Data from FigAux 4 and FigAux 8a-16a. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for beta = 0, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.

Data from FigAux 4 and FigAux 8b-16b. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 1, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.

Data from FigAux 8c-16c. The unfolded $log_{10}(\rho^2)$ distribution for anti-kt R=0.8 jets with $p_T$(lead) > 600 GeV, after the soft drop algorithm is applied for $\beta$ = 2, in data. All uncertainties described in the text are shown on the data; the uncertainties from the calculations are shown on each one. The distributions are normalized to the integrated cross section, sigma(resum), measured in the resummation region, $-3.7 < log_{10}(\rho^2) < -1.7$. Each set of 10 bins corresponds to one $p_T$ bin in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ } and 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.

Data from FigAux 6a. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 0. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.

Data from FigAux 6b. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 1. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.

Data from FigAux 6c. The summed covariance matrices of the systematic and statistical uncertainties for the combined $p_T$ and $log_{10}(\rho^2)$ bins for $\beta$ = 2. Each group of 10 bins corresponds to a bin of $p_T$ in {600, 650, 700, 750, 800, 850, 900, 950, 1000, ∞ }; each bin within the $p_T$ bin corresponds to 10 evenly spaced bins in $log_{10}(\rho^2)$ from -4.5 to -0.5.

Data from FigAux 7a. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 0, inclusive in $p_T$.

Data from FigAux 7b. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 1, inclusive in $p_T$.

Data from FigAux 7c. The summed covariance matrices of the systematic and statistical uncertainties for the $log_{10}(\rho^2)$ bins for $\beta$ = 2, inclusive in $p_T$.

$\textbf{Distribution 4 } -$ Kinematic distribution of ETmiss in bCbv. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Distribution 5 } -$ Kinematic distribution of mT in DM_low. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Distribution 6 } -$ Kinematic distribution of ETmiss in DM_high. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Distribution 7 } -$ Distributions of BDT score for the tN_diag_low region. The SM background predictions are obtained using the background-only fit configuration.

$\textbf{Distribution 8 } -$ Distributions of BDT score for the tN_diag_med region. The SM background predictions are obtained using the background-only fit configuration.

$\textbf{Distribution 9 } -$ Distributions of BDT score for the tN_diag_high region. The SM background predictions are obtained using the background-only fit configuration.

$\textbf{Distribution 10 } -$ Kinematic distribution of ETmiss in tN_med. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Distribution 11 } -$ Kinematic distribution of amT2 in bWN. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Distribution 12 } -$ Kinematic distribution of pT(l)/ETmiss in bffN. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Distribution 13 } -$ Kinematic distribution of pT(l)/ETmiss in bCsoft_diag. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Distribution 14 } -$ Kinematic distribution of pT(l)/ETmiss in bCsoft_med. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Distribution 15 } -$ Kinematic distribution of pT(l)/ETmiss in bCsoft_high. The full event selection in the corresponding signal region is applied, except for the requirement that is imposed on the variable being plotted. The predicted SM backgrounds are scaled with the normalisation factors obtained from the corresponding control regions. The last bin contains overflows.

$\textbf{Exclusion contour 1 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for the direct stop pair production assuming either stop -> t N1, stop -> b W C1 or stop -> b f f' N1 decay with a branching ratio of 100%.

$\textbf{Exclusion contour 1 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for the direct stop pair production assuming either stop -> t N1, stop -> b W C1 or stop -> b f f' N1 decay with a branching ratio of 100%.

$\textbf{Selected SR 1 } -$ Selected signal regions for the bino LSP model in the m(STOP) vs m(NEUTRALINO) plane.

$\textbf{Exclusion contour 2 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(STOP)-m(NEUTRALINO) for the direct stop pair production assuming either stop -> t N1, stop -> b W C1 or stop -> b f f' N1 decay with a branching ratio of 100%.

$\textbf{Exclusion contour 2 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(STOP)-m(NEUTRALINO) for the direct stop pair production assuming either stop -> t N1, stop -> b W C1 or stop -> b f f' N1 decay with a branching ratio of 100%.

$\textbf{Selected SR 2 } -$ Selected signal regions for the bino LSP model in the m(STOP) versus m(STOP)-m(NEUTRALINO) plane.

$\textbf{Exclusion contour 3 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for the direct stop/sbottom pair production in the wino NLSP model under the hypothesis of mq3L < mtR and mu < 0, where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, sbottom -> t C1, sbottom -> b N1, and sbottom -> b N2) are considered with different branching ratios for each signal point. N2 decays to N1 predominantly via either Z boson or Higgs boson depending on the sign of the μ parameter.

$\textbf{Exclusion contour 3 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for the direct stop/sbottom pair production in the wino NLSP model under the hypothesis of mq3L < mtR and mu < 0, where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, sbottom -> t C1, sbottom -> b N1, and sbottom -> b N2) are considered with different branching ratios for each signal point. N2 decays to N1 predominantly via either Z boson or Higgs boson depending on the sign of the μ parameter.

$\textbf{Selected SR 3 } -$ Selected signal regions in the plane of m(STOP) versus m(NEUTRALINO) for the direct stop/sbottom pair production in the wino NLSP model under the hypothesis of mq3L < mtR and mu < 0, where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, sbottom -> t C1, sbottom -> b N1, and sbottom -> b N2) are considered with different branching ratios for each signal point. N2 decays to N1 predominantly via either Z boson or Higgs boson depending on the sign of the μ parameter.

$\textbf{Exclusion contour 4 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for the direct stop/sbottom pair production in the wino NLSP model under the hypothesis of mq3L < mtR and mu > 0, where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, sbottom -> t C1, sbottom -> b N1, and sbottom -> b N2) are considered with different branching ratios for each signal point. N2 decays to N1 predominantly via either Z boson or Higgs boson depending on the sign of the μ parameter.

$\textbf{Exclusion contour 4 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for the direct stop/sbottom pair production in the wino NLSP model under the hypothesis of mq3L < mtR and mu > 0, where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, sbottom -> t C1, sbottom -> b N1, and sbottom -> b N2) are considered with different branching ratios for each signal point. N2 decays to N1 predominantly via either Z boson or Higgs boson depending on the sign of the μ parameter.

$\textbf{Selected SR 4 } -$ Selected signal regions in the plane of m(STOP) versus m(NEUTRALINO) for the direct stop/sbottom pair production in the wino NLSP model under the hypothesis of mq3L < mtR and mu > 0, where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, sbottom -> t C1, sbottom -> b N1, and sbottom -> b N2) are considered with different branching ratios for each signal point. N2 decays to N1 predominantly via either Z boson or Higgs boson depending on the sign of the μ parameter.

$\textbf{Exclusion contour 5 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production assuming b C1 decay with a branching ratio of 100%. The chargino mass is assumed to be close to the stop mass, m(C1) = m(STOP) - 10 GeV.

$\textbf{Exclusion contour 5 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production assuming b C1 decay with a branching ratio of 100%. The chargino mass is assumed to be close to the stop mass, m(C1) = m(STOP) - 10 GeV.

