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vimartin |
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[UPDATE]
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vimartin |
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The datasets used for this analysis are summarized in
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Tables~\ref{tab:DatasetsData} (data) and~\ref{tab:DatasetsMC} (MC).
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The total integrated luminosity is \lumi after
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applying the official good run list. The main Monte Carlo
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samples are generated with Madgraph, though samples with
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alternative generators such as Powheg and MC@NLO are also used for
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the derivation of systematic uncertainties in the \ttbar~background prediction.
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The triggers used to select both the signal and control samples are
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also summarized in Table.~\ref{tab:TrigData}.
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benhoob |
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vimartin |
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vimartin |
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\begin{table}[!ht]
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\begin{center}
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\begin{tabular}{l}
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\hline
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Dataset Name \\
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\hline
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\hline
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Single Lepton Samples \\
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\hline
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/SingleElectron/Run2012A-13Jul2012-v1/AOD \\
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/SingleMu/Run2012A-13Jul2012-v1/AOD \\
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/SingleElectron/Run2012B-13Jul2012-v1/AOD \\
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/SingleMu/Run2012B-13Jul2012-v1/AOD \\
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/SingleElectron/Run2012C-PromptReco-v*/AOD \\
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/SingleMu/Run2012C-PromptReco-v*/AOD \\
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\hline
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\hline
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fkw |
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Dilepton Samples (only used for dilepton control region)\\
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benhoob |
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\hline
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/DoubleElectron/Run2012A-13Jul2012-v1/AOD \\
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/DoubleMu/Run2012A-13Jul2012-v1/AOD \\
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/MuEG/Run2012A-13Jul2012-v1/AOD \\
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/DoubleElectron/Run2012B-13Jul2012-v1/AOD \\
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/DoubleMu/Run2012B-13Jul2012-v1/AOD \\
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/MuEG/Run2012B-13Jul2012-v1/AOD \\
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/DoubleElectron/Run2012C-PromptReco-v*/AOD \\
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/DoubleMu/Run2012C-PromptReco-v*/AOD \\
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/MuEG/Run2012C-PromptReco-v*/AOD \\
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vimartin |
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\hline
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\end{tabular}
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\caption{Summary of data datasets used.\label{tab:DatasetsData}}
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\end{center}
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\end{table}
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\begin{table}[!ht]
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\begin{center}
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{\footnotesize
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\begin{tabular}{l|l|c}
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\hline
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\multicolumn{3}{c}{With Pileup: Processed dataset name is} \\
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\multicolumn{3}{c}{(S3) Summer12\_DR53X-PU\_S10\_START53\_V7A-v*/AODSIM} \\
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vimartin |
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\multicolumn{3}{c}{(S3) Summer11-PU\_S3\_START42\_V11-v*/AODSIM} \\
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\hline
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vimartin |
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%ZZ & \verb=/ZZJetsTo4L_TuneZ2star_8TeV-madgraph-tauola/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 0.1769 \\
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%& \verb=/ZZJetsTo2L2Q_TuneZ2star_8TeV-madgraph-tauola/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 2.4487 \\
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%& \verb=/ZZJetsTo2L2Nu_TuneZ2star_8TeV-madgraph-tauola/Summer12_DR53X-PU_S10_START53_V7A-v3/AODSIM= & 0.3648 \\
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%\hline
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%WZ & \verb=/WZJetsTo3LNu_TuneZ2_8TeV-madgraph-tauola/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 1.0575 \\
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%& \verb=/WZJetsTo2L2Q_TuneZ2star_8TeV-madgraph-tauola/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 2.206 \\
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%\hline
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%WW & \verb=/WWJetsTo2L2Nu_TuneZ2star_8TeV-madgraph-tauola/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 5.8123 \\
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%\hline
