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\clearpage
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\section{Data vs. MC Comparison in Preselection Region}
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\label{sec:yields}
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In this section we compare the data and MC samples passing the selection described in Sec.~\ref{sec:eventSelection}
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In the following, the MC is reweighted to match the data distribution of number of reconstructed primary vertices.
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%{\bf FIXME: UPDATE TO 5.1/fb VTX-REWEIGHTING, CURRENTLY USING OUTDATED FUNCTION}.
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The trigger efficiencies of Sec.~\ref{sec:datasets} are applied. In all plots, the last bin contains the overflow.
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We begin by counting the inclusive Z yields. Here we require the presence of two selected leptons without
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any additional requirements on jets or \MET. In Fig.~\ref{fig:dilmass} the distribution of dilepton invariant
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mass in the ee and $\mu\mu$ channels is displayed. In Table~\ref{table:zyields} the yields for selected dilepton
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events in the Z mass window are indicated. Good data vs. MC agreement is observed, within the systematic uncertainties
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of integrated luminosity (4.5\%), trigger efficiency (3\%), \zjets\ and \ttbar\ cross sections.
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\begin{figure}[hbt]
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\begin{center}
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\includegraphics[width=1.0\linewidth]{plots/dilmass_ee_mm.pdf}
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\caption{
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\label{fig:dilmass}\protect
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Dilepton mass distribution for events with two selected leptons
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in the ee (left) and $\mu\mu$ (right) final states.}
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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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\caption{\label{table:zyields} Data and Monte Carlo yields for events with two selected leptons in the Z mass window
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(\bf updated to \lumi).
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}
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\begin{tabular}{lccccc}
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\hline
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\hline
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Sample & ee & $\mu\mu$ & e$\mu$ & total \\
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\hline
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%Loading babies at : ../output/V00-01-04
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%Using selection : (((((isdata==0 || (run<197556 || run>198913))&&(((leptype==0 && (ee==1 || isdata==0))||(leptype==1 && (mm==1 || isdata==0)))||(leptype==2 && (em==1||me==1||isdata==0))))&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(lep1.pt()>20.0 && lep2.pt()>20.0))&&(dilmass>15.0))&&(dilmass>81 && dilmass<101)
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%Using weight : weight * 9.2 * trgeff * vtxweight
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\zjets &22662501 $\pm$ 1660 &3125059 $\pm$ 1873 &1082 $\pm$ 35.8 &5392392 $\pm$ 2503 \\
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\ttbar &1579.1 $\pm$ 22.6 &1998.3 $\pm$ 24.4 &3592.2 $\pm$ 33.5 &7169.5 $\pm$ 47.2 \\
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WW &290.6 $\pm$ 2.9 &387.2 $\pm$ 3.3 &671.2 $\pm$ 4.4 &1349.0 $\pm$ 6.2 \\
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WZ &2052.6 $\pm$ 3.6 &2686.9 $\pm$ 3.9 & 54.1 $\pm$ 0.5 &4793.5 $\pm$ 5.3 \\
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ZZ &1294.6 $\pm$ 2.7 &1708.5 $\pm$ 3.0 & 5.2 $\pm$ 0.1 &3008.3 $\pm$ 4.0 \\
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single top &150.0 $\pm$ 5.9 &192.6 $\pm$ 6.4 &332.9 $\pm$ 8.6 &675.5 $\pm$ 12.2 \\
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\hline
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total SM MC &2271617 $\pm$ 1661 &3132032 $\pm$ 18723 &5738 $\pm$ 50.0 &5409387 $\pm$ 2503 \\
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\hline
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data & 2329993 & 3169480 & 6182 & 5505655 \\
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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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\clearpage
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We next define the preselection region for the inclusive search using the following requirements:
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\begin{itemize}
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\item Number of jets $\geq$ 2;
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\item Same flavor dileptons (opposite flavor yields will be shown since they are used in data for the FS background estimation);
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\item Dilepton invariant mass $81<m_{\ell\ell}<101$ GeV.
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\end{itemize}
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The dilepton mass distributions in the preselection region of the inclusive search (without the dilepton mass requirement applied)
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for the ee and $\mu\mu$ final states are shown in Figure~\ref{fig:dilmass_2j}. In Table~\ref{table:zyields_2j} the data and MC yields
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in thepreselection region are indicated. Good data vs. MC agreement is observed.
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\begin{figure}[hbt]
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\begin{center}
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\includegraphics[width=1.0\linewidth]{plots/dilmass_ee_mm_2j.pdf}
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\caption{
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\label{fig:dilmass_2j}\protect
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Dilepton mass distribution for events in the preselection region of the inclusive search
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in the ee (left) and $\mu\mu$ (right) final states.}
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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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\caption{\label{table:zyields_2j} Data and MC yields in the preselection region of the inclusive search.