$\textbf{Exclusion contour 6 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly left-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 6 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly left-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Selected SR 6 } -$ Selected signal regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly left-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 7 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly right-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 7 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly right-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Selected SR 7 } -$ Selected signal regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly right-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 8 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for large $\tan\beta$. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 8 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for large $\tan\beta$. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Selected SR 8 } -$ Selected signal regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for large $\tan\beta$. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 9 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2) are considered with different branching ratios depending on the hypothesis being considered. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 9 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2) are considered with different branching ratios depending on the hypothesis being considered. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 10 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly left-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 10 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly left-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Selected SR 10 } -$ Selected signal regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly left-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 11 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly right-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 11 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly right-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Selected SR 11 } -$ Selected signal regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for a mostly right-handed stop. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 12 (exp.) } -$ Expected 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for large $\tan\beta$. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 12 (obs.) } -$ Observed 95% excluded regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for large $\tan\beta$. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Selected SR 12 } -$ Selected signal regions in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model for large $\tan\beta$. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{Exclusion contour 13 (exp.) } -$ Expected 95% excluded regions in the plane of mm(STOP) versus m(NEUTRALINO) or the direct stop/sbottom pair production in the well-tempered neutralino model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, b1 -> t C1, b1 -> b N1, and b1 -> b N2) are considered with different branching ratio for each signal point for the $m_{q_{3L}} < m_{t_{R}}$ hypothesis. Both stop/sbottom pair productions are considered.

$\textbf{Exclusion contour 13 (obs.) } -$ Observed 95% excluded regions in the plane of mm(STOP) versus m(NEUTRALINO) or the direct stop/sbottom pair production in the well-tempered neutralino model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, b1 -> t C1, b1 -> b N1, and b1 -> b N2) are considered with different branching ratio for each signal point for the $m_{q_{3L}} < m_{t_{R}}$ hypothesis. Both stop/sbottom pair productions are considered.

$\textbf{Selected SR 13 } -$ Selected signal regions in the plane of mm(STOP) versus m(NEUTRALINO) or the direct stop/sbottom pair production in the well-tempered neutralino model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, b1 -> t C1, b1 -> b N1, and b1 -> b N2) are considered with different branching ratio for each signal point for the $m_{q_{3L}} < m_{t_{R}}$ hypothesis. Both stop/sbottom pair productions are considered.

$\textbf{Exclusion contour 14 (exp.) } -$ Expected 95% excluded regions in the plane of mm(STOP) versus m(NEUTRALINO) or the direct stop/sbottom pair production in the well-tempered neutralino model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, b1 -> t C1, b1 -> b N1, and b1 -> b N2) are considered with different branching ratio for each signal point for the $m_{q_{3L}} > m_{t_{R}}$. Only stop pair production is considered.

$\textbf{Exclusion contour 14 (obs.) } -$ Observed 95% excluded regions in the plane of mm(STOP) versus m(NEUTRALINO) or the direct stop/sbottom pair production in the well-tempered neutralino model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, b1 -> t C1, b1 -> b N1, and b1 -> b N2) are considered with different branching ratio for each signal point for the $m_{q_{3L}} > m_{t_{R}}$. Only stop pair production is considered.<br><b>Note:</b> As no observed exclusion is found for this model, the contour is empty.

$\textbf{Selected SR 14 } -$ Selected signal regions in the plane of mm(STOP) versus m(NEUTRALINO) or the direct stop/sbottom pair production in the well-tempered neutralino model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2, b1 -> t C1, b1 -> b N1, and b1 -> b N2) are considered with different branching ratio for each signal point for the $m_{q_{3L}} > m_{t_{R}}$. Only stop pair production is considered.

$\textbf{DM Upper Limit 1 } -$ Upper limit on the ratio of the DM production cross-section to the simplified model expectation under the hypothesis of a scalar mediator. The limit is shown as a function of the mediator mass for a fixed mass of the DM candidate of 1 GeV. The coupling of the mediator to SM and DM particles is assumed to be g=1.

$\textbf{DM Upper Limit 2 } -$ Upper limit on the ratio of the DM production cross-section to the simplified model expectation under the hypothesis of a pseudoscalar mediator. The limit is shown as a function of the mediator mass for a fixed mass of the DM candidate of 1 GeV. The coupling of the mediator to SM and DM particles is assumed to be g=1.

$\textbf{DM Upper Limit 3 } -$ Upper limit on the ratio of the DM production cross-section to the simplified model expectation under the hypothesis of a scalar mediator. The limit is shown as a function of the DM candidate mass for a fixed mediator mass of 10 GeV. The coupling of the mediator to SM and DM particles is assumed to be g=1.

$\textbf{DM Upper Limit 4 } -$ Upper limit on the ratio of the DM production cross-section to the simplified model expectation under the hypothesis a pseudoscalar mediator. The limit is shown as a function of the DM candidate mass for a fixed mediator mass of 10 GeV. The coupling of the mediator to SM and DM particles is assumed to be g=1.

$\textbf{X-section U.L. 1 } -$ Observed upper limit on the signal cross section for the bino LSP model in the m(STOP) vs m(NEUTRALINO) plane.

$\textbf{X-section U.L. 2 } -$ Observed upper limit on the signal cross section for the bino LSP model in the m(STOP) vs m(STOP)-m(NEUTRALINO) plane.

$\textbf{X-section U.L. 3 } -$ Observed upper limit on the signal cross section for the wino NLSP model with mu < 0

$\textbf{X-section U.L. 4 } -$ Observed upper limit on the signal cross section for the wino NLSP model with mu > 0

$\textbf{X-section U.L. 5 } -$ Observed upper limit on the signal cross section for the higgsino LSP model with left-handed stop squarks.

$\textbf{X-section U.L. 6 } -$ Observed upper limit on the signal cross section for the higgsino LSP model with right-handed stop squarks.

$\textbf{X-section U.L. 7 } -$ Observed upper limit on the signal cross section for the higgsino LSP model with large tan beta.

$\textbf{X-section U.L. 8 } -$ Observed upper limit on the signal cross section for the variable m(CHARGINO) - m(NEUTRALINO) higgsino LSP model with left-handed stop squarks.

$\textbf{X-section U.L. 9 } -$ Observed upper limit on the signal cross section for the variable m(CHARGINO) - m(NEUTRALINO) higgsino LSP model with right-handed stop squarks.

$\textbf{X-section U.L. 10 } -$ Observed upper limit on the signal cross section for the variable m(CHARGINO) - m(NEUTRALINO) higgsino LSP model with large tan beta.

$\textbf{X-section U.L. 11 } -$ Observed upper limit on the signal cross section for the simplified model with m(STOP) - m(CHARGINO) = 10 GeV.

$\textbf{X-section U.L. 12 } -$ Observed 95% upper cross-section limit in the plane of m(STOP) versus m(NEUTRALINO) for direct stop pair production in the higgsino LSP model where various decay modes (stop -> b C1, stop -> t N1, stop -> t N2) are considered with different branching ratios depending on the hypothesis being considered. In this model, dm(C1,N1) =5 GeV and dm(N2,N1)=10 GeV are assumed.

$\textbf{X-section U.L. 13 } -$ Observed upper limit on the signal cross section for the well-tempered neutralino model with left-handed stop squarks.

$\textbf{X-section U.L. 14 } -$ Observed upper limit on the signal cross section for the well-tempered neutralino model with right-handed stop squarks.

$\textbf{Cutflow 1 } -$ Cutflow for tN_med for the pure bino LSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{0}_{1} )$ = (600, 300) GeV. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV. Numbers are provided for the discovery SR, even if a shape fit is used for placing exclusion limits.

