fhMassM02NLocMax1Ebin[i] = 0 ;
fhMassM02NLocMax2Ebin[i] = 0 ;
fhMassM02NLocMaxNEbin[i] = 0 ;
+
+ fhMassAsyNLocMax1Ebin[i] = 0 ;
+ fhMassAsyNLocMax2Ebin[i] = 0 ;
+ fhMassAsyNLocMaxNEbin[i] = 0 ;
+
+ fhAsyMCGenRecoNLocMax1EbinPi0[i] = 0 ;
+ fhAsyMCGenRecoNLocMax2EbinPi0[i] = 0 ;
+ fhAsyMCGenRecoNLocMaxNEbinPi0[i] = 0 ;
fhMassDispEtaNLocMax1Ebin[i] = 0 ;
fhMassDispEtaNLocMax2Ebin[i] = 0 ;
for(Int_t i = 0; i < 4; i++)
{
- if(IsDataMC())
- {
- fhMCAsymM02NLocMax1MCPi0Ebin[i] = new TH2F(Form("hMCAsymM02NLocMax1MCPi0Ebin%d",i),
- Form("Asymmetry of MC #pi^{0} of 2 highest energy cells #lambda_{0}^{2}, E bin %d",i),
- ssbins,ssmin,ssmax,100,0,1);
- fhMCAsymM02NLocMax1MCPi0Ebin[i]->SetYTitle("Decay asymmetry");
- fhMCAsymM02NLocMax1MCPi0Ebin[i]->SetXTitle("#lambda_{0}^{2}");
- outputContainer->Add(fhMCAsymM02NLocMax1MCPi0Ebin[i]) ;
-
- fhMCAsymM02NLocMax2MCPi0Ebin[i] = new TH2F(Form("hMCAsymM02NLocMax2MCPi0Ebin%d",i),
- Form("Asymmetry of MC #pi^{0} of 2 local maxima cells #lambda_{0}^{2}, E bin %d",i),
- ssbins,ssmin,ssmax,100,0,1);
- fhMCAsymM02NLocMax2MCPi0Ebin[i]->SetYTitle("Decay asymmetry");
- fhMCAsymM02NLocMax2MCPi0Ebin[i]->SetXTitle("#lambda_{0}^{2}");
- outputContainer->Add(fhMCAsymM02NLocMax2MCPi0Ebin[i]) ;
-
- fhMCAsymM02NLocMaxNMCPi0Ebin[i] = new TH2F(Form("hMCAsymM02NLocMaxNMCPi0Ebin%d",i),
- Form("Asymmetry of MC #pi^{0} of N>2 local maxima cells vs #lambda_{0}^{2}, E bin %d",i),
- ssbins,ssmin,ssmax,100,0,1);
- fhMCAsymM02NLocMaxNMCPi0Ebin[i]->SetYTitle("Decay asymmetry");
- fhMCAsymM02NLocMaxNMCPi0Ebin[i]->SetXTitle("#lambda_{0}^{2}");
- outputContainer->Add(fhMCAsymM02NLocMaxNMCPi0Ebin[i]) ;
- }
-
fhMassM02NLocMax1Ebin[i] = new TH2F(Form("hMassM02NLocMax1Ebin%d",i),
- Form("Invariant mass of 2 highest energy cells #lambda_{0}^{2}, E bin %d",i),
+ Form("Invariant mass of split clusters vs #lambda_{0}^{2}, NLM=1, E bin %d",i),
ssbins,ssmin,ssmax,mbins,mmin,mmax);
fhMassM02NLocMax1Ebin[i]->SetYTitle("M (GeV/c^{2})");
fhMassM02NLocMax1Ebin[i]->SetXTitle("#lambda_{0}^{2}");
outputContainer->Add(fhMassM02NLocMax1Ebin[i]) ;
fhMassM02NLocMax2Ebin[i] = new TH2F(Form("hMassM02NLocMax2Ebin%d",i),
- Form("Invariant mass of 2 local maxima cells #lambda_{0}^{2}, E bin %d",i),
+ Form("Invariant mass of split clusters vs #lambda_{0}^{2}, NLM=2, E bin %d",i),
ssbins,ssmin,ssmax,mbins,mmin,mmax);
fhMassM02NLocMax2Ebin[i]->SetYTitle("M (GeV/c^{2})");
fhMassM02NLocMax2Ebin[i]->SetXTitle("#lambda_{0}^{2}");
outputContainer->Add(fhMassM02NLocMax2Ebin[i]) ;
fhMassM02NLocMaxNEbin[i] = new TH2F(Form("hMassM02NLocMaxNEbin%d",i),
- Form("Invariant mass of N>2 local maxima cells vs #lambda_{0}^{2}, E bin %d",i),
