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1   \section{Results}
2   \label{sec:results}
3  
4 < \noindent {\color{red} In the 11 pb everything is very
5 < simple because there are a few zeros.  This text is written
6 < for the full dataset under the assumption that some of these
7 < numbers will not be zero anymore.}
4 > %\noindent {\color{red} In the 11 pb everything is very
5 > %simple because there are a few zeros.  This text is written
6 > %for the full dataset under the assumption that some of these
7 > %numbers will not be zero anymore.}
8  
9   \begin{figure}[tbh]
10   \begin{center}
# Line 33 | Line 33 | is 0.5 events.
33   \begin{table}[hbt]
34   \begin{center}
35   \caption{\label{tab:datayield} Data yields in the four
36 < regions of Figure~\ref{fig:abcdData}.  We also show the
37 < SM Monte Carlo expectations.}
36 > regions of Figure~\ref{fig:abcdData}.  The quoted uncertainty
37 > on the prediction in data is statistical only, assuming Gaussian errors.
38 > We also show the SM Monte Carlo expectations.}
39   \begin{tabular}{|l|c|c|c|c||c|}
40   \hline
41        &A   & B    & C   & D   & AC/B \\ \hline
42 < Data  &3   & 6    & 1   & 0   & $0.5^{+x}_{-y}$ \\
42 > Data  &3   & 6    & 1   & 0   & $0.5^{+0.6}_{-0.5}$ \\
43   SM MC &2.5 &11.2  & 1.5 & 0.4 & 0.4 \\
44   \hline
45   \end{tabular}
46   \end{center}
47   \end{table}
48  
49 < As a cross-check, we can subtract from the yields in
50 < Table~\ref{tab:datayield} the expected DY contributions
51 < from Table~\ref{tab:ABCD-DY} in order to get a ``purer''
52 < estimate of the $t\bar{t}$ contribution.  The result
53 < of this exercise is {\color{red} xx} events.
49 > %As a cross-check, we can subtract from the yields in
50 > %Table~\ref{tab:datayield} the expected DY contributions
51 > %from Table~\ref{tab:ABCD-DY} in order to get a ``purer''
52 > %estimate of the $t\bar{t}$ contribution.  The result
53 > %of this exercise is {\color{red} xx} events.
54  
55   \subsection{Background estimate from the $P_T(\ell\ell)$ method}
56   \label{sec:victoryres}
57  
57
58
58   The number of data events in region $D'$, which is defined in
59   Section~\ref{sec:othBG} to be the same as region $D$ but with the
60   $\met/\sqrt{\rm SumJetPt}$ requirement
61   replaced by a $P_T(\ell\ell)/\sqrt{\rm SumJetPt}$ requirement
62 < is $N_{D'}=0$.  Thus the BG prediction is
63 < $N_D = K^{MC} \cdot K_{\rm fudge} \cdot N_{D'} = xx$
64 < where we used $K^{MC}=xx$ and $K_{\rm fudge}=xx \pm yy$.
62 > is $N_{D'}=1$.  Thus the BG prediction is
63 > $N_D = K \cdot N_{D'} = 1.5$
64 > where $K=1.5 \pm xx$ as derived in Sec.~\ref{sec:victory}.
65   Note that if we were to subtract off from region $D'$
66 < the {\color{red} $xx$} DY events estimated from
67 < Table~\ref{tab:ABCD-DYptll}, the background
68 < prediction would change to $N_D=xx$.
66 > the {\color{red} 0.4 $\pm$ 0.4} DY events estimated from
67 > Section~\ref{sec:othBG}, the background
68 > prediction would change to $N_D=0.9 \pm xx$ events.
69 >
70 > %%%TO BE REPLACED
71 > %{\color{red}As mentioned previously, for the 11/pb analysis
72 > %we use the $K$ factor from data and take $K=1$.
73 > %This will change for the full dataset.  We will also pay
74 > %more attention to the statistical errors.}
75 >
76 > %The number of data events in region $D'$, which is defined in
77 > %Section~\ref{sec:othBG} to be the same as region $D$ but with the
78 > %$\met/\sqrt{\rm SumJetPt}$ requirement
79 > %replaced by a $P_T(\ell\ell)/\sqrt{\rm SumJetPt}$ requirement
80 > %is $N_{D'}=1$.  Thus the BG prediction is
81 > %$N_D = K \cdot K_{\rm fudge} \cdot N_{D'} = 1.5$
82 > %where we used $K=1.5 \pm xx$ and $K_{\rm fudge}=1.0 \pm 0.0$.
83 > %Note that if we were to subtract off from region $D'$
84 > %the {\color{red} 0.4 $\pm$ 0.4} DY events estimated from
85 > %Section~\ref{sec:othBG}, the background
86 > %prediction would change to $N_D=0.9 \pm xx$ events.
87 > %{\color{red} When we do this with a real
88 > %$K_{\rm fudge}$, the fudge factor will be different
89 > %after the DY subtraction.}
90  
91   As a cross-check, we use the $P_T(\ell \ell)$
92   method to also predict the number of events in the
93   control region $120<{\rm SumJetPt}<300$ GeV and
94   \met/$\sqrt{\rm SumJetPt} > 8.5$.  We predict
95   $5.6^{+x}_{-y}$ events and we observe 4.
96 < {\color{red} Note: when we do this more carefully
97 < we will need to use a different $K$ and a different $K_{fudge}$>}
96 > The results of the $P_T(\ell\ell)$ method are
97 > summarized in Figure~\ref{fig:victory}.
98 >
99 > \begin{figure}[hbt]
100 > \begin{center}
101 > \includegraphics[width=0.48\linewidth]{victory_control.png}
102 > \includegraphics[width=0.48\linewidth]{victory_sig.png}
103 > \caption{\label{fig:victory}\protect Distributions of
104 > tcMet/$\sqrt{\rm SumJetPt}$ for the control and signal region.
105 > We show the oberved distributions in both Monte Carlo and data.
106 > We also show the distributions predicted from
107 > ${P_T(\ell\ell)}/\sqrt{\rm SumJetPt}$ in both MC and data.}
108 > \end{center}
109 > \end{figure}
110 >
111  
112 + \subsection{Summary of results}
113   To summarize: we see no evidence for an anomalous
114   rate of opposite sign isolated dilepton events
115   at high \met and high SumJetPt.  The extraction of
116   quantitative limits on new physics models is discussed
117 < in Section~\ref{sec:limits}.
117 > in Section~\ref{sec:limit}.

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