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%single top & \verb=/T_tW-channel-DR_TuneZ2star_8TeV-powheg-tauola/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 11.177 \\
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% & \verb=/Tbar_tW-channel-DR_TuneZ2star_8TeV-powheg-tauola/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 11.177 \\
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%\hline
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%ttV & \verb=/TTZJets_8TeV-madgraph_v2/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 0.208 \\
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%& \verb=/TTWJets_8TeV-madgraph/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 0.232 \\
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%\hline
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%VVV & \verb=/ZZZNoGstarJets_8TeV-madgraph/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 0.01922 \\
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%& \verb=/WWWJets_8TeV-madgraph/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 0.08217 \\
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%& \verb=/WWZNoGstarJets_8TeV-madgraph/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 0.0633 \\
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%%& \verb=/ZZZNoGstarJets_8TeV-madgraph/Summer12_DR53X-PU_S10_START53_V7A-v1/AODSIM= & 0.01922 \\
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Description & Primary Dataset Name & cross-section [pb]\\
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\hline
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$\ttbar$ & /TTJets\_MassiveBinDECAY\_TuneZ2Star\_8TeV-madgraph-tauola (S3) & 225.2 \\
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W $\rightarrow$ $\ell\nu$ & /WJetsToLNu\_TuneZ2Star\_8TeV-madgraph-tauola (S3) & 31314.0 \\
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WW & /WW\_TuneZ2Star\_8TeV\_pythia6\_tauola (S3) & 45.6\\
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WZ & /WZ\_TuneZ2Star\_8TeV\_pythia6\_tauola (S3) & 18.2 \\
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ZZ & /ZZ\_TuneZ2Star\_8TeV\_pythia6\_tauola (S3) & 7.4 \\
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$t$ ($s$-chan) & /T\_TuneZ2Star\_s-channel\_8TeV-powheg-tauola (S3) & 3.19 \\
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$\bar{t}$ ($s$-chan) & /Tbar\_TuneZ2Star\_s-channel\_8TeV-powheg-tauola (S3) & 1.44 \\
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$t$ ($t$-chan) & /T\_TuneZ2Star\_t-channel\_8TeV-powheg-tauola (S3) & 41.92 \\
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$\bar{t}$ ($t$-chan) & /Tbar\_TuneZ2Star\_t-channel\_8TeV-powheg-tauola (S3) & 22.65 \\
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$tW$ & /T\_TuneZ2Star\_tW-channel-DR\_8TeV-powheg-tauola (S3) & 7.87 \\
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$\bar{t} W$ & /Tbar\_TuneZ2Star\_tW-channel-DR\_8TeV-powheg-tauola (S3) & 7.87 \\
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$\dy \To \ell \ell$ & /DYJetsToLL\_TuneZ2Star\_M-50\_8TeV-madgraph-tarball (S3) & 3532.8 \\
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$\ttbar W$ & /TTW\_TuneZ2Star\_8TeV-madgraph (S3) & 0.1633 \\
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$\ttbar Z$ & /TTZ\_TuneZ2Star\_8TeV-madgraph (S3) & 0.139 \\
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$\ttbar \gamma$ & /TTPhoton\_TuneZ2Star\_8TeV-madgraph (S3) & 0.6545 \\
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WW$\gamma$ & /WWPhoton\_TuneZ2Star\_8TeV-madgraph (S3) & 0.177 \\
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WWZ & /WWZNoGstar\_TuneZ2Star\_8TeV-madgraph (S3) & 0.0268\\
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WWW & /WWW\_TuneZ2Star\_8TeV-madgraph (S3) & 0.038 \\
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WZZ & /WZZNoGstar\_TuneZ2Star\_8TeV-madgraph (S3) & 0.0088 \\
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ZZZ & /ZZZNoGstar\_TuneZ2Star\_8TeV-madgraph (S3) & 0.00288 \\
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$\tilde{t}\bar{\tilde{t}}\rightarrow t\bar{t}\chi^0_1\chi^0_1$ & /SMS-T2tt\_Mstop-225to1200\_mLSP-50to1025\_8TeV-Pythia6Z (S2) & scan\\
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$\tilde{t}\bar{\tilde{t}}\rightarrow b\bar{b}\chi^+_1\chi^-_1$ & /SMS-T2bw\_x-0p25to0p75\_mStop-50to850\_mLSP-50to800\_8TeV-Pythia6Z (S2) & scan \\
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\hline
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\hline
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$\ttbar$ ($Q^2 \times 2$) & /TTjets\_TuneZ2Star\_scaleup\_8TeV-madgraph-tauola (S3) & 225.2 \\
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$\ttbar$ ($Q^2 \times 0.5$) & /TTjets\_TuneZ2Star\_scaledown\_8TeV-madgraph-tauola (S3) & 225.2 \\
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$\ttbar$ ($x_q>40~\GeV$) & /TTjets\_TuneZ2Star\_matchingup\_8TeV-madgraph-tauola (S3) & 225.2 \\
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$\ttbar$ ($x_q>10~\GeV$) & /TTjets\_TuneZ2Star\_matchingdown\_8TeV-madgraph-tauola (S3) & 225.2 \\
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$\ttbar$ ($m_{\mathrm{top}} = 178.5~\GeV$) & /TTJets\_TuneZ2Star\_mass178\_5\_8TeV-madgraph-tauola (S3) & 225.2 \\
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$\ttbar$ ($m_{\mathrm{top}} = 166.5~\GeV$) & /TTJets\_TuneZ2Star\_mass166\_5\_8TeV-madgraph-tauola (S3) & 225.2 \\
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$\ttbar$ & /TT\_TuneZ2Star\_8TeV-powheg-tauola (S3) & 225.2 \\
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%$\ttbar \To \ell \ell \nu \nu$ & /TTTo2L2Nu2B\_8TeV-powheg-pythia6 (S3) & 16.5 \\
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%$\ttbar$ & /TT\_TuneZ2Star\_8TeV-mcatnlo (S3) & 157.5 \\
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%$\ttbar$ & /TT\_TuneZ2Star\_8TeV-pythia6-tauola (S3) & 157.5 \\
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vimartin |
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\hline
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\end{tabular}
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benhoob |
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}
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vimartin |
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\caption{Summary of Monte Carlo datasets used. TO BE UPDATED.
