| 44 |
|
a mass less than 500-700~GeV. Several additional interpretations for models with gluino-mediated top and |
| 45 |
|
bottom squark production are presented in Ref.~\cite{ref:ss}. |
| 46 |
|
|
| 47 |
– |
\begin{figure*} |
| 48 |
– |
\centering |
| 49 |
– |
%\begin{center} |
| 50 |
– |
\begin{tabular}{cc} |
| 51 |
– |
\subfloat[] {\includegraphics[width=0.5\textwidth]{HCPPlots/SS_B1.pdf}} & |
| 52 |
– |
\subfloat[] {\includegraphics[width=0.4\textwidth]{HCPPlots/T2bb_interpretation.pdf}} \\ |
| 53 |
– |
\end{tabular} |
| 54 |
– |
\caption{ |
| 55 |
– |
Interpretation of the results of the search in (a) the same-sign dilepton final state for |
| 56 |
– |
bottom squark pair production with $\tilde{b}\to t\chip$ depicted in Fig.~\ref{fig:diagrams}(d), and (b) |
| 57 |
– |
the all-hadronic final state for bottom squark pair production with $\tilde{b}\to b\lsp$ depicted in Fig.~\ref{fig:diagrams}(c). |
| 58 |
– |
\label{fig:ss_interpretation} |
| 59 |
– |
} |
| 60 |
– |
%\end{center} |
| 61 |
– |
\end{figure*} |
| 62 |
– |
|
| 47 |
|
|
| 48 |
|
%\begin{table} |
| 49 |
|
%\centering |
| 61 |
|
%\end{table} |
| 62 |
|
|
| 63 |
|
|
| 64 |
< |
\begin{table*} |
| 64 |
> |
\begin{table*}[t] |
| 65 |
|
\centering |
| 66 |
|
\caption{\label{tab:ss} Summary of the results of the search in the same-sign dilepton final state. |
| 67 |
|
Several signal regions (SR) are indicated, including the kinematic requirements, the prediction of the three background (BG) contributions, |
| 93 |
|
\end{tabular} |
| 94 |
|
\end{scriptsize} |
| 95 |
|
\end{table*} |
| 96 |
+ |
|
| 97 |
+ |
|
| 98 |
+ |
\begin{figure*} |
| 99 |
+ |
\centering |
| 100 |
+ |
%\begin{center} |
| 101 |
+ |
\begin{tabular}{cc} |
| 102 |
+ |
\subfloat[] {\includegraphics[width=0.5\textwidth]{HCPPlots/SS_B1.pdf}} & |
| 103 |
+ |
\subfloat[] {\includegraphics[width=0.4\textwidth]{HCPPlots/T2bb_interpretation.pdf}} \\ |
| 104 |
+ |
\end{tabular} |
| 105 |
+ |
\caption{ |
| 106 |
+ |
Interpretation of the results of the search in (a) the same-sign dilepton final state for |
| 107 |
+ |
bottom squark pair production with $\tilde{b}\to t\chip$ depicted in Fig.~\ref{fig:diagrams}(d), and (b) |
| 108 |
+ |
the all-hadronic final state for bottom squark pair production with $\tilde{b}\to b\lsp$ depicted in Fig.~\ref{fig:diagrams}(c). |
| 109 |
+ |
\label{fig:ss_interpretation} |
| 110 |
+ |
} |
| 111 |
+ |
%\end{center} |
| 112 |
+ |
\end{figure*} |
| 113 |
+ |
|
