The CMS Collaboration has released the results of its search for supersymmetry, by applying an ${\alpha }_T$ method to $1.1/\mathrm{fb}$ of data at 7 TeV. The null result excludes (at 95% C.L.) a low-mass region of the Constrained MSSM’s parameter space that was previously favored by other experiments. Additionally, the negative result of the XENON100 dark matter search has excluded (at 90% C.L.) values of the spin-independent scattering cross sections ${\sigma }_p^{\mathrm{SI}}$ as low as ${10}^{-8}\mathrm{pb}$. We incorporate these improved experimental constraints into a global Bayesian fit of the Constrained MSSM by constructing approximate likelihood functions. In the case of the ${\alpha }_T$ limit, we simulate detector efficiency for the CMS ${\alpha }_{T}1.1/\mathrm{fb}$ analysis and validate our method against the official 95% C.L. contour. We identify the 68% and 95% credible posterior regions of the CMSSM parameters, and also find the best-fit point. We find that the credible regions change considerably once a likelihood from ${\alpha }_T$ is included, in particular, the narrow light Higgs resonance region becomes excluded, but the focus point/horizontal branch region remains allowed at the $1\sigma$ level. Adding the limit from XENON100 has a weaker additional effect, in part due to large uncertainties in evaluating ${\sigma }_p^{\mathrm{SI}}$, which we include in a conservative way, although we find that it reduces the posterior probability of the focus point region to the $2\sigma$ level. The new regions of high posterior favor squarks lighter than the gluino and all but one Higgs bosons heavy. The dark matter neutralino mass is found in the range $250\mathrm{GeV}\lesssim m_{\chi }\lesssim 343\mathrm{GeV}$ (at $1\sigma$) while, as the result of improved limits from the LHC, the favored range of ${\sigma }_p^{\mathrm{SI}}$ is pushed down to values below ${10}^{-9}\mathrm{pb}$. We highlight tension between $\delta (g-2{)}_{\mu }^{\mathrm{SUSY}}$ and $\mathcal{B}\mathcal{R}(\overline{B}\to X_s\gamma )$, which is exacerbated by including the ${\alpha }_T$ limit; each constraint favors a different region of the CMSSM’s mass parameters.

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