+ Form("Invariant mass of split clusters vs vs #lambda_{0}^{2}, NLM>2, E bin %d",i),
ssbins,ssmin,ssmax,mbins,mmin,mmax);
fhMassM02NLocMaxNEbin[i]->SetYTitle("M (GeV/c^{2})");
fhMassM02NLocMaxNEbin[i]->SetXTitle("#lambda_{0}^{2}");
outputContainer->Add(fhMassM02NLocMaxNEbin[i]) ;
+
+ fhMassAsyNLocMax1Ebin[i] = new TH2F(Form("hMassAsyNLocMax1Ebin%d",i),
+ Form("Invariant mass of split clusters vs split asymmetry, NLM=1, E bin %d",i),
+ 200,-1,1,mbins,mmin,mmax);
+ fhMassAsyNLocMax1Ebin[i]->SetYTitle("M (GeV/c^{2})");
+ fhMassAsyNLocMax1Ebin[i]->SetXTitle("asymmetry");
+ outputContainer->Add(fhMassAsyNLocMax1Ebin[i]) ;
+
+ fhMassAsyNLocMax2Ebin[i] = new TH2F(Form("hMassAsyNLocMax2Ebin%d",i),
+ Form("Invariant mass of split clusters vs split asymmetry, NLM=2, E bin %d",i),
+ 200,-1,1,mbins,mmin,mmax);
+ fhMassAsyNLocMax2Ebin[i]->SetYTitle("M (GeV/c^{2})");
+ fhMassAsyNLocMax2Ebin[i]->SetXTitle("asymmetry");
+ outputContainer->Add(fhMassAsyNLocMax2Ebin[i]) ;
+
+ fhMassAsyNLocMaxNEbin[i] = new TH2F(Form("hMassAsyNLocMaxNEbin%d",i),
+ Form("Invariant mass of split clusters vs split asymmetry, NLM>2, E bin %d",i),
+ 200,-1,1,mbins,mmin,mmax);
+ fhMassAsyNLocMaxNEbin[i]->SetYTitle("M (GeV/c^{2})");
+ fhMassAsyNLocMaxNEbin[i]->SetXTitle("asymmetry");
+ outputContainer->Add(fhMassAsyNLocMaxNEbin[i]) ;
+
+
+ if(IsDataMC())
+ {
+ fhMCAsymM02NLocMax1MCPi0Ebin[i] = new TH2F(Form("hMCAsymM02NLocMax1MCPi0Ebin%d",i),
+ Form("Asymmetry of MC #pi^{0} vs #lambda_{0}^{2}, NLM=1, E bin %d",i),
+ ssbins,ssmin,ssmax,100,0,1);
+ fhMCAsymM02NLocMax1MCPi0Ebin[i]->SetYTitle("Decay asymmetry");
+ fhMCAsymM02NLocMax1MCPi0Ebin[i]->SetXTitle("#lambda_{0}^{2}");
+ outputContainer->Add(fhMCAsymM02NLocMax1MCPi0Ebin[i]) ;
+
+ fhMCAsymM02NLocMax2MCPi0Ebin[i] = new TH2F(Form("hMCAsymM02NLocMax2MCPi0Ebin%d",i),
+ Form("Asymmetry of MC #pi^{0} vs #lambda_{0}^{2}, NLM=2, E bin %d",i),
+ ssbins,ssmin,ssmax,100,0,1);
+ fhMCAsymM02NLocMax2MCPi0Ebin[i]->SetYTitle("Decay asymmetry");
+ fhMCAsymM02NLocMax2MCPi0Ebin[i]->SetXTitle("#lambda_{0}^{2}");
+ outputContainer->Add(fhMCAsymM02NLocMax2MCPi0Ebin[i]) ;
+
+ fhMCAsymM02NLocMaxNMCPi0Ebin[i] = new TH2F(Form("hMCAsymM02NLocMaxNMCPi0Ebin%d",i),
+ Form("Asymmetry of MC #pi^{0} vs #lambda_{0}^{2}, NLM>2, E bin %d",i),
+ ssbins,ssmin,ssmax,100,0,1);
+ fhMCAsymM02NLocMaxNMCPi0Ebin[i]->SetYTitle("Decay asymmetry");
+ fhMCAsymM02NLocMaxNMCPi0Ebin[i]->SetXTitle("#lambda_{0}^{2}");
+ outputContainer->Add(fhMCAsymM02NLocMaxNMCPi0Ebin[i]) ;
+
+
+ fhAsyMCGenRecoNLocMax1EbinPi0[i] = new TH2F(Form("hAsyMCGenRecoNLocMax1Ebin%dPi0",i),
+ Form("Generated vs reconstructed asymmetry of split clusters from pi0, NLM=1, E bin %d",i),
