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1 %\section{Preselection yields}
2 %\label{sec:yields}
3
4 The data yields and corresponding MC predictions after this event preselection
5 are given in Table~\ref{tab:yields}. The MC yields are normalized to~\lumifinal\ using
6 next-to-leading order (NLO) cross sections. At the current LHC luminosity, the mean
7 number of expected pile-up interactions is approximately 5. In the MC, pile-up interactions
8 are superimposed on the hard collision, and the MC is reweighted such that the distribution
9 of reconstructed primary vertices matches that in data. As expected, the MC predicts that the
10 sample passing the preselection is dominated by dilepton $t\bar{t}$. The data yield is in
11 reasonable agreement with the prediction. We also quote the yields for
12 the LM1 and LM3 benchmark scenarios.
13
14 \begin{table}[htb]
15 \begin{center}
16 \caption{\label{tab:yields} Data yields and MC predictions after preselection, using the quoted NLO production cross sections $\sigma$.
17 The \ttll\ corrresponds to dilepton $t\bar{t}$, including
18 $t \to W \to \ell$; \tttau\ corresponds to dilepton $t\bar{t}$ in which at least 1 $W$ decays via
19 $t \to W \to \tau \to \ell$; \ttfake\ includes all other $t\bar{t}$ decay modes.
20 The samples of MC $t\bar{t}$, $W^{\pm}$ + jets, and single-top events were
21 generated with \MADGRAPH. The Drell--Yan sample (which includes events with
22 invariant masses as low as 10\GeVcc) was generated using a mixture of \MADGRAPH\ and
23 \PYTHIA and contains decays to the $\tau^+\tau^-$ final state. All other samples were generated with \PYTHIA.
24 The LM0 and LM1 benchmark scenarios are defined in the text; the quoted $\sigma$ values refer to the total production
25 cross section for SUSY particles in these scenarios. Uncertainties are statistical only.
26 }
27 \vspace{2 mm}
28 \begin{tabular}{lr|cccc}
29 \hline
30 Sample & $\sigma$ & $ee$ & $\mu\mu$ & $e\mu$ & total \\
31 \hline
32 \ttll & X & 120.1 $\pm$ 2.9 &133.1 $\pm$ 2.9 &320.3 $\pm$ 4.6 &573.5 $\pm$ 6.1 \\
33 \tttau & X & 27.5 $\pm$ 1.4 & 33.3 $\pm$ 1.4 & 71.5 $\pm$ 2.2 &132.3 $\pm$ 3.0 \\
34 \ttfake & 140.6 & 4.5 $\pm$ 0.6 & 1.3 $\pm$ 0.3 & 8.1 $\pm$ 0.7 & 13.9 $\pm$ 1.0 \\
35 DY & 18417 & 6.6 $\pm$ 1.8 & 9.5 $\pm$ 2.1 & 13.4 $\pm$ 2.6 & 29.6 $\pm$ 3.8 \\
36 \WW & 2.9 & 1.4 $\pm$ 0.2 & 1.5 $\pm$ 0.2 & 3.4 $\pm$ 0.2 & 6.3 $\pm$ 0.3 \\
37 \WZ & 0.3 & 0.3 $\pm$ 0.0 & 0.4 $\pm$ 0.0 & 0.7 $\pm$ 0.1 & 1.3 $\pm$ 0.1 \\
38 \ZZ & 4.3 & 0.1 $\pm$ 0.0 & 0.1 $\pm$ 0.0 & 0.2 $\pm$ 0.0 & 0.4 $\pm$ 0.0 \\
39 single top & 33 & 4.5 $\pm$ 0.2 & 5.0 $\pm$ 0.2 & 11.9 $\pm$ 0.3 & 21.4 $\pm$ 0.5 \\
40 \wjets & 28049 & 4.5 $\pm$ 1.9 & 0.0 $\pm$ 0.0 & 2.8 $\pm$ 1.7 & 7.3 $\pm$ 2.6 \\
41 \hline
42 total SM MC & & 169.7 $\pm$ 4.2 &184.3 $\pm$ 3.9 &432.2 $\pm$ 6.0 &786.1 $\pm$ 8.3 \\
43 \hline
44 data & & 193 & 201 & 485 & 879 \\
45 \hline
46 LM1 & 6.7 & 22.3 $\pm$ 0.6 & 24.8 $\pm$ 0.6 & 12.8 $\pm$ 0.4 & 59.9 $\pm$ 0.9 \\
47 LM3 & X & 5.2 $\pm$ 0.2 & 6.3 $\pm$ 0.2 & 9.0 $\pm$ 0.2 & 20.4 $\pm$ 0.4 \\
48 \hline
49 \end{tabular}
50 \end{center}
51 \end{table}
52