$\textbf{Cutflow 2 } -$ Cutflow for tN_high for the pure bino LSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{0}_{1} )$ = (1000, 1) GeV. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV.

$\textbf{Cutflow 3 } -$ Cutflow for bWN for the pure bino LSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{0}_{1} )$ = (350, 230) GeV in bWN. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV. Numbers are provided for the discovery SR, even if a shape fit is used for placing exclusion limits.

$\textbf{Cutflow 4 } -$ Cutflow for bffN for the pure bino LSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{0}_{1} )$ = (350, 300) GeV. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV. Numbers are provided for the discovery SR, even if a shape fit is used for placing exclusion limits.

$\textbf{Cutflow 5 } -$ Cutflow for bC2x_diag for the wino NLSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{\pm}_{1} , \tilde{\chi}^{0}_{1} )$ = (737, 500, 250) GeV. Only stop pair production is considered in the cutflow. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV.

$\textbf{Cutflow 6 } -$ Cutflow for bC2x_med for the wino NLSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{\pm}_{1} , \tilde{\chi}^{0}_{1} )$ = (842, 300, 150) GeV. Only stop pair production is considered in the cutflow. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV.

$\textbf{Cutflow 7 } -$ Cutflow for the simplified signal model with $\Delta m( \tilde{\chi}^{\pm}_{1} , \tilde{\chi}^{0}_{1} )$ = 10 GeV, considering $m(\tilde{t}_{1} , \tilde{\chi}^{\pm}_{1} , \tilde{\chi}^{0}_{1} )$ = (700, 690, 1). The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV.

$\textbf{Cutflow 8 } -$ Cutflow for bCsoft_diag for the higgsino LSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{\pm}_{1} , \tilde{\chi}^{0}_{1} )$ = (400, 355, 350) GeV, assuming $\tilde{t}_{1} \sim \tilde{t}_{\mathrm{L}}$ and large $\tan\beta$. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV. Numbers are provided for the discovery SR, even if a shape fit is used for placing exclusion limits.

$\textbf{Cutflow 9 } -$ Cutflow for bCsoft_med for the higgsino LSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{\pm}_{1} , \tilde{\chi}^{0}_{1} )$ = (600, 205, 200) GeV, assuming $\tilde{t}_{1} \sim \tilde{t}_{\mathrm{L}}$ and large $\tan\beta$. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV. Numbers are provided for the discovery SR, even if a shape fit is used for placing exclusion limits.

$\textbf{Cutflow 10 } -$ Cutflow for bCsoft_high for the higgsino LSP signal model with $m(\tilde{t}_{1} , \tilde{\chi}^{\pm}_{1} , \tilde{\chi}^{0}_{1} )$ = (800, 155, 150) GeV, assuming $\tilde{t}_{1} \sim \tilde{t}_{\mathrm{L}}$ and large $\tan\beta$. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV. Numbers are provided for the discovery SR, even if a shape fit is used for placing exclusion limits.

$\textbf{Cutflow 11 } -$ Cutflow for DM_high for the spin-0 mediator model with $m(\phi, \chi)$ = (300, 1) GeV, assuming g=1 and a scalar mediator. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV.

$\textbf{Cutflow 12 } -$ Cutflow for DM_low for the spin-0 mediator model with $m(\phi, \chi)$ = (20, 1) GeV, assuming g=1 and a scalar mediator. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV.

$\textbf{Cutflow 13 } -$ Cutflow for DM_low_loose for the spin-0 mediator model with $m(\phi, \chi)$ = (20, 1) GeV, assuming g=1 and a scalar mediator. The DxAOD skimming step requires at least one of the following criteria to be fullfilled: one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ triggers has fired and there is at least one loose muon (electron) with $p_{\mathrm{T}}$ > 3.5 (4.5) GeV; or one of the $E_{\mathrm{T}}^{\mathrm{miss}}$ or lepton triggers has fired and there is at least one loose lepton with $p_{\mathrm{T}}$ > 25 GeV.

$\textbf{Acceptance 1 } -$ Acceptance and efficiency for the bino LSP model in the $m_{\tilde{t}_{1}}$ vs $m_{\tilde{\chi}^{0}_{1}}$ plane. Efficiencies larger than 100% are observed in the bWN SR due differences in $am_{\mathrm{T2}}$ between truth and reconstruction level, in the absence of $b$-tagging inefficiencies. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Efficiency 1 } -$ Acceptance and efficiency for the bino LSP model in the $m_{\tilde{t}_{1}}$ vs $m_{\tilde{\chi}^{0}_{1}}$ plane. Efficiencies larger than 100% are observed in the bWN SR due differences in $am_{\mathrm{T2}}$ between truth and reconstruction level, in the absence of $b$-tagging inefficiencies. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Acceptance 2 } -$ Acceptance and efficiency for the bino LSP model in the $m_{\tilde{t}_{1}}$ vs $\Delta m(\tilde{t}_{1},\tilde{\chi}^{0}_{1})$ plane. Efficiencies larger than 100% are observed in the bWN SR due differences in $am_{\mathrm{T2}}$ between truth and reconstruction level, in the absence of $b$-tagging inefficiencies. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Efficiency 2 } -$ Acceptance and efficiency for the bino LSP model in the $m_{\tilde{t}_{1}}$ vs $\Delta m(\tilde{t}_{1},\tilde{\chi}^{0}_{1})$ plane. Efficiencies larger than 100% are observed in the bWN SR due differences in $am_{\mathrm{T2}}$ between truth and reconstruction level, in the absence of $b$-tagging inefficiencies. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Acceptance 3 } -$ Acceptance and efficiency for the wino NLSP model with $\mu > 0$.

$\textbf{Efficiency 3 } -$ Acceptance and efficiency for the wino NLSP model with $\mu > 0$.

$\textbf{Acceptance 4 } -$ Acceptance and efficiency for the higgsino LSP model with $\Delta m (\tilde{\chi}^{\pm}_{1}, \tilde{\chi}^{0}_{1}) = 5$ GeV. The model assumes large $\tan\beta$ and the $\tilde{t}_{1}$ to be mostly $\tilde{t}_{L}$. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Efficiency 4 } -$ Acceptance and efficiency for the higgsino LSP model with $\Delta m (\tilde{\chi}^{\pm}_{1}, \tilde{\chi}^{0}_{1}) = 5$ GeV. The model assumes large $\tan\beta$ and the $\tilde{t}_{1}$ to be mostly $\tilde{t}_{L}$. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Acceptance 5 } -$ Acceptance and efficiency for the higgsino LSP model with $\Delta m (\tilde{\chi}^{\pm}_{1}, \tilde{\chi}^{0}_{1}) = 5$ GeV, in the region where $\Delta m (\tilde{\chi}^{\pm}_{1}, \tilde{\chi}^{0}_{1}) < m_{\textrm{top}}$. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Efficiency 5 } -$ Acceptance and efficiency for the higgsino LSP model with $\Delta m (\tilde{\chi}^{\pm}_{1}, \tilde{\chi}^{0}_{1}) = 5$ GeV, in the region where $\Delta m (\tilde{\chi}^{\pm}_{1}, \tilde{\chi}^{0}_{1}) < m_{\textrm{top}}$. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Acceptance 6 } -$ Acceptance and efficiency for the simplified model with $\Delta m (\tilde{\chi}^{\pm}_{1}, \tilde{\chi}^{\pm}_{1}) = 10$ GeV.

