStarPi0NLocMax1[7][2] | ! cos(theta^star) vs E, after M02, asymmetry and pi0 mass cuts, NLM=1 |
| TH2F* | fhCosThStarPi0NLocMax2[7][2] | ! cos(theta^star) vs E, after M02, asymmetry and pi0 mass cuts, NLM=2 |
| TH2F* | fhCosThStarPi0NLocMaxN[7][2] | ! cos(theta^star) vs E, after M02, asymmetry and pi0 mass cuts, NLM>2 |
| TH2F* | fhEtaEPairDiffTimeNLM1 | ! E vs Pair of clusters time difference vs E, for selected eta, NLM=1 |
| TH2F* | fhEtaEPairDiffTimeNLM2 | ! E vs Pair of clusters time difference vs E, for selected eta, NLM=2 |
| TH2F* | fhEtaEPairDiffTimeNLMN | ! E vs Pair of clusters time difference vs E, for selected eta, NLM>2 |
| 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* | fhEventPlaneEtaNLocMax1 | ! Event plane for selected eta, N Local Maxima = 1 |
| TH2F* | fhEventPlaneEtaNLocMax2 | ! Event plane for selected eta, N Local Maxima = 2 |
| TH2F* | fhEventPlaneEtaNLocMaxN | ! Event plane for selected eta, N Local Maxima > 2 |
| TH2F* | fhEventPlanePi0NLocMax1 | ! Event plane for selected pi0, N Local Maxima = 1 |
| TH2F* | fhEventPlanePi0NLocMax2 | ! Event plane for selected pi0, N Local Maxima = 2 |
| TH2F* | fhEventPlanePi0NLocMaxN | ! Event plane for selected pi0, N Local Maxima > 2 |
| TH2F* | fhLM1NLocMax[7][2] | ! Split cluster 1 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types |
| TH2F* | fhLM1NLocMaxIdPi0[7][2] | ! Split cluster 1 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types, pi0 selection |
| TH2F* | fhLM1NLocMaxM02Cut[7][2] | ! Split cluster 1 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut |
| TH2F* | fhLM2NLocMax[7][2] | ! Split cluster 2 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types |
| TH2F* | fhLM2NLocMaxIdPi0[7][2] | ! Split cluster 2 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types, pi0 selection |
| TH2F* | fhLM2NLocMaxM02Cut[7][2] | ! Split cluster 2 E distribution vs Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut |
| TH2F* | fhM02AsyCutNLocMax1 | ! M02(E) asym selection, not matched, M02, NLM = 1 |
| TH2F* | fhM02AsyCutNLocMax2 | ! M02(E) asym selection, not matched, M02, NLM = 2 |
| TH2F* | fhM02AsyCutNLocMaxN | ! M02(E) asym selection, not matched, M02, NLM > 2 |
| TH2F* | fhM02BadDistClose[3] | ! m02 of clusters with second LM close to bad channel |
| TH2F* | fhM02ConNLocMax1[7][2] | ! M02 for Mass around close to 0, N Local Maxima = 1 |
| TH2F* | fhM02ConNLocMax2[7][2] | ! M02 for Mass around close to 0, N Local Maxima = 2 |
| TH2F* | fhM02ConNLocMaxN[7][2] | ! M02 for Mass around close to 0, N Local Maxima > 2 |
| TH2F* | fhM02ECellCutPi0[3][20] | ! M02 for selected pi0 with different cut on cell energy, with NLM = 1, = 2, > 2 |
| TH2F* | fhM02EnCutNLocMax1 | ! M02(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhM02EnCutNLocMax2 | ! M02(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhM02EnCutNLocMaxN | ! M02(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM > 2 |
| TH2F* | fhM02EtaNLocMax1[7][2] | ! M02 for Mass around eta, N Local Maxima = 1 |
| TH2F* | fhM02EtaNLocMax2[7][2] | ! M02 for Mass around eta, N Local Maxima = 2 |
| TH2F* | fhM02EtaNLocMaxN[7][2] | ! M02 for Mass around eta, N Local Maxima > 2 |
| 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* | 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* | fhM02NLocMaxDiffCut[5][5][3][2] | ! M02 for 3 kinds of number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks |
| TH2F* | fhM02NLocMaxDiffCutPi0[5][5][3][2] | ! M02 for 3 kinds of number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks, cluster selected as pi0 |
| TH2F* | fhM02NLocMaxN[7][2] | ! M02 vs E for N max in cluster > 2, 1-6 for different MC particle types |
| TH2F* | fhM02OnBorder[3] | ! m02 of clusters with second LM close to EMCAL border |
| TH2F* | fhM02Pi0NLocMax1[7][2] | ! M02 for Mass around pi0, N Local Maxima = 1 |
| TH2F* | fhM02Pi0NLocMax2[7][2] | ! M02 for Mass around pi0, N Local Maxima = 2 |
| TH2F* | fhM02Pi0NLocMaxN[7][2] | ! M02 for Mass around pi0, N Local Maxima > 2 |
| TH2F* | fhM02WeightPi0[3][20] | ! M02 for selected pi0 with different weight, with NLM = 1, = 2, > 2 |
| 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* | fhMCEAsymOverlap0[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, no other MC particles contributes, neutral cluster |
| TH2F* | fhMCEAsymOverlap0Match[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, no other MC particles contributes, charged cluster |
| TH2F* | fhMCEAsymOverlap1[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, 1 other MC particles contributes, neutral cluster |
| TH2F* | fhMCEAsymOverlap1Match[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, 1 other MC particles contributes, charged cluster |
