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claudioc |
1.1 |
\section{Event Preselection}
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\label{sec:eventSel}
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claudioc |
1.6 |
%{\color{red} This needs to be fixed up -- probably many mistakes present.}\\
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claudioc |
1.1 |
As mentioned in the introduction, the preselection is based on the
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$t\bar{t}$ analysis. We select events with two opposite sign isolated
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leptons ($ee$, $e\mu$, or $\mu\mu$); one of the leptons must
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have $P_T > 20$ GeV,
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benhoob |
1.10 |
the other one must have $P_T > 10$ GeV. In case of events with
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claudioc |
1.5 |
more than two such leptons, we select the pair that maximizes the scalar
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benhoob |
1.10 |
sum of lepton $P_T$'s.
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There must be two JPT
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claudioc |
1.5 |
jets of $P_T > 30$ GeV and $|\eta| < 2.5$; the scalar sum of the
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$P_T$ of all such jets must exceed 100 GeV; jets must pass
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{\tt caloJetId} and be separated by $\Delta R >$ 0.4 from the
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benhoob |
1.10 |
two selected leptons.
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%%%TO BE REPLACED
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%{\color{red}The 11 pb iteration only does this for the two selected
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%leptons.}
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%
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Finally $\met > 50$ GeV (we use tcMet). More details are given in the subsections below.
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claudioc |
1.1 |
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\subsection{Event Cleanup}
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\label{sec:cleanup}
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\begin{itemize}
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\item Scraping cut: if there are $\geq$ 10 tracks, require at
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least 25\% of them to be high purity.
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\item Require at least one good vertex:
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\begin{itemize}
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\item not fake
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\item ndof $>$ 4
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\item $|\rho| < 2$ cm
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claudioc |
1.3 |
\item $|z| < 24$ cm.
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claudioc |
1.1 |
\end{itemize}
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\end{itemize}
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\subsection{Muon Selection}
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\label{sec:muon}
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Muon candidates are RECO muon objects passing the following
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requirements:
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\begin{itemize}
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claudioc |
1.5 |
\item $|\eta| < 2.4$.
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claudioc |
1.1 |
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\item Global Muon and Tracker Muon.
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\item $\chi^2$/ndof of global fit $<$ 10.
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\item At least 11 hits in the tracker fit.
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\item Transverse impact parameter with respect to the beamspot $<$ 200 $\mu$m.
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\item $Iso \equiv $ $E_T^{\rm iso}$/Max(20 GeV, $P_T$) $<$ 0.15.
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$E_T^{\rm iso}$
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is defined as the sum of transverse energy/momentum deposits in ecal,
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hcal, and tracker, in a cone of 0.3.
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\item At least one of the hits from the
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standalone muon must be used in the global fit.
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claudioc |
1.9 |
%\item Require tracker $\Delta P_T/P_T < 0.1$. This cut was not in the original top analysis.
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%It is motivated by the observation of
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%poorly measured muons in data with large
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%relative $P_T$ uncertainty, giving significant contributions to the \met.
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%{\color{red} This is not applied to the 11 pb iteration.}
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claudioc |
1.7 |
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claudioc |
1.6 |
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claudioc |
1.1 |
\end{itemize}
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claudioc |
1.2 |
\subsection{Electron Selection}
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claudioc |
1.1 |
\label{sec:electron}
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Electron candidates are RECO GSF electrons passing the following
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requirements:
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\begin{itemize}
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\item $P_T > 10$ GeV. (The $t\bar{t}$ analysis uses 20 GeV but for
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completeness we calculate FR down to 10 GeV).
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\item $|\eta| < 2.5$.
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\item SuperCluster $E_T > 10$ GeV.
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\item The electron must be ecal seeded.
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\item VBTF90 identification\cite{ref:vbtf}.
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\item Transverse impact parameter with respect to the beamspot $<$ 400 $\mu$m.
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\item $Iso \equiv $ $E_T^{\rm iso}$/Max(20 GeV, $P_T$) $<$ 0.15.
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$E_T^{\rm iso}$
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is defined as the sum of transverse energy/momentum deposits in ecal,
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hcal, and tracker, in a
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cone of 0.3. A 1 GeV pedestal is subtracted from the ecal energy
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deposition in the EB, however the ecal energy is never allowed to
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go negative.
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\item Electrons with a tracker or global muon within $\Delta R$ of
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0.1 are vetoed.
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\item The number of missing expected inner hits must be less than
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two\cite{ref:conv}.
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\item Conversion removal via partner track finding: any electron
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where an additional GeneralTrack is found with $Dist < 0.02$ cm
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and $\Delta \cot \theta < 0.02$ is vetoed\cite{ref:conv}.
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claudioc |
1.4 |
\item Cleaning for ECAL spike (aka Swiss-Cross cleaning) has been applied
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at the reconstruction level (CMSSW 38x).