$\textbf{Efficiency 6 } -$ Acceptance and efficiency for the simplified model with $\Delta m (\tilde{\chi}^{\pm}_{1}, \tilde{\chi}^{\pm}_{1}) = 10$ GeV.

$\textbf{Acceptance 7 } -$ Acceptance and efficiency for the spin-0 mediator model, assuming a scalar mediator. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

$\textbf{Efficiency 7 } -$ Acceptance and efficiency for the spin-0 mediator model, assuming a scalar mediator. Acceptance and efficiency numbers are provided for discovery SRs even if shape fits are used for placing exclusion limits.

Absolute cross-sections differential in m(l2b). Uncertainties are signed to show correlations.

Absolute cross-sections differential in E(llb). Uncertainties are signed to show correlations.

Absolute cross-sections differential in mT(llvvb). Uncertainties are signed to show correlations.

Absolute cross-sections differential in m(llb). Uncertainties are signed to show correlations.

Normalised cross-sections differential in E(b). Uncertainties are signed to show correlations.

Normalised cross-sections differential in m(l1b). Uncertainties are signed to show correlations.

Normalised cross-sections differential in m(l2b). Uncertainties are signed to show correlations.

Normalised cross-sections differential in E(llb). Uncertainties are signed to show correlations.

Normalised cross-sections differential in mT(llvvb). Uncertainties are signed to show correlations.

Normalised cross-sections differential in m(llb). Uncertainties are signed to show correlations.

The observed values of Sigma*BR(H->ZZ*), the SM expected cross section sBRsm and their ratio Sigma*BR/(Sigma*BR)_SM for the inclusive production and in each Stage-0 and reduced Stage-1 production bin for an integrated luminosity of 36.1/fb and at sqrt(s)=13 TeV. The bbH contribution is considered as a part of the ggF production bins. The upper limits correspond to the 95% CL obtained with pseudo-experiments using the CL_s method. The uncertainties are given as (stat.)+(exp.)+(th.) for Stage 0 and as (stat.)+(syst.) for reduced Stage 1. Values without uncertainity are 95% CL upper limits.

Signal acceptance obtained as the ratio of the number of simulated signal events satisfying the event selection criteria in each reconstructed event category over the total number of events generated in the phase space specified by a given reduced Stage-1 ggF production bin. Results are obtained in bins of BDT discriminants using coarse binning with several bins merged into one. Values less than 0.0001 are set to 0.

Signal acceptance obtained as the ratio of the number of simulated signal events satisfying the event selection criteria in each reconstructed event category over the total number of events generated in the phase space specified by the given reduced Stage-1 VBF and VH production bins. Results are obtained in bins of BDT discriminants using coarse binning with several bins merged into one. Values less than 0.0001 are set to 0.

The signal strengths mu for the inclusive production and in each Stage-0 and reduced Stage-1 production bin for an integrated luminosity of 36.1/fb and at sqrt(s)=13 TeV. The bbH contribution is considered as a part of the ggF production bins. The upper limits correspond to the 95% CL obtained with pseudo-experiments using the CL_s method. The uncertainties are given as (stat.)+(exp.)+(th.) for Stage 0 and as (stat.)+(syst.) for reduced Stage 1. Values without uncertainity are 95% CL upper limits.

Signal acceptance (in percent) obtained as the ratio of the number of simulated signal events satisfying the event selection criteria in each reconstructed event category to the total number of generated events, as predicted by the MadGraph5_aMC@NLO generator assuming the SM coupling tensor structure or the BSM tensor structure with ($\kappa_{SM}$ = 1, | $\kappa_{AVV}$ | $\neq$ 0).

Number of expected ggF Higgs boson events for an integrated luminosity of $\mathcal L=36.1 \text{fb}^{-1}$ and at $\sqrt{\mathrm{s}}=13$ TeV, as predicted by the MadGraph5_aMC@NLO generator assuming the SM coupling tensor structure or the BSM tensor structure with ($\kappa_{SM}=1$, $|\kappa_{Avv}|=6$). The highest-order SM predicition for the sum of the ggF, ttH and bbH contributions is also shown for comparison.

Number of expected VBF and VH Higgs boson events for an integrated luminosity of $\mathcal L=36.1 \text{fb}^{-1}$ and at $\sqrt{\mathrm{s}}=13$ TeV, as predicted by the MadGraph5_aMC@NLO generator assuming the SM coupling tensor structure or the BSM tensor structure with ($\kappa_{SM}=1$, $|\kappa_{Avv}|=5$). The highest-order SM predicition for the sum of the VBF and VH contributions is also shown for comparison.

Expected Correlation Matrix for Stage 0

Observed Correlation Matrix for Stage 0. As upper limits are derived for ttH and VH POIs using the observed data, the corresponding terms inside the matrix are set to zero.

Expected Correlation Matrix for Reduced Stage 1

Observed Correlation Matrix for Reduced Stage 1. As upper limits are derived for ttH and VH POIs using the observed data, the corresponding terms inside the matrix are set to zero.

Expected Covariance Matrix for Stage 0

Observed Covariance Matrix for Stage 0. As upper limits are derived for ttH and VH POIs using the observed data, the corresponding terms inside the matrix are set to zero.

Expected Covariance Matrix for Reduced Stage 1

Observed Covariance Matrix for Reduced Stage 1. As upper limits are derived for ttH and VH POIs using the observed data, the corresponding terms inside the matrix are set to zero.

Likelihood contours at 68% CL in the (Sigma_ggF*B , Sigma_VBF*B ) plane

Likelihood contours at 95% CL in the (Sigma_ggF*B , Sigma_VBF*B ) plane

Expected two-dimensional negative log-likelihood scans for $\kappa_{HVV}$ versus $\kappa_{AVV}$ coupling parameters using $\mathcal L=36.1 \text{fb}^{-1}$ of data and at $\sqrt{\mathrm{s}}=13$ TeV. The couplings $\kappa_{Hgg}$ and $\kappa_{SM}$ are fixed to the SM value of one in the fit. The 95% CL exclusion limits are shown.

Observed two-dimensional negative log-likelihood scans for $\kappa_{HVV}$ versus $\kappa_{AVV}$ coupling parameters using $\mathcal L=36.1 \text{fb}^{-1}$ of data and at $\sqrt{\mathrm{s}}=13$ TeV. The couplings $\kappa_{Hgg}$ and $\kappa_{SM}$ are fixed to the SM value of one in the fit. The 95% CL exclusion limits are shown.

Expected two-dimensional negative log-likelihood scans for $\kappa_{HVV}$ versus $\kappa_{AVV}$ coupling parameters using $\mathcal L=36.1 \text{fb}^{-1}$ of data and at $\sqrt{\mathrm{s}}=13$ TeV. The coupling $\kappa_{Hgg}$ is fixed to the SM value of one in the fit. The coupling $\kappa_{SM}$ is left as a free parameter of the fit. The 95% CL exclusion limits are shown.

Observed two-dimensional negative log-likelihood scans for $\kappa_{HVV}$ versus $\kappa_{AVV}$ coupling parameters using $\mathcal L=36.1 \text{fb}^{-1}$ of data and at $\sqrt{\mathrm{s}}=13$ TeV. The coupling $\kappa_{Hgg}$ is fixed to the SM value of one in the fit. The coupling $\kappa_{SM}$ is left as a free parameter of the fit. The 95% CL exclusion limits are shown.