| TH2F* | fhMCEAsymOverlapN[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, N other MC particles contributes, neutral cluster |
| TH2F* | fhMCEAsymOverlapNMatch[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, N other MC particles contributes, charged cluster |
| TH2F* | fhMCEEpriOverlap0[3][7] | ! E reco vs primary for different MC origin, no other MC particles contributes, neutral cluster |
| TH2F* | fhMCEEpriOverlap0IdPi0[3][7] | ! E reco vs primary for different MC origin, no other MC particles contributes, neutral cluster, neutral clusters id as pi0 |
| TH2F* | fhMCEEpriOverlap0Match[3][7] | ! E reco vs primary for different MC origin, no other MC particles contributes, charged cluster |
| TH2F* | fhMCEEpriOverlap1[3][7] | ! E reco vs primary for different MC origin, 1 other MC particles contributes, neutral cluster |
| TH2F* | fhMCEEpriOverlap1IdPi0[3][7] | ! E reco vs primary for different MC origin, 1 other MC particles contributes, neutral cluster, neutral clusters id as pi0 |
| TH2F* | fhMCEEpriOverlap1Match[3][7] | ! E reco vs primary for different MC origin, 1 other MC particles contributes, charged cluster |
| TH2F* | fhMCEEpriOverlapN[3][7] | ! E reco vs primary for different MC origin, N other MC particles contributes, neutral cluster |
| TH2F* | fhMCEEpriOverlapNIdPi0[3][7] | ! E reco vs primary for different MC origin, 1 other MC particles contributes, neutral cluster, neutral clusters is as pi0 |
| TH2F* | fhMCEEpriOverlapNMatch[3][7] | ! E reco vs primary for different MC origin, N other MC particles contributes, charged cluster |
| TH2F* | fhMCEM02Overlap0[3][7] | ! E vs M02 for different MC origin, no other MC particles contributes, neutral cluster |
| TH2F* | fhMCEM02Overlap0Match[3][7] | ! E vs M02 for different MC origin, no other MC particles contributes, charged cluster |
| TH2F* | fhMCEM02Overlap1[3][7] | ! E vs M02 for different MC origin, 1 other MC particles contributes, neutral cluster |
| TH2F* | fhMCEM02Overlap1Match[3][7] | ! E vs M02 for different MC origin, 1 other MC particles contributes, charged cluster |
| TH2F* | fhMCEM02OverlapN[3][7] | ! E vs M02 for different MC origin, N other MC particles contributes, neutral cluster |
| TH2F* | fhMCEM02OverlapNMatch[3][7] | ! E vs M02 for different MC origin, N other MC particles contributes, charged cluster |
| TH2F* | fhMCEMassOverlap0[3][7] | ! E vs Mass for different MC origin, no other MC particles contributes, neutral cluster |
| TH2F* | fhMCEMassOverlap0Match[3][7] | ! E vs Mass for different MC origin, no other MC particles contributes, charged cluster |
| TH2F* | fhMCEMassOverlap1[3][7] | ! E vs Mass for different MC origin, 1 other MC particles contributes, neutral cluster |
| TH2F* | fhMCEMassOverlap1Match[3][7] | ! E vs Mass for different MC origin, 1 other MC particles contributes, charged cluster |
| TH2F* | fhMCEMassOverlapN[3][7] | ! E vs Mass for different MC origin, N other MC particles contributes, neutral cluster |
| TH2F* | fhMCEMassOverlapNMatch[3][7] | ! E vs Mass for different MC origin, N other MC particles contributes, charged cluster |
| TH2F* | fhMCENCellOverlap0[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, no other MC particles contributes, neutral cluster |
| TH2F* | fhMCENCellOverlap0Match[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, no other MC particles contributes, charged cluster |
| TH2F* | fhMCENCellOverlap1[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, 1 other MC particles contributes, neutral cluster |
| TH2F* | fhMCENCellOverlap1Match[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, 1 other MC particles contributes, charged cluster |
| TH2F* | fhMCENCellOverlapN[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, N other MC particles contributes, neutral cluster |
| TH2F* | fhMCENCellOverlapNMatch[3][7] | ! E vs sum of splitted cluster energy asymmetry for different MC origin, N other MC particles contributes, charged cluster |
| TH2F* | fhMCENOverlaps[3][7] | ! E vs number of Overlaps in MC, neutral cluster |
| TH2F* | fhMCENOverlapsMatch[3][7] | ! E vs number of Overlaps in MC, charged cluster |
| TH2F* | fhMCEOverlapType | ! what particles overlap with pi0, neutral clusters |
| TH2F* | fhMCEOverlapTypeMatch | ! what particles overlap with pi0, charged clusters |
| TH2F* | fhMCESplitEFracOverlap0[3][7] | ! E vs sum of splitted cluster energy / cluster energy for different MC origin, no other MC particles contributes, neutral cluster |
| TH2F* | fhMCESplitEFracOverlap0Match[3][7] | ! E vs sum of splitted cluster energy / cluster energy for different MC origin, no other MC particles contributes, charged cluster |