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\label{tab:DatasetsMC}}
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vimartin |
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\end{center}
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\end{table}
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\begin{table}[!ht]
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\begin{center}
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benhoob |
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\begin{tabular}{l}
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vimartin |
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\hline
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\hline
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Triggers \\
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\hline
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\hline
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Single Muon Sample\\
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\hline
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\footnotesize{\verb=HLT_IsoMu17_v*=}\\
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\footnotesize{\verb=HLT_IsoMu24_v*=}\\
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\footnotesize{\verb=HLT_IsoMu30_eta2p1_v*=}\\
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\hline
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Single Electron Sample\\
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\hline
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\footnotesize{\verb=HLT_Ele25_CaloIdVT_TrkIdT_CentralTriJet30_v*=}\\
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\footnotesize{\verb=HLT_Ele25_CaloIdVT_TrkIdT_TriCentralJet30_v*=}\\
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\footnotesize{\verb=HLT_Ele25_CaloIdVT_CaloIsoT_TrkIdT_TrkIsoT_TriCentralJet30_v*=}\\
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\footnotesize{\verb=HLT_Ele25_CaloIdVT_CaloIsoT_TrkIdT_TrkIsoT_TriCentralPFJet30_v*=}\\
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\hline
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vimartin |
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Dimuon Sample (only used for dilepton control regions)\\
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vimartin |
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\hline
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\footnotesize{\verb=HLT_DoubleMu7_v*=}\\
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\footnotesize{\verb=HLT_Mu13_Mu7_v*=}\\
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\footnotesize{\verb=HLT_Mu13_Mu8_v*=}\\
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\footnotesize{\verb=HLT_Mu17_Mu8_v*=}\\
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\hline
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vimartin |
1.7 |
Electron-Muon Sample (only used for dilepton control regions)\\
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vimartin |
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\hline
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\footnotesize{\verb=HLT_Mu17_Ele8_CaloIdL_v*=}\\
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\footnotesize{\verb=HLT_Mu8_Ele17_CaloIdL_v*=}\\
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\footnotesize{\verb=HLT_Mu17_Ele8_CaloIdT_CaloIsoVL_v*=}\\
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\footnotesize{\verb=HLT_Mu8_Ele17_CaloIdT_CaloIsoVL_v*=}\\
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\hline
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vimartin |
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Dielectron Sample (only used for dilepton control regions)\\
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vimartin |
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\hline
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\footnotesize{\verb=HLT_Ele17_CaloIdL_CaloIsoVL_Ele8_CaloIdL_CaloIsoVL_v*=}\\
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\footnotesize{\verb=HLT_Ele17_CaloIdT_TrkIdVL_CaloIsoVL_TrkIsoVL_Ele8_CaloIdT_TrkIdVL_CaloIsoVL_TrkIsoVL_v*=}\\
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\footnotesize{\verb=HLT_Ele17_CaloIdT_CaloIsoVL_TrkIdVL_TrkIsoVL_Ele8_CaloIdT_CaloIsoVL_TrkIdVL_TrkIsoVL_v*=}\\
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\hline
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\end{tabular}
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vimartin |
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\caption{Summary of triggers used. TO BE UPDATED
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\label{tab:TrigData}}
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vimartin |
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\end{center}
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\end{table}
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