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# User Rev Content
1 claudioc 1.1 \section{Event Preselection}
2     \label{sec:eventSel}
3     {\color{red} This needs to be fixed up -- probably many mistakes present.}\\
4     As mentioned in the introduction, the preselection is based on the
5     $t\bar{t}$ analysis. We select events with two opposite sign isolated
6     leptons ($ee$, $e\mu$, or $\mu\mu$); one of the leptons must
7     have $P_T > 20$ GeV,
8 claudioc 1.5 the other one must have $P_T > 10$ GeV\footnote{In case of events with
9     more than two such leptons, we select the pair that maximizes the scalar
10     sum of lepton $P_T$'s.};
11     there must be two JPT
12     jets of $P_T > 30$ GeV and $|\eta| < 2.5$; the scalar sum of the
13     $P_T$ of all such jets must exceed 100 GeV; jets must pass
14     {\tt caloJetId} and be separated by $\Delta R >$ 0.4 from the
15     two leptons. Finally $\met > 50$ GeV
16 claudioc 1.1 (we use tcMet). More details are given in the subsection below.
17    
18     \subsection{Event Cleanup}
19     \label{sec:cleanup}
20     \begin{itemize}
21     \item Scraping cut: if there are $\geq$ 10 tracks, require at
22     least 25\% of them to be high purity.
23     \item Require at least one good vertex:
24     \begin{itemize}
25     \item not fake
26     \item ndof $>$ 4
27     \item $|\rho| < 2$ cm
28 claudioc 1.3 \item $|z| < 24$ cm.
29 claudioc 1.1 \end{itemize}
30     \end{itemize}
31    
32    
33     \subsection{Muon Selection}
34     \label{sec:muon}
35    
36     Muon candidates are RECO muon objects passing the following
37     requirements:
38     \begin{itemize}
39    
40 claudioc 1.5 \item $|\eta| < 2.4$.
41 claudioc 1.1
42     \item Global Muon and Tracker Muon.
43    
44     \item $\chi^2$/ndof of global fit $<$ 10.
45    
46     \item At least 11 hits in the tracker fit.
47    
48     \item Transverse impact parameter with respect to the beamspot $<$ 200 $\mu$m.
49    
50     \item $Iso \equiv $ $E_T^{\rm iso}$/Max(20 GeV, $P_T$) $<$ 0.15.
51     $E_T^{\rm iso}$
52     is defined as the sum of transverse energy/momentum deposits in ecal,
53     hcal, and tracker, in a cone of 0.3.
54    
55     \item At least one of the hits from the
56     standalone muon must be used in the global fit.
57    
58     \end{itemize}
59    
60    
61    
62 claudioc 1.2 \subsection{Electron Selection}
63 claudioc 1.1 \label{sec:electron}
64    
65     Electron candidates are RECO GSF electrons passing the following
66     requirements:
67    
68     \begin{itemize}
69    
70     \item $P_T > 10$ GeV. (The $t\bar{t}$ analysis uses 20 GeV but for
71     completeness we calculate FR down to 10 GeV).
72    
73     \item $|\eta| < 2.5$.
74    
75     \item SuperCluster $E_T > 10$ GeV.
76    
77     \item The electron must be ecal seeded.
78    
79     \item VBTF90 identification\cite{ref:vbtf}.
80    
81     \item Transverse impact parameter with respect to the beamspot $<$ 400 $\mu$m.
82    
83     \item $Iso \equiv $ $E_T^{\rm iso}$/Max(20 GeV, $P_T$) $<$ 0.15.
84     $E_T^{\rm iso}$
85     is defined as the sum of transverse energy/momentum deposits in ecal,
86     hcal, and tracker, in a
87     cone of 0.3. A 1 GeV pedestal is subtracted from the ecal energy
88     deposition in the EB, however the ecal energy is never allowed to
89     go negative.
90    
91     \item Electrons with a tracker or global muon within $\Delta R$ of
92     0.1 are vetoed.
93    
94     \item The number of missing expected inner hits must be less than
95     two\cite{ref:conv}.
96    
97     \item Conversion removal via partner track finding: any electron
98     where an additional GeneralTrack is found with $Dist < 0.02$ cm
99     and $\Delta \cot \theta < 0.02$ is vetoed\cite{ref:conv}.
100    
101 claudioc 1.4 \item Cleaning for ECAL spike (aka Swiss-Cross cleaning) has been applied
102     at the reconstruction level (CMSSW 38x).
103 claudioc 1.1
104     \end{itemize}
105    
106 claudioc 1.5 \subsection{Invariant mass requirement}
107 claudioc 1.2 \label{sec:zveto}
108    
109     We remove $e^+e^-$ and $\mu^+ \mu^-$ events with invariant
110 claudioc 1.5 mass between 76 and 106 GeV. We also remove events
111     with invariant mass $<$ 10 GeV.