| TH2F* | fhMCESplitEFracOverlap1[3][7] | ! E vs sum of splitted cluster energy / cluster energy for different MC origin, 1 other MC particles contributes, neutral cluster |
| TH2F* | fhMCESplitEFracOverlap1Match[3][7] | ! E vs sum of splitted cluster energy / cluster energy for different MC origin, 1 other MC particles contributes, charged cluster |
| TH2F* | fhMCESplitEFracOverlapN[3][7] | ! E vs sum of splitted cluster energy / cluster energy for different MC origin, N other MC particles contributes, neutral cluster |
| TH2F* | fhMCESplitEFracOverlapNMatch[3][7] | ! E vs sum of splitted cluster energy / cluster energy for different MC origin, N other MC particles contributes, charged cluster |
| 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* | 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* | 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* | 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* | fhMCGenFracNLocMax1NoOverlap[7][2] | ! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, no overlap found |
| 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* | fhMCGenFracNLocMax2NoOverlap[7][2] | ! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, no overlap found |
| 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* | 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* | fhMCGenFracNLocMaxNNoOverlap[7][2] | ! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, no overlap found |
| 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* | 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* | fhMCGenSplitEFracNLocMax1NoOverlap[7][2] | ! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types, no overlap |
| 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* | fhMCGenSplitEFracNLocMax2NoOverlap[7][2] | ! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types, no overlap |
| 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* | fhMCGenSplitEFracNLocMaxNNoOverlap[7][2] | ! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster > 2, 1-6 for different MC particle types, no overlap |
| TH2F* | fhMCPi0AnyNLMPair | ! E vs NLM when cluster originated in pi0 merging and a both highest energy pairs and other pairs correspond to 2 photons |
| TH2F* | fhMCPi0AnyNLMPairNoMCMatch | ! E vs NLM when cluster originated in pi0 merging and a both highest energy pairs and other pairs correspond to 2 photons |
| TH2F* | fhMCPi0AnyNLMPairNoMCMatchOverlap | ! E vs NLM when cluster originated in pi0 merging and a both highest energy pairs and other pairs correspond to 2 photons, overlap |
| TH2F* | fhMCPi0AnyNLMPairOverlap | ! E vs NLM when cluster originated in pi0 merging and a both highest energy pairs and other pairs correspond to 2 photons, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjHighLM | ! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMDiffELM1[3] | ! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMDiffELM1vsELM1[3] | ! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMDiffELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMDiffELM2vsELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMOverlap | ! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMOverlapDiffELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMOverlapDiffELM1vsELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMOverlapDiffELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMOverlapDiffELM2vsELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjHighLMOverlapMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the adjacent cell local maxima, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLM | ! E vs NLM when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMDiffELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMDiffELM1vsELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMDiffELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMDiffELM2vsELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMOverlap | ! E vs NLM when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMOverlapDiffELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMOverlapDiffELM1vsELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMOverlapDiffELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMOverlapDiffELM2vsELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjOtherLMOverlapMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay do not hit the adjacent cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjacent | ! E vs NLM when cluster originated in pi0 merging and MC photon decay hit adjacen cells, not 2 LM |
| TH2F* | fhMCPi0DecayPhotonAdjacentMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay hit adjacen cells, not 2 LM |
