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Examples of SUSY scenarios producing at least one SM Higgs boson in the final state. Left: $\stoptwo$ pair production, with $\stoptwo \ra H/Z \, \stopone$ investigated in~\cite{higgs_from_stop}; right: higgsino pair production with $\chi \ra H/Z \, \tilde{G}$ searched for by~\cite{higgs_from_ewkino}.
Exclusion limits of \cite{higgs_from_stop} for the $\stoptwo \ra H/Z \stopone$ simplified model. Left: $\stoptwo \ra H \stopone$ (100\%), center: $\stoptwo \ra Z \stopone$ (100\%), right: summary plot with the two extreme cases and the case $\BR(\stoptwo \ra H \stopone) = \BR(\stoptwo \ra Z \stopone) =$ 50\%.
Exclusion limits of \cite{higgs_from_stop} for the $\stoptwo \ra H/Z \stopone$ simplified model. Left: $\stoptwo \ra H \stopone$ (100\%), center: $\stoptwo \ra Z \stopone$ (100\%), right: summary plot with the two extreme cases and the case $\BR(\stoptwo \ra H \stopone) = \BR(\stoptwo \ra Z \stopone) =$ 50\%.
Exclusion limits for the CMS $M_{T2}$ analysis \cite{MT2} for direct $\tilde{q}$ pair production (left plot) and gluino production with each gluino decaying to a light $q\bar{q}$ pair and the LSP (center plot). Right plot: exclusion limits for the direct production of $\sbottom$ pairs in \cite{sbottom}.
Left: exclusion limits for the monojet search \cite{monojet}. Right: exclusion limits for gluino pairs production, with gluinos decaying to different mixtures of $b \bar{b} \chiz$, $b \bar{t} \chiz$, and $t \bar{t} \chiz$, obtained by the razor inclusive analysis \cite{razor_incl}.
Exclusion limits for the CMS $M_{T2}$ analysis \cite{MT2} for direct $\tilde{q}$ pair production (left plot) and gluino production with each gluino decaying to a light $q\bar{q}$ pair and the LSP (center plot). Right plot: exclusion limits for the direct production of $\sbottom$ pairs in \cite{sbottom}.
Results of the opposite-sign same-flavor dilepton analysis \cite{edge}. Left: fit of the central events; the black dotted line represents the flavor symmetric background (dominated by $t\bar{t}$), the red component is the Drell-Yan background, and the green dotted line corresponds to the small signal-like excess that is seen. Right: results of the cut-and-count analysis for the central events.
Cross sections for the main SUSY production mechanisms at the LHC, at a $p-p$ collision energy of 8 TeV.
Examples of SUSY scenarios producing at least one SM Higgs boson in the final state. Left: $\stoptwo$ pair production, with $\stoptwo \ra H/Z \, \stopone$ investigated in~\cite{higgs_from_stop}; right: higgsino pair production with $\chi \ra H/Z \, \tilde{G}$ searched for by~\cite{higgs_from_ewkino}.
Exclusion limits of \cite{higgs_from_ewkino} on higgsino production. Left plot: limits as a function of the higgsino mass (x axis) and $\BR(\chiz \ra h \tilde{G}) = 1 - \BR(\chiz \ra Z \tilde{G})$ (y axis); the bottom left corner below the black solid line is excluded by the analysis. The right plot shows the most sensitive channel on the same plane contributing to the exclusion.
Left: exclusion limits for the monojet search \cite{monojet}. Right: exclusion limits for gluino pairs production, with gluinos decaying to different mixtures of $b \bar{b} \chiz$, $b \bar{t} \chiz$, and $t \bar{t} \chiz$, obtained by the razor inclusive analysis \cite{razor_incl}.
Exclusion limits of the razor photon analysis \cite{razor_phot}. Left plot: exclusion in the $m_{\tilde{g}}$ vs $m_{\tilde{q}}$ plane in a General Gauge Mediated scenario, right plot: exclusions for the simplified model in which gluino pairs are produced and each gluino decays to $q\bar{q}\chiz$, with the virtual $\chiz$ decaying to a gravitino $\tilde{G}$ and a photon.
Exclusion limits for the CMS $M_{T2}$ analysis \cite{MT2} for direct $\tilde{q}$ pair production (left plot) and gluino production with each gluino decaying to a light $q\bar{q}$ pair and the LSP (center plot). Right plot: exclusion limits for the direct production of $\sbottom$ pairs in \cite{sbottom}.
Exclusion limits of \cite{higgs_from_ewkino} on higgsino production. Left plot: limits as a function of the higgsino mass (x axis) and $\BR(\chiz \ra h \tilde{G}) = 1 - \BR(\chiz \ra Z \tilde{G})$ (y axis); the bottom left corner below the black solid line is excluded by the analysis. The right plot shows the most sensitive channel on the same plane contributing to the exclusion.
Exclusion limits of \cite{higgs_from_stop} for the $\stoptwo \ra H/Z \stopone$ simplified model. Left: $\stoptwo \ra H \stopone$ (100\%), center: $\stoptwo \ra Z \stopone$ (100\%), right: summary plot with the two extreme cases and the case $\BR(\stoptwo \ra H \stopone) = \BR(\stoptwo \ra Z \stopone) =$ 50\%.
Results of the opposite-sign same-flavor dilepton analysis \cite{edge}. Left: fit of the central events; the black dotted line represents the flavor symmetric background (dominated by $t\bar{t}$), the red component is the Drell-Yan background, and the green dotted line corresponds to the small signal-like excess that is seen. Right: results of the cut-and-count analysis for the central events.
Exclusion limits of the razor photon analysis \cite{razor_phot}. Left plot: exclusion in the $m_{\tilde{g}}$ vs $m_{\tilde{q}}$ plane in a General Gauge Mediated scenario, right plot: exclusions for the simplified model in which gluino pairs are produced and each gluino decays to $q\bar{q}\chiz$, with the virtual $\chiz$ decaying to a gravitino $\tilde{G}$ and a photon.