Expected two-dimensional negative log-likelihood scans for $\kappa_{HVV}$ versus $\kappa_{SM}$ coupling parameters using $\mathcal L=36.1 \text{fb}^{-1}$ of data and at $\sqrt{\mathrm{s}}=13$ TeV. The 95% CL exclusion limits are shown.

Observed two-dimensional negative log-likelihood scans for $\kappa_{HVV}$ versus $\kappa_{SM}$ coupling parameters using $\mathcal L=36.1 \text{fb}^{-1}$ of data and at $\sqrt{\mathrm{s}}=13$ TeV. The 95% CL exclusion limits are shown.

Expected two-dimensional negative log-likelihood scans for $\kappa_{AVV}$ versus $\kappa_{SM}$ coupling parameters using $\mathcal L=36.1 \text{fb}^{-1}$ of data and at $\sqrt{\mathrm{s}}=13$ TeV. The 95% CL exclusion limits are shown.

Observed two-dimensional negative log-likelihood scans for $\kappa_{AVV}$ versus $\kappa_{SM}$ coupling parameters using $\mathcal L=36.1 \text{fb}^{-1}$ of data and at $\sqrt{\mathrm{s}}=13$ TeV. The 95% CL exclusion limits are shown.

Observed and expected background and signal effective mass distributions for SR4j-2200. For signal, a gluino direct decay model where gluinos have mass of 1800 GeV and the neutralino1 has mass of 800 GeV is shown.

Observed and expected background and signal effective mass distributions for SR6j-2600. For signal, a gluino onestep decay model where gluinos have mass of 1705 GeV, the chargino1 has mass of 865 GeV and the neutralino1 has mass of 25 GeV is shown.

Observed and expected background and signal effective mass distributions for SR2jB-2400. For signal, a gluino onestep decay model where gluinos have mass of 1600 GeV, the chargino1 has mass of 1590 GeV and the neutralino1 has mass of 60 GeV is shown.

Observed and expected background and signal effective mass distributions for SR2j-1200. For signal, a squark direct decay model where squarks have mass of 900 GeV and the neutralino1 has mass of 500 GeV is shown.

Observed and expected background and signal effective mass distributions for SR2j-1600. For signal, a squark direct decay model where squarks have mass of 1200 GeV and the neutralino1 has mass of 500 GeV is shown.

Observed and expected background and signal effective mass distributions for SR2j-2000. For signal, a squark direct decay model where squarks have mass of 1200 GeV and the neutralino1 has mass of 0 GeV is shown.

Observed and expected background and signal effective mass distributions for SR2j-2400. For signal, a squark direct decay model where squarks have mass of 1500 GeV and the neutralino1 has mass of 0 GeV is shown.

Observed and expected background and signal effective mass distributions for SR2j-3600. For signal, a squark direct decay model where squarks have mass of 1200 GeV and the neutralino1 has mass of 0 GeV is shown.

Observed and expected background and signal effective mass distributions for SR2jB-1600. For signal, a gluino onestep decay model where gluinos have mass of 1600 GeV, the chargino1 has mass of 1590 GeV and the neutralino1 has mass of 60 GeV is shown.

Observed and expected background and signal effective mass distributions for SR3j-1300. For signal, a squark direct decay model where squarks have mass of 600 GeV and the neutralino1 has mass of 595 GeV is shown.

Observed and expected background and signal effective mass distributions for SR4j-1400. For signal, a gluino direct decay model where gluinos have mass of 1800 GeV and the neutralino1 has mass of 0 GeV is shown.

Observed and expected background and signal effective mass distributions for SR4j-1800. For signal, a gluino direct decay model where gluinos have mass of 1800 GeV and the neutralino1 has mass of 0 GeV is shown.

Observed and expected background and signal effective mass distributions for SR4j-2600. For signal, a gluino direct decay model where gluinos have mass of 1800 GeV and the neutralino1 has mass of 0 GeV is shown.

Observed and expected background and signal effective mass distributions for SR4j-3000. For signal, a gluino direct decay model where gluinos have mass of 1800 GeV and the neutralino1 has mass of 0 GeV is shown.

Observed and expected background and signal effective mass distributions for SR5j-1600. For signal, a gluino onestep decay model where gluinos have mass of 1705 GeV, the chargino1 has mass of 865 GeV and the neutralino1 has mass of 25 GeV is shown.

Observed and expected background and signal effective mass distributions for SR5j-1700. For signal, a gluino direct decay model where gluinos have mass of 1800 GeV and the neutralino1 has mass of 0 GeV is shown.

Observed and expected background and signal effective mass distributions for SR5j-2000. For signal, a gluino onestep decay model where gluinos have mass of 1705 GeV, the chargino1 has mass of 865 GeV and the neutralino1 has mass of 25 GeV is shown.

Observed and expected background and signal effective mass distributions for SR5j-2600. For signal, a gluino onestep decay model where gluinos have mass of 1705 GeV, the chargino1 has mass of 865 GeV and the neutralino1 has mass of 25 GeV is shown.

Observed and expected background and signal effective mass distributions for SR6j-1200. For signal, a gluino onestep decay model where gluinos have mass of 1705 GeV, the chargino1 has mass of 865 GeV and the neutralino1 has mass of 25 GeV is shown.

Observed and expected background and signal effective mass distributions for SR6j-1800. For signal, a gluino onestep decay model where gluinos have mass of 1705 GeV, the chargino1 has mass of 865 GeV and the neutralino1 has mass of 25 GeV is shown.

Observed and expected background and signal effective mass distributions for SR6j-2200. For signal, a gluino onestep decay model where gluinos have mass of 1705 GeV, the chargino1 has mass of 865 GeV and the neutralino1 has mass of 25 GeV is shown.

Observed 95% CL upper limit on the signal cross-section from searches in a SUSY scenario where squarks are produced in pairs and decay directly into the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from searches on the light-flavor squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay directly into the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from searches on the light-flavor squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay directly into the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the light-flavor squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay directly into the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the light-flavor squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay directly into the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from RJR-based searches on the light-flavor squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay directly into the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from RJR-based searches on the light-flavor squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay directly into the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from searches in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from RJR-based searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from RJR-based searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay directly into the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from searches in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from searches on the squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from searches on the squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from RJR-based searches on the squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from RJR-based searches on the squark and lightest neutralino masses in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from Meff-based searches in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the squark mass and the mass gap ratio x in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the squark mass and the mass gap ratio x in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from searches in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from RJR-based searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from RJR-based searches on the gluino and lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from Meff-based searches in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the gluino mass and the mass gap ratio x in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the gluino mass and the mass gap ratio x in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from Meff-based searches in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate the second lightest neutralino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{2}^{0} \rightarrow qq Z \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the gluino and second lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate the second lightest neutralino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{2}^{0} \rightarrow qq Z \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the gluino and second lightest neutralino masses in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate the second lightest neutralino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{2}^{0} \rightarrow qq Z \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from Meff-based searches in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino or second lightest neutralino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$, or $\tilde{q} \rightarrow q \tilde{\chi}_{2}^{0} \rightarrow qq Z/h \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the squark mass and the mass gap ratio x in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino or second lightest neutralino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$, or $\tilde{q} \rightarrow q \tilde{\chi}_{2}^{0} \rightarrow qq Z/h \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the squark mass and the mass gap ratio x in a SUSY scenario where squarks are produced in pairs and decay via an intermediate lightest chargino or second lightest neutralino to the lightest neutralino, $\tilde{q} \rightarrow q \tilde{\chi}_{1}^{\pm} \rightarrow q W^{\pm} \tilde{\chi}_{1}^{0}$, or $\tilde{q} \rightarrow q \tilde{\chi}_{2}^{0} \rightarrow qq Z/h \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from Meff-based searches in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino or second lightest neutralino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$, or $\tilde{g} \rightarrow qq \tilde{\chi}_{2}^{0} \rightarrow qq Z/h \tilde{\chi}_{1}^{0}$.

