Ratios of B+ differential production cross sections at 13 TeV and at 7 TeV as a function of |yB| for 10 < ptB < 100 GeV or 17 < ptB < 100 GeV. The calculations from FONLL and PYTHIA are provided as well.

B+ differential production cross sections DSIG/DPT for |yB|< 1.45 or |yB|< 2.1, at 13 TeV. The calculations from FONLL and PYTHIA are provided.

B+ differential production cross sections DSIG/DETARAP for 10 < ptB < 100 GeV or 17 < ptB < 100 GeV, at 13 TeV. The calculations from FONLL and PYTHIA are provided.

B+ production cross section for the phase-space region of 10 <= pTB < 17 GeV and |yB| < 1.45, and 17 <= pTB < 100 GeV and |yB| < 2.1. The calculations from FONLL and PYTHIA are provided.

RMS of raw subtracted $p_T$ for jets reconstructed in PbPb collisions (in different centrality bins) with the anti-k$_T$ algorythm with a distance parameter $R=0.3$, in $|\eta|<0.2$.

Inclusive jet cross section in pp collisions, for anti-k$_T$ jets with a distance parameter $R=0.2, 0.3, 0.4$, reconstructed in $|\eta|<0.2$. The '3.7%' luminosity uncertainty is a fully correlated uncertainty, and not included in the point-to-point uncertainty.

Inclusive jet spectra in different centrality bins of PbPb collisions, for anti-k$_T$ jets of distance parameter $R=0.2$, reconstructed in $|\eta|<0.2$. The PbPb spectra in each case are scaled by TAA. The uncertainty on the TAA is considered as global uncertainty (common to all points for a given centrality), and it is not included in the point-to-point uncertainties.

Inclusive jet spectra in different centrality bins of PbPb collisions, for anti-k$_T$ jets of distance parameter $R=0.3$, reconstructed in $|\eta|<0.2$. The PbPb spectra in each case are scaled by TAA. The uncertainty on the TAA is considered as global uncertainty (common to all points for a given centrality), and it is not included in the point-to-point uncertainties.

Inclusive jet spectra in different centrality bins of PbPb collisions, for anti-k$_T$ jets of distance parameter $R=0.4$, reconstructed in $|\eta|<0.2$. The PbPb spectra in each case are scaled by TAA. The uncertainty on the TAA is considered as global uncertainty (common to all points for a given centrality), and it is not included in the point-to-point uncertainties.

Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|<2$, for 0-5\% PbPb centrality. The '5.5%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.

Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|<2$, for 5-10\% PbPb centrality. The '5.9%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.

Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|<2$, for 10-30\% PbPb centrality. The '6.9%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.

Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|<2$, for 30-50\% PbPb centrality. The '10%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.

Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|<2$, for 50-70\% PbPb centrality. The '15%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.

Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, with $|\eta|<2$, for 70-90\% PbPb centrality. The '18%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.

Inclusive jet RAA as a function of average Npart, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, reconstructed in the range $80< p_T < 90$GeV/c and $|\eta|<2$.

Inclusive jet RAA as a function of average Npart, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3, 0.4$, reconstructed in the range $130< p_T < 150$GeV/c and $|\eta|<2$.

Inclusive jet RAA as a function of jet $p_T$, for anti-k$_T$ jets with distance parameter $R=0.2, 0.3$, reconstructed in the range $|\eta|<2$, for 0-10\% PbPb centrality. The '5.7%' combined uncertainty on the pp luminosity and PbPb TAA is considered as global uncertainty (common to all points), and it is not included in the point-to-point uncertainties.

Variance of near-side peak in the 0-10% centrality bin divided by the variance of the near-side peak in the 50-80% centrality bin.

Depletion yield calculated by taking the difference of the fit and the data, and normalized by the total yield of the peak.

Variance of the near-side jet peak from a generalized Gaussian fit.

Variance of the near-side jet peak from a generalized Gaussian fit.

Variance of near-side peak in the 0-10% centrality bin divided by the variance of the near-side peak in the 50-80% centrality bin.

Depletion yield calculated by taking the difference of the fit and the data, and normalized by the total yield of the peak.

Pb-Pb collision centrality 30-40%.

Pb-Pb collision centrality 40-50%.

Pb-Pb collision centrality 50-80%.

Pb-Pb collision centrality 0-10%.

Pb-Pb collision centrality 10-20%.

Pb-Pb collision centrality 20-30%.

Pb-Pb collision centrality 30-40%.

Pb-Pb collision centrality 40-50%.

Pb-Pb collision centrality 50-80%.

Three-particle correlation with respect to the 2nd order event plane from Pb-going side in pPb collisions as a function of multiplicity with individual track pT between 0.3 to 3.0 GeV/c.

Three-particle correlation with respect to the 2nd order event plane in PbPb collisions as a function of multiplicity with individual track pT between 0.3 to 3.0 GeV/c.

Three-particle correlation with respect to the 2nd order event plane in PbPb collisions as a function of centrality with individual track pT between 0.3 to 3.0 GeV/c, where the average multiplicity value is plotted on figure in order to compare with pPb collisions.

