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\section{Search in the All-Hadronic Final State} |
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\label{sec:alphat} |
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\begin{figure*}[!ht] |
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\centering |
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%\begin{center} |
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\begin{tabular}{cc} |
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\includegraphics[width=0.45\textwidth]{HCPPlots/AlphaT_le3j_prelim.pdf} & |
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\includegraphics[width=0.4\textwidth]{HCPPlots/hadronic_2b_le3j_logy.pdf} \\ |
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\end{tabular} |
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\caption{ |
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The distribution of the \alphat\ variable (left) and the $H_T$ distribution in data, compared to the SM background expectation (right). |
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\label{fig:alphat} |
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} |
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%\end{center} |
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\end{figure*} |
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|
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The production of bottom squark pairs, followed by the decay $\tilde{b}\to b\lsp$, leads events with |
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two b-jets and \met. In this section we report the results from a search in the all-hadronic final state using the |
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\alphat\ variable, discussed below, which discriminates between backgrounds with real and fake \met. |
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These results probe bottom squarks with masses up to approximately 600 GeV. Additional interpretations in models with gluino-mediated |
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top and bottom squark pair production are presented in Ref.~\cite{ref:alphat}. |
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\begin{figure*} |
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\centering |
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%\begin{center} |
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\begin{tabular}{cc} |
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\includegraphics[width=0.45\textwidth]{HCPPlots/AlphaT_le3j_prelim.pdf} & |
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\includegraphics[width=0.45\textwidth]{HCPPlots/hadronic_2b_le3j_logy.pdf} \\ |
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\end{tabular} |
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\caption{ |
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The distribution of the \alphat\ variable (left) and the $H_T$ distribution in data, compared to the SM background expectation (right). |
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\label{fig:alphat} |
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} |
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%\end{center} |
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\end{figure*} |