Expected 95% CL exclusion contours from Meff-based searches on the gluino mass and the mass gap ratio x in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino or second lightest neutralino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$, or $\tilde{g} \rightarrow qq \tilde{\chi}_{2}^{0} \rightarrow qq Z/h \tilde{\chi}_{1}^{0}$.

Observed 95% CL exclusion contours from Meff-based searches on the gluino mass and the mass gap ratio x in a SUSY scenario where gluinos are produced in pairs and decay via an intermediate lightest chargino or second lightest neutralino to the lightest neutralino, $\tilde{g} \rightarrow qq \tilde{\chi}_{1}^{\pm} \rightarrow qq W^{\pm} \tilde{\chi}_{1}^{0}$, or $\tilde{g} \rightarrow qq \tilde{\chi}_{2}^{0} \rightarrow qq Z/h \tilde{\chi}_{1}^{0}$.

Observed 95% CL upper limit on the signal cross-section from Meff-based searches for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=0$ GeV.

Expected 95% CL exclusion contours from Meff-based searches on the gluino and squark masses for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=0$ GeV.

Observed 95% CL exclusion contours from Meff-based searches on the gluino and squark masses for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=0$ GeV.

Observed 95% CL upper limit on the signal cross-section from Meff-based searches for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=695$ GeV.

Expected 95% CL exclusion contours from Meff-based searches on the gluino and squark masses for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=695$ GeV.

Observed 95% CL exclusion contours from Meff-based searches on the gluino and squark masses for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=695$ GeV.

Observed 95% CL upper limit on the signal cross-section from Meff-based searches for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=995$ GeV.

Expected 95% CL exclusion contours from Meff-based searches on the gluino and squark masses for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=995$ GeV.

Observed 95% CL exclusion contours from Meff-based searches on the gluino and squark masses for inclusive squark-gluino production in pMSSM models with $m_{\tilde{\chi}_{1}^0}=995$ GeV.

Cut-flow of Meff-2j for three supersymmetric models: a gluino direct decay model where gluinos have mass of 2000 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 0 $\mathrm{\ Ge\kern -0.1em V}$ (10000 generated events); and a squark direct decay model where squarks have mass of 1200 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 600 $\mathrm{\ Ge\kern -0.1em V}$ (20000 generated events); and a squark direct decay model where squarks have mass of 1500 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 0 $\mathrm{\ Ge\kern -0.1em V}$ (10000 generated events). The numbers are normalized to a luminosity of 36.1 fb$^{-1}$.

Cut-flow of Meff-3j,4j for three supersymmetric models: a gluino direct decay model where gluinos have mass of 2000 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 0 $\mathrm{\ Ge\kern -0.1em V}$ (10000 generated events); and a squark direct decay model where squarks have mass of 1200 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 600 $\mathrm{\ Ge\kern -0.1em V}$ (20000 generated events); and a squark direct decay model where squarks have mass of 1500 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 0 $\mathrm{\ Ge\kern -0.1em V}$ (10000 generated events). The numbers are normalized to a luminosity of 36.1 fb$^{-1}$.

Cut-flow of Meff-5j,6j for three supersymmetric models: a gluino direct decay model where gluinos have mass of 2000 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 0 $\mathrm{\ Ge\kern -0.1em V}$ (10000 generated events); and a squark direct decay model where squarks have mass of 1200 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 600 $\mathrm{\ Ge\kern -0.1em V}$ (20000 generated events); and a squark direct decay model where squarks have mass of 1500 $\mathrm{\ Ge\kern -0.1em V}$ and the $\tilde{\chi}_{1}^{0}$ has mass of 0 $\mathrm{\ Ge\kern -0.1em V}$ (10000 generated events). The numbers are normalized to a luminosity of 36.1 fb$^{-1}$.

Cut-flow for RJR-based SR's targeting squarks for SS direct model points. Expected yields are normalized to a luminosity of 36.1 fb$^{-1}$.

Cut-flow for RJR-based SR's targeting gluinos for GG direct model points. Expected yields are normalized to a luminosity of 36.1 fb$^{-1}$.

Cut-flow for RJR-based SR's targeting compressed mass-spectra signals for SS direct and GG direct model points. Expected yields are normalized to a luminosity of 36.1 fb$^{-1}$.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-1200.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-1600.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-2000.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-2400.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-2800.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-3600.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-2100.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-3j-1300.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-1000.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-1400.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-1800.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-2200.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-2600.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-3000.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-5j-1700.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-5j-1600.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-5j-2000.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-5j-2600.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-6j-1200.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-6j-1800.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-6j-2200.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-6j-2600.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2jB-1600.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2jB-2400.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S1a.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S1b.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S2a.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S2b.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S3a.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S3b.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S4.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C1.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C2.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C3.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C4.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C5.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G1a.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G1b.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G2a.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G2b.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G3a.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G3b.

Signal region acceptance for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G4.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-1200.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-1600.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-2000.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-2400.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-2800.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-3600.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-2100.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-3j-1300.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-1000.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-1400.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-1800.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-2200.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-2600.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-3000.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-5j-1700.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-5j-1600.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-5j-2000.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-5j-2600.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-6j-1200.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-6j-1800.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-6j-2200.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-6j-2600.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2jB-1600.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2jB-2400.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S1a.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S1b.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S2a.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S2b.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S3a.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S3b.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S4.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C1.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C2.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C3.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C4.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C5.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G1a.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G1b.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G2a.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G2b.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G3a.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G3b.

Signal region acceptance for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G4.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-1200.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-1600.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-2000.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-2400.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-2800.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-3600.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-2100.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-3j-1300.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-1000.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-1400.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-1800.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-2200.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-2600.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-3000.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-5j-1700.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-5j-1600.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-5j-2000.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-5j-2600.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-6j-1200.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-6j-1800.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-6j-2200.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-6j-2600.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2jB-1600.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2jB-2400.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S1a.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S1b.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S2a.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S2b.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S3a.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S3b.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S4.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C1.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C2.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C3.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C4.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C5.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G1a.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G1b.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G2a.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G2b.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G3a.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G3b.

Signal region acceptance for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G4.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-1200.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-1600.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-2000.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-2400.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-2800.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-3600.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-2100.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-3j-1300.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-1000.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-1400.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-1800.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-2200.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-2600.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-3000.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-5j-1700.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-5j-1600.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-5j-2000.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-5j-2600.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-6j-1200.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-6j-1800.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-6j-2200.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-6j-2600.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2jB-1600.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2jB-2400.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S1a.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S1b.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S2a.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S2b.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S3a.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S3b.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S4.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C1.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C2.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C3.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C4.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C5.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G1a.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G1b.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G2a.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G2b.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G3a.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G3b.