Three-particle correlation with respect to the 2nd order event plane from Pb-going side, p-going side in pPb collisions as a function of multiplicity with individual track pT between 0.3 to 3.0 GeV/c.

Three-particle correlation with respect to the 2nd order event plane in PbPb collisions as a function of multiplicity with individual track pT between 0.3 to 3.0 GeV/c.

Three-particle correlation with respect to the 2nd order event plane in PbPb collisions as a function of centrality with individual track pT between 0.3 to 3.0 GeV/c, where the average multiplicity value is plotted on figure in order to compare with pPb collisions.

Three-particle correlation with respect to the 2nd order event plane from Pb-going and p-going direction in pPb collisions and in PbPb collisions as a function DeltaEta for multiplicity [185,220) with individual track pT between 0.3 to 3.0 GeV/c. Data points are plotted at the bin center.

Prompt J/$\psi$ $v_{2}$ as a function of rapidity.

Prompt J/$\psi$ $v_{2}$ as a function of $p_{T}$.

Prompt J/$\psi$ $v_{2}$ as a function of $p_{T}$.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality at high $p_{\rm T}$, 6.5$<p_{\rm T}<$30 GeV/c, in three different $|y|$ regions.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality at high $p_{\rm T}$, 6.5$<p_{\rm T}<$30 GeV/c, in three different $|y|$ regions.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality, at forward rapidity, 1.6$<|y|<$2.4, for two different $p_{\rm T}$ regions.

Prompt J/$\psi$ $R_{\rm AA}$ as a function of centrality, at forward rapidity, 1.6$<|y|<$2.4, for two different $p_{\rm T}$ regions.

Nonprompt J/$\psi$ $v_{2}$ as a function of $p_{\rm T}$.

Nonprompt J/$\psi$ $v_{2}$ as a function of $p_{\rm T}$.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of rapidity.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of $p_{\rm T}$.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Nonprompt J/$\psi$ $R_{\rm AA}$ as a function of centrality. The average ${N}_{\rm part}$ values correspond to events flatly distributed across centrality.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Absolute cross section at particle level.

Covariance matrix of absolute cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Normalized cross section at particle level.

Covariance matrix of normalized cross section at particle level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Absolute cross section at parton level.

Covariance matrix of absolute cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Normalized cross section at parton level.

Covariance matrix of normalized cross section at parton level.

Observed 95% CL upper limits on $\mathcal{B}(H \rightarrow inv)$ assuming a Higgs boson with a mass of 125 GeV whose production cross sections are scaled, relative to their SM values as a function of the coupling modifiers $\kappa_{F}$ and $\kappa_{V}$.

Observed 95% CL upper limits on $\mathcal{B}(H \rightarrow inv)$ assuming a Higgs boson with a mass of 125 GeV whose production cross sections are scaled, relative to their SM values, by $\mu_{\mathrm{qqH,VH}}$ and $\mu_{\mathrm{ggH}}$.

Observed and expected 95% CL upper limit on $\mathcal{B}(H \rightarrow inv)$ assuming a Higgs boson with a mass of 125 GeV whose production cross sections are scaled, relative to their SM values as a function of $\kappa_{V}$, fixing $\kappa_{F}=1$..

Observed and expected 95% CL upper limit on $\mathcal{B}(H \rightarrow inv)$ assuming a Higgs boson with a mass of 125 GeV whose production cross sections are scaled, relative to their SM values as a function of $\kappa_{F}$, fixing $\kappa_{V}=1$..

Profile likelihood ratio as a function of $\mathcal{B}(H\rightarrow inv)$ assuming SM production cross sections of a Higgs boson with a mass of 125 GeV. The solid curves represent the observations in data and the dashed curves represent the expected result assuming no invisible decays of the Higgs boson. The observed and expected likelihood scans for the partial combinations of the qqH tagged, VH tagged, and ggH tagged analyses, and the full combination.

Profile likelihood ratio as a function of $\mathcal{B}(H\rightarrow inv)$ assuming SM production cross sections of a Higgs boson with a mass of 125 GeV. The solid curves represent the observations in data and the dashed curves represent the expected result assuming no invisible decays of the Higgs boson. The observed and expected likelihood scans for the partial combinations of the 7+8 and 13 TeV analyses, and the full combination.

A summary of benchmark simplified models, the most sensitive $n_{\mathrm{jet}}$ categories, and representative values for the corresponding experimental acceptance times efficiency ($\mathcal{A}\varepsilon$), the dominant systematic uncertainties, the theoretical production cross section ($\sigma_{\mathrm{theory}}$), and the expected and observed upper limits on the production cross section, expressed in terms of the signal strength parameter ($\mu$).

Summary of the mass limits obtained for the fourteen classes of simplified models. The limits indicate the strongest observed and expected (in parentheses) mass exclusions in $\tilde{g}$, $\tilde{q}$, $\tilde{b}$, $\tilde{t}$, and $\tilde{\chi}_1^0$. The quoted values have uncertainties of $\pm 25$ and $\pm 10$ GeV for models involving the pair production of, respectively, gluinos and squarks.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the observed exclusion.

