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Revision 1.3 by benhoob, Wed Sep 26 22:07:08 2012 UTC

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1   \section{Interpretation}
2  
3 < The results of this search will be interpreted in the context of simplified model spectra (SMS).
4 < For the inclusive analysis, we will use the T5zz model depicted in Fig.~\ref{fig:diagrams} (left).
5 < For the targeted analysis, we will use the TChiWZ model depicted in Fig.~\ref{fig:diagrams} (right),
6 < and a GMSB model which produces a signature of \zzmet.
3 > In this section, we interpret the results of the targeted search in the context of the \wzmet\ model depicted in Fig.~\ref{fig:diagrams} (right).
4 > An interpretation in the GMSB model which produces a signature of \zzmet\ will be added. The results of the targeted search presented here
5 > will be combined with those of the trilepton ewkino search for the final \wzmet\ interpretation, and with the quadlepton ewkino search
6 > for the final GMSB \zzmet\ interpretation.
7 >
8 > The exclusion is performed using the results of simultaneous counting experiments in the exclusive \MET\ signal regions defined by \MET\ $>$ 80 GeV,
9 > as summarized in Table~\ref{tab:results_targ} (commonly referred to as a ``shape analysis'').
10 > The signal efficiency times acceptance and cross section upper limits are displayed in Fig.~\ref{fig:results_wzmet},
11 > along with the observed and expected exclusion contours, which are compared to the 2011 observed exclusion contour.
12 > Figure~\ref{fig:results_wzmetpoints} shows the excluded points used to derive the exclusion contours. We note that the map of exclusion
13 > contours appears quite ragged since for many of the points the cross section upper limit is very close to the theory cross section.
14 > Therefore we do not expect the ragged exclusion region to be an issue for the final results since
15 > we currently have 9.2 fb$^{-1}$ and expect the luminosity to increase significantly. A {\bf VERY APPROXIMATE} projection of the expected excluded region
16 > for an integrated luminosity of 15 fb$^{-1}$ (a rough guess at the final HCP data sample) is obtained by scaling the expected cross section limits by
17 > $\sqrt{(9.2 \rm{fb}^{-1})/(15 \rm{fb}^{-1})}$, as displayed in Fig.~\ref{fig:results_15fb}.
18 >
19 > \begin{figure}[!ht]
20 > \begin{center}
21 > \begin{tabular}{cc}
22 > \includegraphics[width=0.45\textwidth]{plots/wzsms_eff.pdf}
23 > \includegraphics[width=0.45\textwidth]{plots/wzsms_xsec.pdf}
24 > \end{tabular}
25 > \caption{ Interpretation of the targeted analysis in the \wzmet\ model. The acceptance times efficiency (left) and cross section
26 > upper limit (right) and displayed. The observed and expected exclusion contours are indicated and compared to the observed
27 > exclusion from the 2011 analysis.
28 > \label{fig:results_wzmet}}
29 > \end{center}
30 > \end{figure}
31 >
32 > \begin{figure}[!hb]
33 > \begin{center}
34 > \includegraphics[width=0.75\textwidth]{plots/wzsms_points.pdf}
35 > \caption{ Observed (left) and expected (right) excluded points for the \wzmet\ interpretation, with the corresponding exclusion contours overlaid.
36 > \label{fig:results_wzmetpoints}}
37 > \end{center}
38 > \end{figure}
39 >
40 > \clearpage
41 >
42 > \begin{figure}[!ht]
43 > \begin{center}
44 > \includegraphics[width=0.5\textwidth]{plots/wzsms_expected_15fb.pdf}
45 > \caption{ A {\bf VERY APPROXIMATE} projection of the expected excluded points for an integrated luminosity of 15$^{-1}$.
46 > \label{fig:results_15fb}}
47 > \end{center}
48 > \end{figure}
49 >

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