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\section{Interpretation}
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\label{sec:interpretation}
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{\bf All results in this section correspond to 9.2 fb$^{-1}$ results and will be updated later.}
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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)
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and a gauge-mediated SUSY breaking (GMSB) model that produces a signature of \zzmet\ will be added. The results of the targeted search presented here
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will be combined with those of the trilepton ewkino search for the final \wzmet\ interpretation, and with the quadlepton ewkino search
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for the final GMSB \zzmet\ interpretation.
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The exclusion is performed using the results of simultaneous counting experiments in the five exclusive \MET\ signal regions defined by \MET\ $>$ 80 GeV,
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as summarized in Table~\ref{tab:results_targ} (commonly referred to as a ``shape analysis'').
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The upper limit calculation is performed with the LandS software using the LHC-type CLs criterion.
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The signal efficiency uncertainties include the luminosity (4.4\%), acceptance for the b-jet veto (4\%), lepton ID and isolation efficiency (2\% per lepton),
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and trigger efficiency (3\%). The uncertainty from JES is determined following the POG-recommended procedure, by varying the jet energies by the
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\pt- and $\eta$-dependent uncertainties and propagating this to the jet multiplicity, dijet mass, and \MET.
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The background uncertainties are quoted in Table~\ref{tab:results_targ}. For each background contribution, the uncertainty is assumed to be 100\%
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correlated across all signal regions.
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For the \wzmet\ model, the signal efficiency times acceptance and cross section upper limits are displayed in Fig.~\ref{fig:results_wzmet},
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along with the observed and expected exclusion contours, which are compared to the 2011 observed exclusion contour.
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Figure~\ref{fig:results_wzmetpoints} shows the excluded points used to derive the exclusion contours. We note that the map of exclusion
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contours appears quite ragged since for many of the points the cross section upper limit is very close to the theory cross section.
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Therefore we do not expect the ragged exclusion region to be an issue for the final results since
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we currently have 9.2 fb$^{-1}$ and expect the luminosity to increase significantly. A {\bf VERY APPROXIMATE} projection of the expected excluded region
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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
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$\sqrt{(9.2 \rm{fb}^{-1})/(15 \rm{fb}^{-1})}$, as displayed in Fig.~\ref{fig:results_15fb}.
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\begin{figure}[!ht]
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\begin{center}
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\begin{tabular}{cc}
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\includegraphics[width=0.45\textwidth]{plots/wzsms_eff.pdf}
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\includegraphics[width=0.45\textwidth]{plots/wzsms_xsec.pdf}
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\end{tabular}
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\caption{ Interpretation of the targeted analysis in the \wzmet\ model. The acceptance times efficiency (left) and cross section
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upper limit (right) are displayed. The observed and expected exclusion contours are indicated and compared to the observed
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exclusion from the 2011 analysis.
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%\newline
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%Interpretation of the $\rm{Z}+\rm{dijet}$ analysis in the \wzmet\ model of Fig.~2(a).
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%The shading indicates the cross section upper limit. The observed and expected exclusion contours are indicated and compared to the observed
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%exclusion from the 2011 analysis. The region below the contours is excluded at 95\% confidence level.
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\label{fig:results_wzmet}}
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\end{center}
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\end{figure}
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\begin{figure}[!hb]
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\begin{center}
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\includegraphics[width=0.75\textwidth]{plots/wzsms_points.pdf}
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\caption{ Observed (left) and expected (right) excluded points for the \wzmet\ interpretation, with the corresponding exclusion contours overlaid.
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\label{fig:results_wzmetpoints}}
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\end{center}
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\end{figure}
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\clearpage
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\begin{figure}[!ht]
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\begin{center}
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\includegraphics[width=0.5\textwidth]{plots/wzsms_expected_15fb.pdf}
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\caption{ A {\bf VERY APPROXIMATE} projection of the expected excluded points for an integrated luminosity of 15$^{-1}$.
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\label{fig:results_15fb}}
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\end{center}
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\end{figure}
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The results of the interpretation in the GMSB \zzmet\ model are displayed in Fig.~\ref{fig:results_gmsb},
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as a function of the chargino and neutralino mass parameter $\mu$. These results exclude the range $196 < \mu < 316$~GeV.
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\begin{figure}[!hb]
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\begin{center}
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\includegraphics[width=0.5\textwidth]{plots/ZDIJET_GMSB.pdf}
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\caption{ Interpretation of the targeted analysis in the GMSB \zzmet\ model.
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%\newline
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%Interpretation of the $\rm{Z}+\rm{dijet}$ analysis in the GMSB model discussed in the text.
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%The observed and expected cross section upper limits are indicated as a function of the mass parameter $\mu$, and are compared to the theory
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%cross section. The region $196 < \mu < 316$~GeV is excluded at 95\% confidence level.
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\label{fig:results_gmsb}}
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\end{center}
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\end{figure}
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\begin{table}[htb]
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\begin{center}
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\footnotesize
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\caption{\label{tab:gmsb} Summary of the parameters for the GMSB model used for the \zzmet\ interpretation.
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The masses of the lightest and second light neutralino, lightest chargino, and total next-to-leading order
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cross section, are indicated.}
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\begin{tabular}{l|cccc}
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\hline
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\hline
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$\mu$ [GeV] & $m_{\chizi}$ [GeV] & $m_{\chizii}$ [GeV] & $m_{\chipm}$ [GeV] & $\sigma_{\mathrm{NLO}}$ [pb] \\
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%$\mu$ [GeV] & $m_{\chizi}$ [GeV] & & & \\
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\hline
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%110 & 102 & 111 & 104 & 7.3 \\
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130 & 122 & 131 & 124 & 3.8 \\
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150 & 141 & 151 & 144 & 2.1 \\
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170 & 161 & 171 & 164 & 1.3 \\
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190 & 181 & 191 & 184 & 0.84 \\
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210 & 201 & 211 & 203 & 0.56 \\
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230 & 221 & 231 & 223 & 0.38 \\
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250 & 240 & 251 & 243 & 0.27 \\
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270 & 260 & 271 & 263 & 0.20 \\
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290 & 280 & 291 & 283 & 0.14 \\
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310 & 299 & 311 & 302 & 0.11 \\
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330 & 319 & 331 & 322 & 0.080 \\
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350 & 339 & 351 & 342 & 0.061 \\
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370 & 358 & 371 & 362 & 0.047 \\
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390 & 378 & 391 & 381 & 0.037 \\
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410 & 398 & 411 & 401 & 0.029 \\
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\hline
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\hline
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\end{tabular}
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\end{center}
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\end{table}
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