Covariance matrix for the SM background estimates obtained using the simplified binning scheme, determined from a simultaneous fit to data in the control regions only (CR-only fit). The uncertainties in the background estimates are correlated in such a way that the covariance is typically positive. Small positive values, as well as the few negative values, are not shown.

Correlation matrix for the SM background estimates obtained using the simplified binning scheme, determined from a simultaneous fit to data in the control regions only (CR-only fit).

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the expected exclusion.

Observed data counts and "post-fit" background expectations based on the result of a combined fit to the signal region and multiple control regions under the SM-only hypothesis for the "monojet" event category. The rows labelled SM "pre-fit' show the background expectations when excluding the signal region from the fit. The uncertainties include statistical as well as systematic contributions.

Observed data counts and "post-fit" background expectations based on the result of a combined fit to the signal region and multiple control regions under the SM-only hypothesis for the "asymmetric" event categories. The rows labelled SM "pre-fit" show the background expectations when excluding the signal region from the fit. The uncertainties include statistical as well as systematic contributions.

Observed data counts and "post-fit" background expectations based on the result of a combined fit to the signal region and multiple control regions under the SM-only hypothesis for the "symmetric" event categories. The rows labelled SM "pre-fit" show the background expectations when excluding the signal region from the fit. The uncertainties include statistical as well as systematic contributions.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the observed exclusion.

Summary of a simplified binning scheme comprising $H_{\mathrm{T}}^{\mathrm{miss}}$ shapes for eight representative event topologies, defined in terms of requirements on $n_{\mathrm{jet}}$ both symmetric and asymmetric categories) and $n_{\mathrm{b}}$. For each topology, event yields are integrated over the full $H_{\mathrm{T}}$ range, $H_{\mathrm{T}} > 200$ GeV, and are categorised according to eight bins in $H_{\mathrm{T}}^{\mathrm{miss}}$ -- $130 < H_{\mathrm{T}}^{\mathrm{miss}} < 200$ GeV, six bins 100 GeV wide in the region $200 < H_{\mathrm{T}}^{\mathrm{miss}} < 800$ GeV, and an open final bin, $H_{\mathrm{T}}^{\mathrm{miss}} > 800$ GeV. This categorisation scheme leads to 64 bins that are exclusive, contiguous, and provide complete coverage of the signal region. The corresponding SM background estimates for these 64 bins are obtained using the nominal likelihood model. The $H_{\mathrm{T}}^{\mathrm{miss}}$ template for each topology is determined from simulation and the normalisation for each template is given by an aggregate of estimates from several ($n_{\mathrm{jet}}$, $n_{\mathrm{b}}$, $H_{\mathrm{T}}$) bins, defined according to the nominal binning scheme.

Observed data yields and "CR-only fit" SM background expectations using the simplified binning scheme, as a function of topology and $H_{\mathrm{T}}^{\mathrm{miss}}$. The SM backgrounds are determined from a simultaneous fit to data in the control regions. The data yields in the signal region are masked and excluded from the fit. The uncertainties include statistical as well as systematic contributions.

Expected ($\mu_{\mathrm{exp}}$) and observed ($\mu_{\mathrm{obs}}$) upper limits on the production cross section, expressed in terms of the signal strength parameter, obtained using both the nominal and simplified binning schema. Comparable values are obtained from the two schema for these benchmark SUSY models because the signal events typically populate bins at high values of $H_{\mathrm{T}}$ and $H_{\mathrm{T}}^{\mathrm{miss}}$ and so are at or near the limit of the search sensitivity. Larger differences in $\mu$ can be observed for models that populate the core of these distributions.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1tttt model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1tttt model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1ttbb model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1ttbb model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5tttt_DM175 model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1qqqq model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5tttt_DM175 model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{q} } }, m_{\tilde{\chi}^0_1 })$ plane for the T2qq model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5ttcc model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1bbbb model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5ttcc model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1tttt model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1tttt model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1tttt model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ b } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bb model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1tttt model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1ttbb model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1ttbb model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ b } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bb model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1ttbb model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T1ttbb model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5tttt_DM175 model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tb model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5tttt_DM175 model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5tttt_DM175 model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5tttt_DM175 model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tb model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5ttcc model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5ttcc model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5ttcc model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{g} } }, m_{\tilde{\chi}^0_1 })$ plane for the T5ttcc model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ b } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bb model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ b } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bb model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ b } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bb model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ b } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bb model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tb model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2cc model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tb model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tb model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tb model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2cc model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt_degen model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2cc model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2cc model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt_degen model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2cc model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2cc model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt_degen model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2_mixed model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt_degen model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt_degen model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2tt_degen model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2_mixed model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2_mixed model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2_mixed model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2_mixed model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bW model. This line is the expected exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2_mixed model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bW model. This line is the $+1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bW model. This line is the $-1\sigma $ expected exclusion due to experimental uncertainties.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bW model. This line is the observed exclusion.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bW model. This line is the $+1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.

Upper limit on the cross section in the $(m_{ \tilde{ \mathrm{ t } } }, m_{\tilde{\chi}^0_1 })$ plane for the T2bW model. This line is the $-1\sigma $ observed exclusion due to theoretical uncertainties on the signal cross section.