112 claudioc 1.2
113     \subsection{Trigger Selection}
114 claudioc 1.1 \label{sec:trigSel}
115    
116     Because most of the triggers implemented in the 2nd half of the
117     2010 run were not implemented in the Monte Carlo, no trigger
118     selection is applied on Monte Carlo data. As discussed in
119     Section~\ref{sec:trgEff}, a trigger efficiency weight is applied
120     to each event, based on the trigger efficiencies measured on data.
121     Trigger efficiency weights are very close to 1.
122    
123 claudioc 1.5 %For data, we require the logical OR of all (or most?) unprescaled
124     %single and double lepton triggers that were deployed during the 2010
125     %run. These are:
126     %{\color{red} Here we need to list the triggers, somehow.}
127    
128     For data, we use a cocktail of unprescaled single
129     and double lepton triggers. An event
130     in the $ee$ final state is required to pass at least 1
131     single- or double-electron trigger, a
132     $\mu\mu$ event is required to pass at least 1 single
133     or double-muon trigger, while an $e\mu$ event
134     is required to pass at least 1 single-muon, single-electron,
135     or $e-\mu$ cross trigger.
136     % We currently
137     % do not require MC events to pass any triggers.
138 claudioc 1.1
139 claudioc 1.5 \begin{itemize}
140     \item single-muon triggers
141     \begin{itemize}
142     \item \verb=HLT_Mu5=
143     \item \verb=HLT_Mu7=
144     \item \verb=HLT_Mu9=
145     \item \verb=HLT_Mu11=
146     \item \verb=HLT_Mu13_v1=
147     \item \verb=HLT_Mu15_v1=
148     \item \verb=HLT_Mu17_v1=
149     \item \verb=HLT_Mu19_v1=
150     \end{itemize}
151     \item double-muon triggers
152     \begin{itemize}
153     \item \verb=HLT_DoubleMu3=
154     \item \verb=HLT_DoubleMu3_v2=
155     \item \verb=HLT_DoubleMu5_v1=
156     \end{itemize}
157     \item single-electron triggers
158     \begin{itemize}
159     \item \verb=HLT_Ele10_SW_EleId_L1R=
160     \item \verb=HLT_Ele10_LW_EleId_L1R=
161     \item \verb=HLT_Ele10_LW_L1R=
162     \item \verb=HLT_Ele10_SW_L1R=
163     \item \verb=HLT_Ele15_SW_CaloEleId_L1R=
164     \item \verb=HLT_Ele15_SW_EleId_L1R=
165     \item \verb=HLT_Ele15_SW_L1R=
166     \item \verb=HLT_Ele15_LW_L1R=
167     \item \verb=HLT_Ele17_SW_TightEleId_L1R=
168     \item \verb=HLT_Ele17_SW_TighterEleId_L1R_v1=
169     \item \verb=HLT_Ele17_SW_CaloEleId_L1R=
170     \item \verb=HLT_Ele17_SW_EleId_L1R=
171     \item \verb=HLT_Ele17_SW_LooseEleId_L1R=
172     \item \verb=HLT_Ele17_SW_TighterEleIdIsol_L1R_v2=
173     \item \verb=HLT_Ele20_SW_L1R=
174     \item \verb=HLT_Ele22_SW_TighterEleId_L1R_v2=
175     \item \verb=HLT_Ele32_SW_TightCaloEleIdTrack_L1R_v1=
176     \item \verb=HLT_Ele32_SW_TighterEleId_L1R_v2=
177     \item \verb=HLT_Ele27_SW_TightCaloEleIdTrack_L1R_v1=
178     \item \verb=HLT_Ele22_SW_TighterCaloIdIsol_L1R_v2=
179     \item \verb=HLT_Ele22_SW_TighterEleId_L1R_v3=
180     \item \verb=HLT_Ele22_SW_TighterCaloIdIsol_L1R_v2=
181     \end{itemize}
182     \item double-electron triggers
183     \begin{itemize}
184     \item \verb=HLT_DoubleEle15_SW_L1R_v1=
185     \item \verb=HLT_DoubleEle17_SW_L1R_v1=
186     \item \verb=HLT_Ele17_SW_TightCaloEleId_Ele8HE_L1R_v1=
187     \item \verb=HLT_Ele17_SW_TightCaloEleId_SC8HE_L1R_v1=
188     \item \verb=HLT_DoubleEle10_SW_L1R=
189     \item \verb=HLT_DoubleEle5_SW_L1R=
190     \end{itemize}
191     \item e-$\mu$ cross triggers
192     \begin{itemize}
193     \item \verb=HLT_Mu5_Ele5_v1=
194     \item \verb=HLT_Mu5_Ele9_v1=
195     \item \verb=HLT_Mu11_Ele8_v1=
196     \item \verb=HLT_Mu8_Ele8_v1=
197     \item \verb=HLT_Mu5_Ele13_v2=
198     \item \verb=HLT_Mu5_Ele17_v1=
199     \end{itemize}
200     \end{itemize}