+ 200,-1,1,200,-1,1);
+ fhAsyMCGenRecoNLocMax1EbinPi0[i]->SetYTitle("M (GeV/c^{2})");
+ fhAsyMCGenRecoNLocMax1EbinPi0[i]->SetXTitle("asymmetry");
+ outputContainer->Add(fhAsyMCGenRecoNLocMax1EbinPi0[i]) ;
+
+ fhAsyMCGenRecoNLocMax2EbinPi0[i] = new TH2F(Form("hAsyMCGenRecoNLocMax2Ebin%dPi0",i),
+ Form("Generated vs reconstructed asymmetry of split clusters from pi0, NLM=2, E bin %d",i),
+ 200,-1,1,200,-1,1);
+ fhAsyMCGenRecoNLocMax2EbinPi0[i]->SetYTitle("M (GeV/c^{2})");
+ fhAsyMCGenRecoNLocMax2EbinPi0[i]->SetXTitle("asymmetry");
+ outputContainer->Add(fhAsyMCGenRecoNLocMax2EbinPi0[i]) ;
+
+ fhAsyMCGenRecoNLocMaxNEbinPi0[i] = new TH2F(Form("hAsyMCGenRecoNLocMaxNEbin%dPi0",i),
+ Form("Generated vs reconstructed asymmetry of split clusters from pi0, NLM>2, E bin %d",i),
+ 200,-1,1,200,-1,1);
+ fhAsyMCGenRecoNLocMaxNEbinPi0[i]->SetYTitle("M (GeV/c^{2})");
+ fhAsyMCGenRecoNLocMaxNEbinPi0[i]->SetXTitle("asymmetry");
+ outputContainer->Add(fhAsyMCGenRecoNLocMaxNEbinPi0[i]) ;
+ }
+
if(fFillSSExtraHisto)
{
fhMassDispEtaNLocMax1Ebin[i] = new TH2F(Form("hMassDispEtaNLocMax1Ebin%d",i),
fhM02MCGenFracNLocMax1Ebin [mcindex][ebin]->Fill(efrac , l0 );
fhMassMCGenFracNLocMax1Ebin[mcindex][ebin]->Fill(efrac , mass );
}
- fhMCAsymM02NLocMax1MCPi0Ebin [ebin]->Fill(l0 , asymGen );
+ fhMCAsymM02NLocMax1MCPi0Ebin [ebin]->Fill(l0 , asymGen );
+ fhAsyMCGenRecoNLocMax1EbinPi0[ebin]->Fill(asym, asymGen );
}
if(fFillSSExtraHisto)
fhMassSplitEFractionNLocMax1Ebin[0][ebin]->Fill(splitFrac, mass);
if(IsDataMC())fhMassSplitEFractionNLocMax1Ebin[mcindex][ebin]->Fill(splitFrac, mass);
- fhMassM02NLocMax1Ebin [ebin]->Fill(l0 , mass );
+ fhMassM02NLocMax1Ebin [ebin]->Fill(l0 , mass );
+ fhMassAsyNLocMax1Ebin [ebin]->Fill(asym, mass );
+
if(fFillSSExtraHisto)
{
fhMassDispEtaNLocMax1Ebin[ebin]->Fill(dispEta, mass );
fhM02MCGenFracNLocMax2Ebin [mcindex][ebin]->Fill(efrac , l0 );
fhMassMCGenFracNLocMax2Ebin[mcindex][ebin]->Fill(efrac , mass );
}
- fhMCAsymM02NLocMax2MCPi0Ebin [ebin]->Fill(l0 , asymGen );
-
+ fhMCAsymM02NLocMax2MCPi0Ebin [ebin]->Fill(l0 , asymGen );
+ fhAsyMCGenRecoNLocMax2EbinPi0[ebin]->Fill(asym, asymGen );
}
if(fFillSSExtraHisto)
{
fhMassSplitEFractionNLocMax2Ebin[0][ebin]->Fill(splitFrac, mass);
if(IsDataMC())fhMassSplitEFractionNLocMax2Ebin[mcindex][ebin]->Fill(splitFrac, mass);
- fhMassM02NLocMax2Ebin [ebin]->Fill(l0 , mass );
+ fhMassM02NLocMax2Ebin [ebin]->Fill(l0 , mass );
+ fhMassAsyNLocMax2Ebin [ebin]->Fill(asym, mass );
+
if(fFillSSExtraHisto)
{
fhMassDispEtaNLocMax2Ebin[ebin]->Fill(dispEta, mass );
fhM02MCGenFracNLocMaxNEbin [mcindex][ebin]->Fill(efrac , l0 );
fhMassMCGenFracNLocMaxNEbin[mcindex][ebin]->Fill(efrac , mass );