| TH2F* | fhMCPi0DecayPhotonAdjacentOverlap | ! E vs NLM when cluster originated in pi0 merging and MC photon decay hit adjacen cells, not 2 LM, overlap |
| TH2F* | fhMCPi0DecayPhotonAdjacentOverlapMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay hit adjacen cells, not 2 LM, overlap |
| TH2F* | fhMCPi0DecayPhotonHitHighLM | ! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMDiffELM1[3] | ! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMDiffELM1vsELM1[3] | ! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMDiffELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMDiffELM2vsELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMOverlap | ! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the cell local maxima, overlap |
| TH2F* | fhMCPi0DecayPhotonHitHighLMOverlapDiffELM1[3] | ! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMOverlapDiffELM1vsELM1[3] | ! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMOverlapDiffELM2[3] | ! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMOverlapDiffELM2vsELM2[3] | ! E vs Ephoton-Esplit cluster when cluster originated in pi0 merging and MC photon decay hit the cell local maxima |
| TH2F* | fhMCPi0DecayPhotonHitHighLMOverlapMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the cell local maxima, overlap |
| TH2F* | fhMCPi0DecayPhotonHitNoLM | ! E vs NLM when cluster originated in pi0 merging and MC photon decay do not hit the cell local maximas |
| TH2F* | fhMCPi0DecayPhotonHitNoLMMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay do not hit the cell local maximas |
| TH2F* | fhMCPi0DecayPhotonHitNoLMOverlap | ! E vs NLM when cluster originated in pi0 merging and MC photon decay do not hit the cell local maximas, overlap |
| TH2F* | fhMCPi0DecayPhotonHitNoLMOverlapMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay do not hit the cell local maximas, overlap |
| TH2F* | fhMCPi0DecayPhotonHitOtherLM | ! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMDiffELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMDiffELM1vsELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMDiffELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMDiffELM2vsELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMOverlap | ! E vs NLM when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMOverlapDiffELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMOverlapDiffELM1vsELM1[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMOverlapDiffELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMOverlapDiffELM2vsELM2[3] | ! E vs Ephoton-Esplit when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap |
| TH2F* | fhMCPi0DecayPhotonHitOtherLMOverlapMass[3] | ! E vs Mass when cluster originated in pi0 merging and MC photon decay hit the cell local maximas, not high, overlap |
| TH2F* | fhMCPi0HighNLMPair | ! E vs NLM when cluster originated in pi0 merging and highest energy local maxima correspond to 2 photons |
| TH2F* | fhMCPi0HighNLMPairNoMCMatch | ! E vs NLM when cluster originated in pi0 merging and highest energy local maxima correspond to 2 photons |
| TH2F* | fhMCPi0HighNLMPairNoMCMatchOverlap | ! E vs NLM when cluster originated in pi0 merging and highest energy local maxima correspond to 2 photons, overlap |
| TH2F* | fhMCPi0HighNLMPairOverlap | ! E vs NLM when cluster originated in pi0 merging and highest energy local maxima correspond to 2 photons, overlap |
| TH2F* | fhMCPi0LowNLMPair | ! E vs NLM when cluster originated in pi0 merging and a pair of local maxima except highest energy correspond to 2 photons |
| TH2F* | fhMCPi0LowNLMPairNoMCMatch | ! E vs NLM when cluster originated in pi0 merging and a pair of local maxima except highest energy correspond to 2 photons |
| TH2F* | fhMCPi0LowNLMPairNoMCMatchOverlap | ! E vs NLM when cluster originated in pi0 merging and a pair of local maxima except highest energy correspond to 2 photons, overlap |
| TH2F* | fhMCPi0LowNLMPairOverlap | ! E vs NLM when cluster originated in pi0 merging and a pair of local maxima except highest energy correspond to 2 photons, overlap |
| TH2F* | fhMCPi0MassM02Overlap0[3][4] | ! MC Pi0 M02 vs Mass for different MC origin, no other MC particles contributes, neutral cluster, 4 E bins |
| TH2F* | fhMCPi0MassM02Overlap0Match[3][4] | ! MC Pi0 M02 vs Mass for different MC origin, no other MC particles contributes, charged cluster, 4 E bins |
| TH2F* | fhMCPi0MassM02Overlap1[3][4] | ! MC Pi0 M02 vs Mass for different MC origin, 1 other MC particles contributes, neutral cluster, 4 E bins |
| TH2F* | fhMCPi0MassM02Overlap1Match[3][4] | ! MC Pi0 M02 vs Mass for different MC origin, 1 other MC particles contributes, charged cluster, 4 E bins |
