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root/cvsroot/UserCode/benhoob/cmsnotes/StopSearch/CR2.tex
Revision: 1.4
Committed: Wed Oct 10 04:03:33 2012 UTC (12 years, 7 months ago) by vimartin
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Branch: MAIN
Changes since 1.3: +15 -30 lines
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added new signal regions

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# Content
1
2 \subsection{Single Lepton Top MC Modelling Validation from CR2}
3 \label{sec:cr2}
4
5 IS THIS GOING TO BE DONE WITH A BVETO OR NOT. IF SO, IS IT GOING TO
6 BE CSVL OR CSVM? NEED TO DISCUSS THIS.
7
8 The \mt\ tail for single-lepton top events (\ttsl\ and single top) is dominated by jet resolution effects. The \W\ cannot be far off-shell because $\mW < \mtop$.
9 The modeling of the \mt\ tail from jet resolution effects is studied using \zjets\ data and MC samples.
10 \Z\ events are selection by requiring 2 good leptons (satisfying ID and isolation requirements) and requiring the \mll\ to be in the range $81-101$ GeV.
11 The negative lepton is treated as a neutrino and so is added to the MET: \met\ $\rightarrow$ \pt(\Lepm) + \met,
12 and the \mt\ is recalculated with the positive lepton \mt(\Lepp, \met).
13 The resulting ``pseudo-\mt'' is dominated by jet resolution effects, since no off-shell
14 \Z\ production enters the sample due to the \mll\ requirement.
15 This section describes how well the MC predicts the tail of ``pseudo-\mt''.
16
17 The underlying distributions are shown in Fig.~\ref{fig:cr2met}
18 and~\ref{fig:cr2mtrest}. The comparison of data and MC event counts
19 is shown in Table~\ref{tab:cr2yields}. From this table we extract
20 the data to MC scale factors $SFR^{e}_{top}$ and $SFR^{\mu}_{top}$.
21
22
23 \begin{table}[!h]
24 \begin{center}
25 {\footnotesize
26 \begin{tabular}{l||c|c||c|c|c|c|c}
27 \hline
28 Sample & CR2PRESEL0 &CR2PRESEL1 & CR2A & CR2B & CR2C &
29 CR2D & CR2E \\
30 \hline
31 \hline
32 MC & $36 \pm 2$ & $30 \pm 2$ & $18 \pm 1$ & $30 \pm 2$ & $13 \pm 1$ & $5 \pm 0$ & $2 \pm 0$ \\
33 Data & $56$ & $43$ & $32$ & $40$ & $21$ & $12$ & $2$ \\
34 \hline
35 Data/MC & $1.56 \pm 0.23$ & $1.44 \pm 0.24$ & $1.77 \pm 0.34$ & $1.32 \pm 0.22$ & $1.65 \pm 0.37$ & $2.65 \pm 0.79$ & $0.99 \pm 0.71$ \\
36 \hline
37 \hline
38 \hline
39 DY MC & $27 \pm 2$ & $23 \pm 2$ & $14 \pm 2$ & $25 \pm 3$ & $11 \pm 2$ & $3 \pm 1$ & $1 \pm 1$ \\
40 DY Data & $47 \pm 8$ & $36 \pm 7$ & $28 \pm 6$ & $35 \pm 6$ & $19 \pm 5$ & $11 \pm 3$ & $1 \pm 1$ \\
41 \hline
42 DY Data/MC & $1.75 \pm 0.31$ & $1.58 \pm 0.32$ & $2.00 \pm 0.47$ & $1.38 \pm 0.31$ & $1.78 \pm 0.56$ & $3.29 \pm 1.73$ & $0.98 \pm 1.20$ \\
43 \hline
44 \hline
45 \hline
46 $SFR_{top}$ & $1.66 \pm 0.23$ & $1.51 \pm 0.24$ & $1.89 \pm
47 0.34$ & $1.35 \pm 0.22$ & $1.71 \pm 0.37$ & $2.97 \pm 0.79$ & $0.98
48 \pm 0.71$ \\
49 \hline
50 \end{tabular}}
51 \caption{ Yields in \mt\ tail comparing the \zjets\ MC prediction (after
52 applying SFs) to data after subtracting the non-\zjets\ components.
53 CR2PRESEL refers to a sample with $\met>50$ GeV and $\mt>150$ GeV.
54 The uncertainties are statistical only. NEED TO ADD THE SYMBOLS
55 DEFINED IN THE TEXT FOR THESE SCALE FACTORS. IS THIS GOING TO BE
56 DONE SEPARATELY FOR MUONS AND ELECTRONS???
57 MAYBE WANT TO REMOVE LAST ENTRIES WHERE STATS ARE VERY LOW
58 \label{tab:cr2yields}}
59 \end{center}
60 \end{table}
61
62
63 \begin{figure}[hbt]
64 \begin{center}
65 % \includegraphics[width=0.5\linewidth]{plots/CR2plots/met_scaled_nj4_emucomb.pdf}%
66 \includegraphics[width=0.5\linewidth]{plots/CR2plots/met_lepcor_scaled_nj4_emucomb.pdf}%
67 \includegraphics[width=0.5\linewidth]{plots/CR2plots/mt_lepcor_scaled_nj4_emucomb.pdf}
68 \includegraphics[width=0.5\linewidth]{plots/CR2plots/mt_lepcor_scaled_met50_nj4_emucomb.pdf}%
69 \includegraphics[width=0.5\linewidth]{plots/CR2plots/mt_lepcor_scaled_met100_nj4_emucomb.pdf}
70
71 \caption{
72 Comparison of the pseudo\-\met\ (top, left), pseudo\-\mt\ (top,
73 right and bottom) distributions in data vs. MC for events
74 satisfying the requirements of CR2, combining both the muon and
75 electron channels. The pseudo\-\mt\ distributions are shown
76 before any additional requirements (top, right) and after
77 requiring pseudo\-\met>50 GeV (bottom, left) and pseudo\-\met>100 GeV (bottom, right) .
78 \label{fig:cr2met}
79 }
80 \end{center}
81 \end{figure}
82
83 \begin{figure}[hbt]
84 \begin{center}
85 \includegraphics[width=0.5\linewidth]{plots/CR2plots/mt_lepcor_scaled_met150_nj4_emucomb.pdf}%
86 \includegraphics[width=0.5\linewidth]{plots/CR2plots/mt_lepcor_scaled_met200_nj4_emucomb.pdf}
87 \includegraphics[width=0.5\linewidth]{plots/CR2plots/mt_lepcor_scaled_met250_nj4_emucomb.pdf}%
88 \includegraphics[width=0.5\linewidth]{plots/CR2plots/mt_lepcor_scaled_met300_nj4_emucomb.pdf}
89 \caption{
90 Comparison of the \mt\ distribution in data vs. MC for events
91 satisfying the requirements of CR2, combining both the muon and
92 electron channels. The pseudo-\met\ requirements used are
93 150 GeV (top, left), 200 GeV (top, right), 250 GeV (bottom,
94 left) and 300 GeV (bottom, right).
95 \label{fig:cr2mtrest}
96 }
97 \end{center}
98 \end{figure}
99 \clearpage