}
- fhMCAsymM02NLocMaxNMCPi0Ebin [ebin]->Fill(l0 , asymGen);
+ fhMCAsymM02NLocMaxNMCPi0Ebin [ebin]->Fill(l0 , asymGen );
+ fhAsyMCGenRecoNLocMaxNEbinPi0[ebin]->Fill(asym, asymGen );
}
if(fFillSSExtraHisto)
{
fhMassSplitEFractionNLocMaxNEbin[0][ebin]->Fill(splitFrac, mass);
if(IsDataMC())fhMassSplitEFractionNLocMaxNEbin[mcindex][ebin]->Fill(splitFrac, mass);
- fhMassM02NLocMaxNEbin [ebin]->Fill(l0 , mass );
+ fhMassM02NLocMaxNEbin [ebin]->Fill(l0 , mass );
+ fhMassAsyNLocMaxNEbin [ebin]->Fill(asym, mass );
+
if(fFillSSExtraHisto)
{
fhMassDispEtaNLocMaxNEbin[ebin]->Fill(dispEta, mass );
if( l0 < fM02MinCut || l0 > fM02MaxCut ) continue ;
- Bool_t m02OK = GetCaloPID()->IsInMergedM02Range(en,l0,nMax);
+ Bool_t m02OK = GetCaloPID()->IsInPi0M02Range(en,l0,nMax);
Bool_t asyOK = GetCaloPID()->IsInPi0SplitAsymmetryRange(en,asym,nMax);
fhNLocMaxM02Cut[0][matched]->Fill(en,nMax);
TH2F * fhMassSplitECutNLocMax2 ; //! 85% of split energy, not matched, Mass of split clusters, NLM = 1
TH2F * fhMassSplitECutNLocMaxN ; //! 85% of split energy, not matched, Mass of split clusters, NLM > 2
- TH2F * fhMassM02NLocMax1[7][2] ; //! Mass of 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 * fhMassM02NLocMax1[7][2] ; //! Mass of splitted clusters when 1 local max vs M02, for E > 7 GeV, 1-6 for different MC particle types
+ TH2F * fhMassM02NLocMax2[7][2] ; //! Mass of splitted clusters when 2 local max vs M02, for E > 7 GeV, 1-6 for different MC particle types
+ TH2F * fhMassM02NLocMaxN[7][2] ; //! Mass of splitted clusters when >2 local max vs M02, for E > 7 GeV, 1-6 for different MC particle types
- TH2F * 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 * 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 * 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 * 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 * 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 * fhMCGenFracAfterCutsNLocMax1MCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 1, MCPi0 after M02 and asymmetry cut
+ TH2F * fhMCGenFracAfterCutsNLocMax2MCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster = 2, MCPi0, after M02 and asymmetry cut
+ TH2F * fhMCGenFracAfterCutsNLocMaxNMCPi0 ; //! E generated particle / E reconstructed vs E reconstructed for N max in cluster > 2, MCPi0, after M02 and asymmetry cut
TH2F * fhMCGenSplitEFracNLocMax1[7][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 1, 1-6 for different MC particle types
TH2F * fhMCGenSplitEFracNLocMax2[7][2] ; //! E generated particle / E1+E2 reconstructed vs E reconstructed for N max in cluster = 2, 1-6 for different MC particle types