| TH2F* | fhMCPi0MassM02OverlapN[3][4] | ! MC Pi0 M02 vs Mass for different MC origin, N other MC particles contributes, neutral cluster, 4 E bins |
| TH2F* | fhMCPi0MassM02OverlapNMatch[3][4] | ! MC Pi0 M02 vs Mass for different MC origin, N other MC particles contributes, charged cluster, 4 E bins |
| TH2F* | fhMCPi0NoneNLMPair | ! E vs NLM when cluster originated in pi0 merging and a both no NLM corresponds to the photons |
| TH2F* | fhMCPi0NoneNLMPairNoMCMatch | ! E vs NLM when cluster originated in pi0 merging and a both no NLM corresponds to the photons |
| TH2F* | fhMCPi0NoneNLMPairNoMCMatchOverlap | ! E vs NLM when cluster originated in pi0 merging and a both no NLM corresponds to the photons, overlap |
| TH2F* | fhMCPi0NoneNLMPairOverlap | ! E vs NLM when cluster originated in pi0 merging and a both no NLM corresponds to the photons, overlap |
| TH2F* | fhMassAfterCutsNLocMax1[7][2] | ! Mass after M02, asymmetry cuts for MC part, N Local Maxima = 1 |
| TH2F* | fhMassAfterCutsNLocMax2[7][2] | ! Mass after M02, asymmetry cuts for MC part, N Local Maxima = 2 |
| TH2F* | fhMassAfterCutsNLocMaxN[7][2] | ! Mass after M02, asymmetry cuts for MC part, N Local Maxima > 2 |
| TH2F* | fhMassAsyCutNLocMax1 | ! Mass(E) asym selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhMassAsyCutNLocMax2 | ! Mass(E) asym selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhMassAsyCutNLocMaxN | ! Mass(E) asym selection, not matched, Mass of split clusters, NLM > 2 |
| 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* | fhMassBadDistClose[3] | ! split mass of clusters with second LM close to bad channel |
| TH2F* | fhMassConNLocMax1[7][2] | ! Mass for selected around close to 0, N Local Maxima = 1 |
| TH2F* | fhMassConNLocMax2[7][2] | ! Mass for selected around close to 0, N Local Maxima = 2 |
| TH2F* | fhMassConNLocMaxN[7][2] | ! Mass for selected around close to 0, N Local Maxima > 2 |
| TH2F* | fhMassDispAsyNLocMax1[7][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* | fhMassDispAsyNLocMax1Ebin[4] | ! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters |
| TH2F* | fhMassDispAsyNLocMax2[7][2] | ! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types |
| TH2F* | fhMassDispAsyNLocMax2Ebin[4] | ! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters |
| TH2F* | fhMassDispAsyNLocMaxN[7][2] | ! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types |
| TH2F* | fhMassDispAsyNLocMaxNEbin[4] | ! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters |
| TH2F* | fhMassDispEtaNLocMax1[7][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* | fhMassDispEtaNLocMax1Ebin[4] | ! Mass of 2 highest energy cells when 1 local max, vs M02, 4 E bins, neutral clusters |
| TH2F* | fhMassDispEtaNLocMax2[7][2] | ! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types |
| TH2F* | fhMassDispEtaNLocMax2Ebin[4] | ! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters |
| TH2F* | fhMassDispEtaNLocMaxN[7][2] | ! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types |
| 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 > 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* | fhMassDispPhiNLocMax2[7][2] | ! Mass of 2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types |
| TH2F* | fhMassDispPhiNLocMax2Ebin[4] | ! Mass of 2 cells local maxima, vs M02, 4 E bins, neutral clusters |
| TH2F* | fhMassDispPhiNLocMaxN[7][2] | ! Mass of >2 cells local maxima, vs M02, for E > 8 GeV, 1-6 for different MC particle types |
| TH2F* | fhMassDispPhiNLocMaxNEbin[4] | ! Mass of >2 cells local maxima, vs M02, 4 E bins, neutral clusters |
| TH2F* | fhMassEnCutNLocMax1 | ! Mass(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhMassEnCutNLocMax2 | ! Mass(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhMassEnCutNLocMaxN | ! Mass(E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM > 2 |
| TH2F* | fhMassEtaNLocMax1[7][2] | ! Mass for selected around eta, N Local Maxima = 1 |
| TH2F* | fhMassEtaNLocMax2[7][2] | ! Mass for selected around eta, N Local Maxima = 2 |
| TH2F* | fhMassEtaNLocMaxN[7][2] | ! Mass for selected around eta, N Local Maxima > 2 |
| TH2F* | fhMassM02CutNLocMax1 | ! Mass(E) M02 selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhMassM02CutNLocMax2 | ! Mass(E) M02 selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhMassM02CutNLocMaxN | ! Mass(E) M02 selection, not matched, Mass of split clusters, NLM > 2 |
| TH2F* | fhMassM02NLocMax1[7][2] | ! Mass of splitted clusters when 1 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* | fhMassM02NLocMax2[7][2] | ! Mass of splitted clusters when 2 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types |
