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root/cvsroot/UserCode/claudioc/OSNote2010/sigregion.tex
Revision: 1.8
Committed: Wed Dec 8 12:04:25 2010 UTC (14 years, 4 months ago) by benhoob
Content type: application/x-tex
Branch: MAIN
CVS Tags: FR1, v4, v3, HEAD
Changes since 1.7: +9 -5 lines
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Update with official json v3

File Contents

# Content
1 \section{Definition of the signal region}
2 \label{sec:sigregion}
3
4 We define a signal region to look for possible
5 new physics contributions in the opposite sign isolated
6 dilepton sample. The choice of signal region is driven by
7 three observations:
8 \begin{enumerate}
9 \item astrophysical evidence for dark matter suggests that
10 we concentrate on the region of high \met;
11 \item new physics signals should have high $\sqrt{\hat{s}}$;
12 \item observable high cross section new physics signals
13 are likely to be produced strongly; thus, we expect significant
14 hadronic activity in conjunction with the two leptons.
15 \end{enumerate}
16
17 Following these observations, we add the following two requirements
18 to the preselection of Section~\ref{sec:eventSel}:
19 \begin{center}
20 $\mathrm{SumJetPt}>300$~GeV and $\met/\sqrt{\rm SumJetPt} > 8.5$~GeV$^{1/2}$.
21 \end{center}
22
23 \noindent This selection preserves about 1\% of the $t\bar{t}$
24 signal. As shown in Table~\ref{tab:sigyield}, the expected total SM yield in 34.0~pb$^{-1}$ is 1.3 events,
25 while the expectations from the LMO and LM1 SUSY benchmark points are 8.6 and
26 3.6 events, respectively, computed at NLO.
27
28
29 We cut on \met$/\sqrt{\rm SumJetPt}$ rather than \met
30 because the variables SumJetPt and \met$/\sqrt{\rm SumJetPt}$ are
31 largely uncorrelated for the dominant $t\bar{t}$ background.
32 This allows us to use a data driven ABCD method to estimate the
33 background (see Section~\ref{sec:abcd}).
34
35
36
37
38 \begin{table}[hbt]
39 \begin{center}
40 \caption{\label{tab:sigyield} MC expected yields in the signal region for 34.0~pb$^{-1}$.
41 The errors are statistical only.}
42 \begin{tabular}{lcccc}
43 %%%official json v3, 33.96/pb, 38X MC (D6T for ttbar and DY)
44 \hline
45 Sample & $ee$ & $\mu\mu$ & $e\mu$ & tot \\
46 \hline
47 $t\bar{t}\rightarrow \ell^{+}\ell^{-}$ & 0.28 $\pm$ 0.03 & 0.22 $\pm$ 0.03 & 0.57 $\pm$ 0.05 & 1.07 $\pm$ 0.06 \\
48 $t\bar{t}\rightarrow \mathrm{other}$ & 0.01 $\pm$ 0.01 & 0.00 $\pm$ 0.00 & 0.01 $\pm$ 0.01 & 0.02 $\pm$ 0.01 \\
49 $Z^0 \rightarrow \ell^{+}\ell^{-}$ & 0.04 $\pm$ 0.04 & 0.04 $\pm$ 0.04 & 0.04 $\pm$ 0.04 & 0.12 $\pm$ 0.07 \\
50 $W^{\pm}$ + jets & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 \\
51 $W^+W^-$ & 0.00 $\pm$ 0.00 & 0.01 $\pm$ 0.00 & 0.02 $\pm$ 0.01 & 0.03 $\pm$ 0.01 \\
52 $W^{\pm}Z^0$ & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 \\
53 $Z^0Z^0$ & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 \\
54 single top & 0.00 $\pm$ 0.00 & 0.00 $\pm$ 0.00 & 0.01 $\pm$ 0.00 & 0.01 $\pm$ 0.00 \\
55 \hline
56 total SM MC & 0.34 $\pm$ 0.05 & 0.28 $\pm$ 0.05 & 0.65 $\pm$ 0.06 & 1.27 $\pm$ 0.10 \\
57 \hline
58 data & 0 & 0 & 1 & 1 \\
59 \hline
60 % LM0 & 1.71 $\pm$ 0.10 & 2.05 $\pm$ 0.11 & 2.36 $\pm$ 0.12 & 6.12 $\pm$ 0.19 \\
61 % LM1 & 0.87 $\pm$ 0.03 & 1.08 $\pm$ 0.03 & 0.55 $\pm$ 0.02 & 2.50 $\pm$ 0.04 \\
62 %susy k-factors
63 LM0 & 2.37 $\pm$ 0.14 & 2.85 $\pm$ 0.15 & 3.41 $\pm$ 0.17 & 8.63 $\pm$ 0.27 \\
64 LM1 & 1.24 $\pm$ 0.04 & 1.51 $\pm$ 0.04 & 0.81 $\pm$ 0.03 & 3.56 $\pm$ 0.06 \\
65
66 \hline
67 \end{tabular}
68 \end{center}
69 \end{table}