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# User Rev Content
1 benhoob 1.1 \section{Introduction}
2     \label{sec:intro}
3    
4     Supersymmetry (SUSY) is a popular extension to the standard model (SM) of particle physics, which may explain
5     the 16 orders of magnitude difference between the electroweak and Planck scales (hierarchy problem), introduce
6     a natural candidate for the dark matter weakly-interacting massive particle (WIMP), and lead to the unification of
7     gauge couplings. In order to solve the hierarchy problem without fine-tuning, SUSY must introduce
8     light top and bottom squarks (SUSY partners of the top and bottom quarks) and light gluinos
9     (SUSY partner of the gluon)~\cite{Barbieri:1987fn,deCarlos1993320,Dimopoulos1995573,Barbieri199676,Papucci:2011wy}.
10     If R-parity is conserved, the lightest SUSY particle (LSP),
11     usually the lightest neutralino \lsp, is a stable WIMP. If produced in pp collisions this
12     particle carries away undetected energy and leads to large missing transverse energy (\met).
13     In this note we present the results of searches for the top and bottom squarks in final states with \met,
14     using data collected by the Compact Muon Solenoid (CMS) detector at the
15     Large Hadron Collider (LHC). The data was collected at a center-of-mass energy of $\sqrt{s}=8$~TeV in 2012
16     and corresponds to an integrated luminosity of approximately 10~fb$^{-1}$.
17    
18     \begin{figure*}
19     \centering
20     %\begin{center}
21     \begin{tabular}{cc}
22     \includegraphics[width=0.45\textwidth]{HCPPlots/T2tt.pdf} &
23     \includegraphics[width=0.45\textwidth]{HCPPlots/A2.pdf} \\
24     \includegraphics[width=0.45\textwidth]{HCPPlots/T2bb.pdf} &
25     \includegraphics[width=0.45\textwidth]{HCPPlots/B2.pdf} \\
26     \end{tabular}
27     \caption{
28     Examples of topologies with top and bottom squarks targeted in the searches described in the text.
29     Top (top) and bottom (bottom) squarks may be produced either directly in pairs (left), or in the
30     decays of the gluino (right).
31     \label{fig:diagrams}
32     }
33     %\end{center}
34     \end{figure*}
35    
36    
37     %\begin{figure*}
38     %\centering
39     %\includegraphics[width=1cm,clip]{HCPPlots/T2tt.pdf}
40     %% Use the relevant command for your figure-insertion program
41     %% to insert the figure file. See example above.
42     %% If not, use
43     %\vspace*{5cm} % Give the correct figure height in cm
44     %\caption{Please write your figure caption here}
45     %\label{fig:diagrams} % Give a unique label
46     %\end{figure*}
47    
48     Top and bottom squarks may either be produced directly in pairs
49     (direct pair production) or in the decays of the gluinos (gluino-mediated squark production).
50     Examples of such processes are indicated in Fig.~\ref{fig:diagrams}.
51     The production of these particles may lead to excesses above the SM background expectations in several final states,
52     depending on the mass hierarchy of the SUSY particles.
53     Here we report the results from three searches which focus on the single lepton final state using the transverse
54     mass~\cite{ref:stop}, the same-sign dilepton final state~\cite{ref:ss}, and the all-hadronic final state~\cite{ref:alphat}.
55