| TH2F* | fhMassM02NLocMax2Ebin[4] | ! Mass of splitted clusters when 2 local max vs M02, 4 E bins, neutral clusters |
| TH2F* | fhMassM02NLocMaxN[7][2] | ! Mass of splitted clusters when >2 local max vs M02, for E > 8 GeV, 1-6 for different MC particle types |
| TH2F* | fhMassM02NLocMaxNEbin[4] | ! Mass of splitted clusters when >2 local max vs M02, 4 E bins, neutral clusters |
| 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* | fhMassNLocMax1[7][2] | ! Split Inv Mass vs cluster E, NLM=1, different MC particle types, track matching on/off |
| TH2F* | fhMassNLocMax2[7][2] | ! Split Inv Mass vs cluster E, NLM=2, different MC particle types, track matching on/off |
| TH2F* | fhMassNLocMaxDiffCut[5][5][3][2] | ! Mass for 3 kinds of number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks |
| TH2F* | fhMassNLocMaxDiffCutPi0[5][5][3][2] | ! M02 for 3 kinds of number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks |
| TH2F* | fhMassNLocMaxN[7][2] | ! Split Inv Mass vs cluster E, NLM>2, different MC particle types, track matching on/off |
| TH2F* | fhMassOnBorder[3] | ! split mass of clusters with second LM on EMCAL border |
| TH2F* | fhMassPi0NLocMax1[7][2] | ! Mass for selected pi0, N Local Maxima = 1 |
| TH2F* | fhMassPi0NLocMax2[7][2] | ! Mass for selected around pi0, N Local Maxima = 2 |
| TH2F* | fhMassPi0NLocMaxN[7][2] | ! Mass for selected around pi0, N Local Maxima > 2 |
| TH2F* | fhMassSplitEAfterCutsNLocMax1[7][2] | ! Split Inv Mass vs E1+E2, NLM=1, after M02, asymmetry cuts, different MC particle types, track matching on/off |
| TH2F* | fhMassSplitEAfterCutsNLocMax2[7][2] | ! Split Inv Mass vs E1+E2, NLM=2, after M02, asymmetry cuts, different MC particle types, track matching on/off |
| TH2F* | fhMassSplitEAfterCutsNLocMaxN[7][2] | ! Split Inv Mass vs E1+E2, NLM>2, after M02, asymmetry cuts, different MC particle types, track matching on/off |
| 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* | 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* | fhMassSplitENLocMax1[7][2] | ! Split Inv Mass vs E1+E2, NLM=1, different MC particle types, track matching on/off |
| TH2F* | fhMassSplitENLocMax2[7][2] | ! Split Inv Mass vs E1+E2, NLM=2, different MC particle types, track matching on/off |
| TH2F* | fhMassSplitENLocMaxN[7][2] | ! Split Inv Mass vs E1+E2, NLM>2, different MC particle types, track matching on/off |
| TH2F* | fhMassSplitEPi0NLocMax1[7][2] | ! Split Inv Mass vs E1+E2, NLM=1, after pi0 selection, different MC particle types, track matching on/off |
| TH2F* | fhMassSplitEPi0NLocMax2[7][2] | ! Split Inv Mass vs E1+E2, NLM=2, after pi0 selection, different MC particle types, track matching on/off |
| TH2F* | fhMassSplitEPi0NLocMaxN[7][2] | ! Split Inv Mass vs E1+E2, NLM>2, after pi0 selection, different MC particle types, track matching on/off |
| TH2F* | fhNCellEtaNLocMax1[7][2] | ! n cells for selected around eta, N Local Maxima = 1 |
| TH2F* | fhNCellEtaNLocMax2[7][2] | ! n cells for selected around eta, N Local Maxima = 2 |
| TH2F* | fhNCellEtaNLocMaxN[7][2] | ! n cells for selected around eta, N Local Maxima > 2 |
| TH2F* | fhNCellM02EHighNLocMax1MCPi0 | ! n cells in cluster vs m02 for high energy clusters, for N max in cluster = 1, for MC pi0 |
| TH2F* | fhNCellM02EHighNLocMax2MCPi0 | ! n cells in cluster vs m02 for high energy clusters, for N max in cluster = 2, for MC pi0 |
| TH2F* | fhNCellM02EHighNLocMaxNMCPi0 | ! n cells in cluster vs m02 for high energy clusters, for N max in cluster > 2, for MC pi0 |
| TH2F* | fhNCellM02ELowNLocMax1MCPi0 | ! n cells in cluster vs m02 for low energy clusters, for N max in cluster = 1, for MC pi0 |
| TH2F* | fhNCellM02ELowNLocMax2MCPi0 | ! n cells in cluster vs m02 for low energy clusters, for N max in cluster = 2, for MC pi0 |
| TH2F* | fhNCellM02ELowNLocMaxNMCPi0 | ! n cells in cluster vs m02 for low energy clusters, for N max in cluster > 2, for MC pi0 |
| TH2F* | fhNCellMassEHighNLocMax1MCPi0 | ! n cells in cluster vs mass for high energy clusters, for N max in cluster = 1, for MC pi0 |
| TH2F* | fhNCellMassEHighNLocMax2MCPi0 | ! n cells in cluster vs mass for high energy clusters, for N max in cluster = 2, for MC pi0 |
| TH2F* | fhNCellMassEHighNLocMaxNMCPi0 | ! n cells in cluster vs mass for high energy clusters, for N max in cluster > 2, for MC pi0 |
| TH2F* | fhNCellMassELowNLocMax1MCPi0 | ! n cells in cluster vs mass for low energy clusters, for N max in cluster = 1, for MC pi0 |
| TH2F* | fhNCellMassELowNLocMax2MCPi0 | ! n cells in cluster vs mass for low energy clusters, for N max in cluster = 2, for MC pi0 |