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claudioc |
1.1 |
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\end{itemize}
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claudioc |
1.5 |
\subsection{Invariant mass requirement}
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claudioc |
1.2 |
\label{sec:zveto}
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We remove $e^+e^-$ and $\mu^+ \mu^-$ events with invariant
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claudioc |
1.5 |
mass between 76 and 106 GeV. We also remove events
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with invariant mass $<$ 10 GeV.
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claudioc |
1.2 |
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\subsection{Trigger Selection}
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claudioc |
1.1 |
\label{sec:trigSel}
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Because most of the triggers implemented in the 2nd half of the
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2010 run were not implemented in the Monte Carlo, no trigger
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selection is applied on Monte Carlo data. As discussed in
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Section~\ref{sec:trgEff}, a trigger efficiency weight is applied
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to each event, based on the trigger efficiencies measured on data.
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Trigger efficiency weights are very close to 1.
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claudioc |
1.5 |
%For data, we require the logical OR of all (or most?) unprescaled
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%single and double lepton triggers that were deployed during the 2010
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%run. These are:
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%{\color{red} Here we need to list the triggers, somehow.}
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For data, we use a cocktail of unprescaled single
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and double lepton triggers. An event
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in the $ee$ final state is required to pass at least 1
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single- or double-electron trigger, a
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$\mu\mu$ event is required to pass at least 1 single
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or double-muon trigger, while an $e\mu$ event
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is required to pass at least 1 single-muon, single-electron,
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or $e-\mu$ cross trigger.
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% We currently
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% do not require MC events to pass any triggers.
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claudioc |
1.1 |
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claudioc |
1.5 |
\begin{itemize}
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\item single-muon triggers
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\begin{itemize}
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\item \verb=HLT_Mu5=
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\item \verb=HLT_Mu7=
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\item \verb=HLT_Mu9=
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\item \verb=HLT_Mu11=
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\item \verb=HLT_Mu13_v1=
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\item \verb=HLT_Mu15_v1=
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\item \verb=HLT_Mu17_v1=
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\item \verb=HLT_Mu19_v1=
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\end{itemize}
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\item double-muon triggers
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\begin{itemize}
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\item \verb=HLT_DoubleMu3=
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\item \verb=HLT_DoubleMu3_v2=
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\item \verb=HLT_DoubleMu5_v1=
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\end{itemize}
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\item single-electron triggers
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\begin{itemize}
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\item \verb=HLT_Ele10_SW_EleId_L1R=
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\item \verb=HLT_Ele10_LW_EleId_L1R=
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\item \verb=HLT_Ele10_LW_L1R=
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\item \verb=HLT_Ele10_SW_L1R=
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\item \verb=HLT_Ele15_SW_CaloEleId_L1R=
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\item \verb=HLT_Ele15_SW_EleId_L1R=
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\item \verb=HLT_Ele15_SW_L1R=
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\item \verb=HLT_Ele15_LW_L1R=
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\item \verb=HLT_Ele17_SW_TightEleId_L1R=
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\item \verb=HLT_Ele17_SW_TighterEleId_L1R_v1=
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\item \verb=HLT_Ele17_SW_CaloEleId_L1R=
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\item \verb=HLT_Ele17_SW_EleId_L1R=
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\item \verb=HLT_Ele17_SW_LooseEleId_L1R=
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\item \verb=HLT_Ele17_SW_TighterEleIdIsol_L1R_v2=
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\item \verb=HLT_Ele20_SW_L1R=
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\item \verb=HLT_Ele22_SW_TighterEleId_L1R_v2=
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\item \verb=HLT_Ele32_SW_TightCaloEleIdTrack_L1R_v1=
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\item \verb=HLT_Ele32_SW_TighterEleId_L1R_v2=
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\item \verb=HLT_Ele27_SW_TightCaloEleIdTrack_L1R_v1=
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\item \verb=HLT_Ele22_SW_TighterCaloIdIsol_L1R_v2=
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\item \verb=HLT_Ele22_SW_TighterEleId_L1R_v3=
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\item \verb=HLT_Ele22_SW_TighterCaloIdIsol_L1R_v2=
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\end{itemize}
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\item double-electron triggers
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\begin{itemize}
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\item \verb=HLT_DoubleEle15_SW_L1R_v1=
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\item \verb=HLT_DoubleEle17_SW_L1R_v1=
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\item \verb=HLT_Ele17_SW_TightCaloEleId_Ele8HE_L1R_v1=
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\item \verb=HLT_Ele17_SW_TightCaloEleId_SC8HE_L1R_v1=
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\item \verb=HLT_DoubleEle10_SW_L1R=
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\item \verb=HLT_DoubleEle5_SW_L1R=
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\end{itemize}
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\item e-$\mu$ cross triggers
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\begin{itemize}
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\item \verb=HLT_Mu5_Ele5_v1=
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\item \verb=HLT_Mu5_Ele9_v1=
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\item \verb=HLT_Mu11_Ele8_v1=
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\item \verb=HLT_Mu8_Ele8_v1=
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\item \verb=HLT_Mu5_Ele13_v2=
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\item \verb=HLT_Mu5_Ele17_v1=
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\end{itemize}
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\end{itemize}
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