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}
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\begin{tabular}{lccccc}
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\hline
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\hline
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Sample & ee & $\mu\mu$ & e$\mu$ & total \\
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\hline
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\zjets & 53187.8 $\pm$ 988.5 &78070.5 $\pm$ 1165.7 & 5.6 $\pm$ 3.6 &131264.0 $\pm$ 1528.4 \\
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\ttbar & 645.3 $\pm$ 17.7 &865.1 $\pm$ 19.7 &1470.4 $\pm$ 25.8 &2980.8 $\pm$ 37.0 \\
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WZ & 431.2 $\pm$ 2.4 &594.6 $\pm$ 2.7 & 5.8 $\pm$ 0.2 &1031.6 $\pm$ 3.6 \\
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ZZ & 269.9 $\pm$ 1.6 &377.7 $\pm$ 1.8 & 0.5 $\pm$ 0.0 &648.1 $\pm$ 2.4 \\
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WW & 15.2 $\pm$ 0.8 & 22.2 $\pm$ 0.9 & 38.9 $\pm$ 1.3 & 76.4 $\pm$ 1.7 \\
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single top & 28.8 $\pm$ 3.2 & 38.0 $\pm$ 3.4 & 72.0 $\pm$ 4.9 &138.8 $\pm$ 6.7 \\
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\hline
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total SM MC & 54578.1 $\pm$ 988.7 &79968.3 $\pm$ 1165.9 &1593.3 $\pm$ 26.5 &136139.7 $\pm$ 1528.9 \\
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data & 54426 & 80367 & 1565 & 136358 \\
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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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\clearpage
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benhoob |
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We next define the preselection region for the targeted search by adding the following requirements:
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\begin{itemize}
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\item Veto events containing a b-tagged jet;
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\item Dijet invariant mass $70<m_{jj}<110$ GeV;
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\item Veto events containing a third selected lepton (electron or muon) with \pt $>$ 20 GeV; %{\bf FIXME: lower third lepton \pt threshold to 10 GeV}.
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\end{itemize}
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The rejection of events with a b-tagged jet strongly suppresses the \ttbar\ background, which is the dominant background in the inclusive search
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after requiring large \MET. The requirement that the jet pair is consistent with originating from W/Z decay is motivated by the fact that we are
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searching for signatures producing V(jj)Z($\ell\ell$)+\MET; this requirement suppresses the \zjets\ and \ttbar\ backgrounds. The veto of events
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containting a third electron or muon suppresses the WZ background, and also serves to make this analyis exclusive with respect to searches in
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the trilepton final state.
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The dilepton mass distributions in the preselection region of the targeted search (without the dilepton mass requirement applied)
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for the ee and $\mu\mu$ final states are shown in Figure~\ref{fig:dilmass_2j_targeted}. In Table~\ref{table:zyields_2j_targeted}
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the data and MC yields in the preselection region are indicated. Good data vs. MC agreement is observed.
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We also show the distribution of dijet mass in the targeted preselection (with the requirement on this quantity removed) in Fig.~\ref{fig:mjj},
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which demonstrates that the MC does a reasonable job of modeling this quantity.
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benhoob |
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\begin{figure}[hbt]
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\begin{center}
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\includegraphics[width=1.0\linewidth]{plots/dilmass_ee_mm_2j_targeted.pdf}
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\caption{
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\label{fig:dilmass_2j_targeted}\protect
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Dilepton mass distribution for events in the preselection region of the targeted search
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in the ee (left) and $\mu\mu$ (right) final states.}
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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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\caption{\label{table:zyields_2j_targeted} Data and MC yields in the preselection region of the inclusive search.
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}
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\begin{tabular}{lccccc}
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\hline
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\hline
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Sample & ee & $\mu\mu$ & e$\mu$ & total \\
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\hline
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\zjets &14108.9 $\pm$ 486.3 &21927.1 $\pm$ 606.4 & 0.0 $\pm$ 0.0 &36036.0 $\pm$ 777.4 \\
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\ttbar & 21.0 $\pm$ 2.9 & 33.4 $\pm$ 3.9 & 53.7 $\pm$ 5.0 &108.0 $\pm$ 6.9 \\
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WZ &135.6 $\pm$ 1.4 &188.5 $\pm$ 1.6 & 1.0 $\pm$ 0.1 &325.1 $\pm$ 2.1 \\
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ZZ &106.0 $\pm$ 1.0 &148.8 $\pm$ 1.2 & 0.1 $\pm$ 0.0 &254.9 $\pm$ 1.5 \\
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WW & 3.4 $\pm$ 0.4 & 4.1 $\pm$ 0.4 & 7.8 $\pm$ 0.5 & 15.2 $\pm$ 0.7 \\
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single top & 2.0 $\pm$ 0.8 & 2.8 $\pm$ 1.1 & 5.5 $\pm$ 1.4 & 10.3 $\pm$ 1.9 \\
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\hline
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total SM MC &14376.9 $\pm$ 486.3 &22304.7 $\pm$ 606.5 & 68.0 $\pm$ 5.2 &36749.6 $\pm$ 777.4 \\
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data & 14647 & 21840 & 74 & 36561 \\
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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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\clearpage
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\begin{figure}[hbt]
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\begin{center}
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\includegraphics[width=1.0\linewidth]{plots/mjj.pdf}
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\caption{
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\label{fig:mjj}\protect
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Distributions of dijet mass for the targeted preselection in the ee (left), $\mu\mu$ (middle) and e$\mu$ (right) final state.}
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\end{center}
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\end{figure}
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