| TH2F* | fhNCellMassELowNLocMaxNMCPi0 | ! n cells in cluster vs mass for low energy clusters, for N max in cluster > 2, for MC pi0 |
| 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* | fhNCellPi0NLocMax1[7][2] | ! n cells for selected around pi0, N Local Maxima = 1 |
| TH2F* | fhNCellPi0NLocMax2[7][2] | ! n cells for selected around pi0, N Local Maxima = 2 |
| TH2F* | fhNCellPi0NLocMaxN[7][2] | ! n cells for selected around pi0, N Local Maxima > 2 |
| TH2F* | fhNLocMax[7][2] | ! Number of maxima in cluster vs E, 1-6 for different MC particle types |
| TH2F* | fhNLocMaxDiffCut[5][5][2] | ! Number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks |
| TH2F* | fhNLocMaxDiffCutPi0[5][5][2] | ! Number of maxima for different values of min Loc Max value and min difference between cells, matched/unmatched with tracks, cluster selected as pi0 |
| TH2F* | fhNLocMaxIdPi0[7][2] | ! Number of maxima in cluster vs E, 1-6 for different MC particle types, after pi0 selection |
| TH2F* | fhNLocMaxM02Cut[7][2] | ! Number of maxima in cluster vs E, 1-6 for different MC particle types, after SS cut |
| 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* | fhPi0CellEMax2ClusterFrac[3] | ! pi0's energy vs energy fraction of second LM and cluster 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* | fhPi0CellEMaxClusterFrac[3] | ! pi0's energy vs energy fraction of main LM and cluster energy with NLM = 1, = 2, > 2 |
| TH2F* | fhPi0CellEMaxEMax2Frac[3] | ! pi0's energy vs fraction of 2 main maxima 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* | fhPi0CellLogEFrac[3] | ! pi0's energy vs cluster log cell energy fraction with NLM = 1, = 2, > 2 |
| TH2F* | fhPi0EPairDiffTimeNLM1 | ! E vs Pair of clusters time difference vs E, for selected pi0, NLM=1 |
| TH2F* | fhPi0EPairDiffTimeNLM2 | ! E vs Pair of clusters time difference vs E, for selected pi0, NLM=2 |
| TH2F* | fhPi0EPairDiffTimeNLMN | ! E vs Pair of clusters time difference vs E, for selected pi0, NLM>2 |
| 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* | fhSplitClusterENLocMax[7][2] | ! Number of maxima in cluster vs E of splitted clusters, 1-6 for different MC particle types |
| TH2F* | fhSplitClusterEPi0NLocMax[7][2] | ! Number of maxima in cluster vs E of splitted clusters when cluster id as pi0, 1-6 for different MC particle types |
| TH2F* | fhSplitEFracEnCutNLocMax1 | ! Split E fraction (E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhSplitEFracEnCutNLocMax2 | ! Split E fraction (E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM = 1 |
| TH2F* | fhSplitEFracEnCutNLocMaxN | ! Split E fraction (E) E sub-cluster cut selection, not matched, Mass of split clusters, NLM > 2 |
| TH2F* | fhSplitEFractionAfterCutsNLocMax1[7][2] | ! sum of splitted cluster energy / cluster energy for N Local Maxima = 1, after M02 and asymmetry cut |
| TH2F* | fhSplitEFractionAfterCutsNLocMax2[7][2] | ! sum of splitted cluster energy / cluster energy for N Local Maxima = 2, after M02 and asymmetry cut |
| TH2F* | fhSplitEFractionAfterCutsNLocMaxN[7][2] | ! sum of splitted cluster energy / cluster energy for N Local Maxima > 2, after M02 and asymmetry cut |
| 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* | 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* | fhTrackMatchedDEtaNLocMax1[7] | ! Eta distance between track and cluster vs cluster E, 1 local maximum |
| TH2F* | fhTrackMatchedDEtaNLocMax1Neg[7] | ! Eta distance between track and cluster vs cluster E, 1 local maximum |
| TH2F* | fhTrackMatchedDEtaNLocMax1Pos[7] | ! Eta distance between track and cluster vs cluster E, 1 local maximum |
| TH2F* | fhTrackMatchedDEtaNLocMax2[7] | ! Eta distance between track and cluster vs cluster E, 2 local maximum |
| TH2F* | fhTrackMatchedDEtaNLocMax2Neg[7] | ! Eta distance between track and cluster vs cluster E, 2 local maximum |
| TH2F* | fhTrackMatchedDEtaNLocMax2Pos[7] | ! Eta distance between track and cluster vs cluster E, 2 local maximum |
| TH2F* | fhTrackMatchedDEtaNLocMaxN[7] | ! Eta distance between track and cluster vs cluster E, more than 2 local maximum |
| TH2F* | fhTrackMatchedDEtaNLocMaxNNeg[7] | ! Eta distance between track and cluster vs cluster E, more than 2 local maximum |