Signal region acceptance for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G4.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-1200.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-1600.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-2000.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-2400.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-2800.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-3600.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2j-2100.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-3j-1300.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-1000.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-1400.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-1800.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-2200.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-2600.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-4j-3000.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-5j-1700.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-5j-1600.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-5j-2000.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-5j-2600.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-6j-1200.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-6j-1800.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-6j-2200.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-6j-2600.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2jB-1600.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR Meff-2jB-2400.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S1a.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S1b.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S2a.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S2b.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S3a.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S3b.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-S4.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C1.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C2.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C3.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C4.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-C5.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G1a.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G1b.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G2a.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G2b.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G3a.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G3b.

Signal region efficiency for simplified model with squark pair production and direct decays to a quark and neutralino in SR RJR-G4.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-1200.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-1600.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-2000.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-2400.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-2800.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-3600.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2j-2100.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-3j-1300.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-1000.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-1400.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-1800.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-2200.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-2600.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-4j-3000.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-5j-1700.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-5j-1600.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-5j-2000.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-5j-2600.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-6j-1200.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-6j-1800.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-6j-2200.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-6j-2600.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2jB-1600.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR Meff-2jB-2400.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S1a.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S1b.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S2a.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S2b.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S3a.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S3b.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-S4.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C1.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C2.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C3.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C4.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-C5.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G1a.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G1b.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G2a.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G2b.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G3a.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G3b.

Signal region efficiency for simplified model with gluino pair production and direct decays to two quarks and neutralino in SR RJR-G4.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-1200.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-1600.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-2000.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-2400.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-2800.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-3600.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2j-2100.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-3j-1300.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-1000.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-1400.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-1800.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-2200.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-2600.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-4j-3000.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-5j-1700.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-5j-1600.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-5j-2000.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-5j-2600.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-6j-1200.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-6j-1800.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-6j-2200.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-6j-2600.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2jB-1600.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR Meff-2jB-2400.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S1a.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S1b.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S2a.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S2b.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S3a.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S3b.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-S4.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C1.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C2.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C3.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C4.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-C5.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G1a.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G1b.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G2a.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G2b.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G3a.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G3b.

Signal region efficiency for simplified model with squark pair production and decays to a quark and chargino in SR RJR-G4.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-1200.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-1600.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-2000.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-2400.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-2800.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-3600.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2j-2100.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-3j-1300.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-1000.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-1400.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-1800.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-2200.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-2600.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-4j-3000.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-5j-1700.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-5j-1600.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-5j-2000.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-5j-2600.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-6j-1200.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-6j-1800.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-6j-2200.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-6j-2600.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2jB-1600.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR Meff-2jB-2400.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S1a.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S1b.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S2a.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S2b.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S3a.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S3b.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-S4.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C1.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C2.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C3.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C4.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-C5.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G1a.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G1b.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G2a.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G2b.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G3a.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G3b.

Signal region efficiency for simplified model with gluino pair production and decays to two quarks and chargino in SR RJR-G4.

Pixel-tracklet $p_{T}$ spectrum of signal ($\tau_{\tilde{\chi}_{1}^{\pm}}$ = 0.2 ns and $m_{\tilde{\chi}_{1}^{\pm}}$ = 400 GeV) in electroweak channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of total background in electroweak channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of observed data in electroweak channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of fake tracklet in strong channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of muon background in strong channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of hadron and electron background in strong channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of signal ($m_{\tilde{g}}$ = 1600 GeV, $m_{\tilde{\chi}_{1}^{\pm}} = 500 GeV$) in strong channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of total background in strong channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of observed data in strong channel in the low-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of fake tracklet in electroweak channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of muon background in electroweak channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of hadron and electron background in electroweak channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of signal ($\tau_{\tilde{\chi}_{1}^{\pm}}$ = 0.2 ns and $m_{\tilde{\chi}_{1}^{\pm}}$ = 400 GeV) in electroweak channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of total background in electroweak channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of observed data in electroweak channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of fake tracklet in strong channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of muon background in strong channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of hadron and electron background in strong channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of signal ($m_{\tilde{g}}$ = 1600 GeV, $m_{\tilde{\chi}_{1}^{\pm}} = 500 GeV$) in strong channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of total background in strong channel in the high-Emiss region.

Pixel-tracklet $p_{T}$ spectrum of observed data in strong channel in the high-Emiss region.

Expected exclusion limit at 95% CL obtained in the electroweak production channel in terms of the chargino lifetime ($\tau_{\tilde{\chi}_{1}^{\pm}}$) and mass ($m_{\tilde{\chi}_{1}^{\pm}}$).

Observed exclusion limit at 95% CL obtained in the electroweak production channel in terms of the chargino lifetime ($\tau_{\tilde{\chi}_{1}^{\pm}}$) and mass ($m_{\tilde{\chi}_{1}^{\pm}}$).

Expected exclusion limit at 95% CL obtained in the strong production channel in terms of the gluino and chargino masses. The limit is shown assuming a chargino lifetime 0.2 ns.

Observed exclusion limit at 95% CL obtained in the strong production channel in terms of the gluino and chargino masses. The limit is shown assuming a chargino lifetime 0.2 ns.

Expected exclusion limit at 95% CL obtained in the strong production channel in terms of the gluino and chargino masses. The limit is shown assuming a chargino lifetime 1.0 ns.

Observed exclusion limit at 95% CL obtained in the strong production channel in terms of the gluino and chargino masses. The limit is shown assuming a chargino lifetime 1.0 ns.

Expected exclusion limit at 95% CL obtained in the electroweak production channel in terms of the chargino lifetime ($\tau_{\tilde{\chi}_{1}^{\pm}}$) and mass ($m_{\tilde{\chi}_{1}^{\pm}}$).

Observed exclusion limit at 95% CL obtained in the electroweak production channel in terms of the chargino lifetime ($\tau_{\tilde{\chi}_{1}^{\pm}}$) and mass ($m_{\tilde{\chi}_{1}^{\pm}}$).

Model dependent upper limits on cross-section (pb) for the electroweak production are shown by grey numbers in terms of the chargino lifetime ($\tau_{\tilde{\chi}_{1}^{\pm}}$) and mass ($m_{\tilde{\chi}_{1}^{\pm}}$).

Total acceptance $\times$ efficiency of the electroweak channel. The total signal acceptance $\times$ efficiency is defined as the probability of an event passing the signal region selection when an electroweak gaugino pair is produced in a pp collision.

Total acceptance $\times$ efficiency of the strong channel. In white regions, no simulation sample is available. The left-upper triangle region is not allowed kinematically in wino-LSP scenarios. The total signal acceptance $\times$ efficiency is calculated relative to events in which the gluinos decay into electroweak gaugino pairs.

The generator-level acceptance for charginos produced in the electroweak channel as a function of the chargino $eta$ and chargino decay radius (at generator level).

The acceptance $\times$ efficiency after reconstruction, for selecting and reconstructing charginos produced in the electroweak channel as a function of the chargino $\eta$ and chargino decay radius (at generator level). The acceptance $\times$ efficiency after reconstruction is the probability of a signal event, which passes all the event-level requirements, passing all the track/tracklet requirements after reconstruction.

The generator-level acceptance for charginos produced in the strong channel as a function of the chargino $\eta$ and chargino decay radius (at generator level).