| TH2F* | fhTrackMatchedDEtaNLocMaxNPos[7] | ! Eta distance between track and cluster vs cluster E, more than 2 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMax1[7] | ! Phi distance between track and cluster vs cluster E, 1 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMax1Neg[7] | ! Phi distance between track and cluster vs cluster E, 1 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMax1Pos[7] | ! Phi distance between track and cluster vs cluster E, 1 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMax2[7] | ! Phi distance between track and cluster vs cluster E, 2 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMax2Neg[7] | ! Phi distance between track and cluster vs cluster E, 2 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMax2Pos[7] | ! Phi distance between track and cluster vs cluster E, 2 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMaxN[7] | ! Phi distance between track and cluster vs cluster E, more than 2 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMaxNNeg[7] | ! Phi distance between track and cluster vs cluster E, more than 2 local maximum |
| TH2F* | fhTrackMatchedDPhiNLocMaxNPos[7] | ! Phi distance between track and cluster vs cluster E, more than 2 local maximum |
Class Charts
| Inheritance Chart: | ||||||||||||
|
Function documentation
void CheckLocalMaximaMCOrigin(AliVCluster* cluster, Int_t mcindex, Int_t noverlaps, Float_t e1, Float_t e2, Float_t mass)
Float_t m02, TLorentzVector l1, TLorentzVector l2) Check origin NLM tower of the cluster, when MC gives merged pi0
void FillAngleHistograms(Int_t nMax, Bool_t matched, Int_t mcindex, Float_t en, Float_t e1, Float_t e2, Float_t angle, Float_t mass, Float_t anglePrim, Float_t m02, Float_t asym, Int_t pid, Int_t noverlaps)
Fill histograms related to opening angle
void FillArmenterosHistograms(Int_t nMax, Int_t ebin, Int_t mcindex, Float_t pi0E, Float_t m02, Int_t pid)
Fill Armeteros type histograms
void FillThetaStarHistograms(Int_t nMax, Bool_t matched, Int_t mcindex, Float_t pi0E, Float_t m02, Int_t pid)
Fill cos Theta^star histograms
void FillEBinHistograms(Int_t ebin, Int_t nMax, Int_t mcindex, Float_t splitFrac, Float_t mass, Float_t asym, Float_t l0)
Fill some histograms integrating in few energy bins
void FillHistograms1(Float_t en, Float_t e1, Float_t e2, Int_t nMax, Float_t mass, Float_t l0, Float_t eta, Float_t phi, Bool_t matched, Int_t mcindex)
Fill histograms for clusters before any selection after spliting
void FillHistograms2(Float_t en, Float_t eprim, Float_t e1, Float_t e2, Int_t nMax, Float_t mass, Float_t l0, Bool_t matched, Int_t mcindex)
Fill histograms for clusters passing the first M02 selection
void FillIdPi0Histograms(Float_t en, Float_t e1, Float_t e2, Int_t nc, Int_t nMax, Float_t t12diff, Float_t mass, Float_t l0, Float_t eta, Float_t phi, Bool_t matched, Int_t mcindex)
Fill histograms for clusters passing the pi0 selection
void FillIdEtaHistograms(Float_t en, Float_t e1, Float_t e2, Int_t nc, Int_t nMax, Float_t t12diff, Float_t mass, Float_t l0, Float_t eta, Float_t phi, Bool_t matched, Int_t mcindex)
Fill histograms for clusters passing the eta selection
void FillIdConvHistograms(Float_t en, Int_t nMax, Float_t asym, Float_t mass, Float_t l0, Bool_t matched, Int_t mcindex)
Fill histograms for clusters passing the photon selection
void FillMCHistograms(Float_t en, Float_t e1, Float_t e2, Int_t ebin, Int_t mcindex, Int_t noverlaps, Float_t l0, Float_t mass, Int_t nMax, Bool_t matched, Float_t splitFrac, Float_t asym, Float_t eprim, Float_t asymGen)
Fill histograms needing some MC input
void FillMCOverlapHistograms(Float_t en, Float_t enprim, Int_t nc, Float_t mass, Float_t l0, Float_t asym, Float_t splitFrac, Int_t nlm, Int_t ebin, Bool_t matched, Int_t mcindex, Int_t noverlaps)
Fill histograms for MC Overlaps
void FillNCellHistograms(Int_t ncells, Float_t energy, Int_t nMax, Bool_t matched, Int_t mcindex, Float_t mass, Float_t l0)
Fill optional histograms with more SS parameters
void FillNLMDiffCutHistograms(AliVCluster* cluster, AliVCaloCells* cells, Bool_t matched)
Calculate NLM for different settings
void FillSSExtraHistograms(AliVCluster* cluster, Int_t nMax, Bool_t matched, Int_t mcindex, Float_t mass, Int_t ebin)
Fill optional histograms with more SS parameters
void FillSSWeightHistograms(AliVCluster* cluster, Int_t nlm, Int_t absId1, Int_t absId2)
Calculate weights and fill histograms
void FillTrackMatchingHistograms(AliVCluster* cluster, Int_t nMax, Int_t mcindex)
Fill histograms related to track matching
TList * GetCreateOutputObjects()
Create histograms to be saved in output file and store them in outputContainer
void GetMCIndex(AliVCluster* cluster, Int_t& mcindex, Int_t& mcTag)
void GetMCPrimaryKine(AliVCluster* cluster, Int_t mcindex, Int_t mcTag, Bool_t matched, Float_t& eprim, Float_t& asymGen, Float_t& angleGen, Int_t& noverlaps)
Check origin of the candidates, get primary kinematics if overlapped meson decay
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.)
Calculates new center of gravity in the local EMCAL-module coordinates and tranfers into global ALICE coordinates Calculates Dispersion and main axis