The acceptance $\times$ efficiency after reconstruction, for selecting and reconstructing charginos produced in the strong channel as a function of the chargino $\eta$ and chargino decay radius (at generator level). The acceptance $\times$ efficiency after reconstruction is the probability of a signal event, which passes all the event-level requirements, passing all the track/tracklet requirements after reconstruction.

Summary of the selection criteria, and the corresponding observed number of events in data as well as the expected number of signal events in simulation for two benchmark models: a chargino produced in direct electroweak production with ($m_{\tilde{\chi}_{1}^{\pm}}$, $\tau_{\tilde{\chi}_{1}^{\pm}}$) = (400 GeV, 0.2 ns) in the high-Emiss region. The expected number of signal events is normalised to 36.1 fb${}^{-1}$. The signal selection efficiencies are also shown in parentheses. The first row shows the number of events after the application of detector and data quality conditions. Requirements below the dashed line are applied to tracks and tracklets.

Summary of the selection criteria, and the corresponding observed number of events in data as well as the expected number of signal events in simulation for two benchmark models: a chargino produced in the strong channel with ($m_{\tilde{g}}$, $m_{\tilde{\chi}_{1}^{\pm}}$, $\tau_{\tilde{\chi}_{1}^{\pm}}$) = (1600 GeV, 500 GeV, 0.2 ns) in the high-Emiss region. The expected number of signal events is normalised to 36.1 fb${}^{-1}$. The signal selection efficiencies are also shown in parentheses. The first row shows the number of events after the application of detector and data quality conditions. Requirements below the dashed line are applied to tracks and tracklets.

The event and tracklet generator-level acceptance and selection efficiency for a few electroweak signal models studied in this search. The last column shows the probability ($P$) for a reconstructed tracklet to have $p_{T}$ greater than 100 GeV.

The event and tracklet generator-level acceptance and selection efficiency for a few strong signal models studied in this search. The last column shows the probability ($P$) for a reconstructed tracklet to have $p_{T}$ greater than 100 GeV.

Systematic uncertainties in the signal event yields at $m_{\tilde{\chi}_{1}^{\pm}}$ = 400 GeV for the electroweak channel and at $m_{\tilde{g}}$ = 1600 GeV, $m_{\tilde{\chi}_{1}^{\pm}}$ = 500 GeV for the strong channel. The lifetime of the chargino is not relevant here. The uncertainty in the cross-section of the strong production is large due to the large effect from the PDF uncertainty.

Observed events, expected background for null signal, and expected signal yields for two benchmark models: electroweak channel with ($m_{\tilde{\chi}_{1}^{\pm}}$, $\tau_{\tilde{\chi}_{1}^{\pm}}$) = (400 GeV, 0.2 ns) and strong channel with ($m_{\tilde{g}}$, $m_{\tilde{\chi}_{1}^{\pm}}$, $\tau_{\tilde{\chi}_{1}^{\pm}}$) = (1600 GeV, 500 GeV, 0.2 ns) in the high-Emiss region. Also shown are the probability of a background-only experiment being more signal-like than observed ($p_0$) and the upper limit on the model-independent visible cross-section at 95\% CL. The uncertainty in the total background yield is different from the sum of uncertainties in quadrature due to anti-correlation between different backgrounds.

Effects of systematic uncertainties on the signal exclusion significance at $m_{\tilde{\chi}_{1}^{\pm}}$ = 400 GeV for the electroweak channel and at $m_{\tilde{g}}$ = 1600 GeV, $m_{\tilde{\chi}_{1}^{\pm}}$ = 500 GeV for the strong channel. The lifetime of the chargino is not relevant here. Effects of uncertainties on the fake-tracklet background is smaller in the strong channel analysis because the estimated number of the fake-tracklet background events is small.

Cross-section upper limits for the strong production, presented in unit of fb. Left-upper triangle region is unphysical because the wino mass is larger than the gluino mass.

Transverse mass mT in the llnunu search for the muon channel.

Upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance mass mH for the ggF production mode

Upper limits at 95% CL on the cross section times branching ratio as a function of the heavy resonance mass mH for the VBF production mode

Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function of mH for an additioinal heavy scalar assuming a width of 1% of mH

Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function of mH for an additioinal heavy scalar assuming a width of 5% of mH

Upper limits at 95% CL on the cross section for the ggF production model times branching ratio as a function of mH for an additioinal heavy scalar assuming a width of 10% of mH

Upper limits at 95% CL on the cross section times branching ratio for a KK graviton produced with k/M_{PI} = 1.

Upper limits on A to Z h production cross section x branching fraction in pb (gluon fusion production)

Upper limits on A to Z h production cross section x branching fraction in pb ( production with associated b-quarks)

Acceptance * Reconstruction efficiency for pp-> Zprime

Acceptance * Reconstruction efficiency for pp-> Zprime

Acceptance * Reconstruction efficiency for pp-> Wprime

Acceptance * Reconstruction efficiency for pp-> A (gluon fusion)

Acceptance * Reconstruction efficiency for pp-> A (gluon fusion)

Acceptance * Reconstruction efficiency for pp-> A (b-quark associated)

Acceptance * Reconstruction efficiency for pp-> A (b-quark associated)

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 10%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 20%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 30%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 40%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 50%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 60%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 70%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 80%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 90%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 1% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 2% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 3% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 4% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 5% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 6% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 7% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 8% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 9% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 10% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Upper limits at the 95% CL on the product of the production cross-section for pp->A and the branching fractions for A->Zh and h->bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 11% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 0%.

Event distributions of mT,Vh for the 0-lepton channel in the resolved 1-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of mT,Vh for the 0-lepton channel in the resolved 2-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of m,Vh for the 1-lepton channel in the resolved 1-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of m,Vh for the 1-lepton channel in the resolved 2-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of mT,Vh for the 2-lepton channel in the resolved 1-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of m,Vh for the 2-lepton channel in the resolved 2-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of mT,Vh for the 0-lepton channel in the boosted 1-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of mT,Vh for the 0-lepton channel in the boosted 2-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of m,Vh for the 1-lepton channel in the boosted 1-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of m,Vh for the 1-lepton channel in the boosted 2-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of m,Vh for the 2-lepton channel in the boosted 1-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

Event distributions of m,Vh for the 2-lepton channel in the boosted 2-btag category. The background prediction is shown after a background-only maximum-likelihood fit to the data.

The three isolated photons cross section with systematic and statistical uncertainties as a function of DPhi(Photon1,Photon2).

The three isolated photons cross section with systematic and statistical uncertainties as a function of DPhi(Photon1,Photon3).

The three isolated photons cross section with systematic and statistical uncertainties as a function of DPhi(Photon2,Photon3).

The three isolated photons cross section with systematic and statistical uncertainties as a function of |DEta(Photon1,Photon2)|.

The three isolated photons cross section with systematic and statistical uncertainties as a function of |DEta(Photon1,Photon3)|.

The three isolated photons cross section with systematic and statistical uncertainties as a function of |DEta(Photon2,Photon3)|.

The three isolated photons cross section with systematic and statistical uncertainties as a function of M(Photon1,Photon2).

The three isolated photons cross section with systematic and statistical uncertainties as a function of M(Photon1,Photon3).

The three isolated photons cross section with systematic and statistical uncertainties as a function of M(Photon2,Photon3).

The three isolated photons cross section with systematic and statistical uncertainties as a function of M(Photon1,Photon2,Photon3).