Measured charge asymmetry, $A_c$, values for the electron and muon channels combined after unfolding as a function of the $t\bar{t}$ transverse momentum, $p_{{\rm T}, t\bar{t}}$. The quoted uncertainties include statistical and systematic components after the marginalisation.

Correlation coefficients $\rho_{i,j}$ for the statistical and systematic uncertainties between the $i$-th and $j$-th bin of the differential $A_c$ measurement as a function of the $t\bar{t}$ invariant mass, $m_{t\bar{t}}$.

Correlation coefficients $\rho_{i,j}$ for the statistical and systematic uncertainties between the $i$-th and $j$-th bin of the differential $A_c$ measurement as a function of the $t\bar{t}$ velocity along the z-axis, $\beta_{z,t\bar{t}}$.

Correlation coefficients $\rho_{i,j}$ for the statistical and systematic uncertainties between the $i$-th and $j$-th bin of the differential $A_c$ measurement as a function of the transverse momentum, $p_{{\rm T}, t\bar{t}}$.

Measured prompt $X(3872) / \psi(2S)$ production ratio using the two-lifetime fit model.

Measured non-prompt $X(3872) / \psi(2S)$ production ratio using the two-lifetime fit model.

Measured short-lived non-prompt $X(3872)$ / total non-prompt $\psi(2S)$ production ratio using the two-lifetime fit model.

Measured long-lived non-prompt $X(3872)$ / total non-prompt $\psi(2S)$ production ratio using the two-lifetime fit model.

Measured cross section times branching fractions as a function of pT for prompt $\psi$(2S) production.

Measured cross section times branching fractions as a function of pT for non-prompt $\psi$(2S) production.

Measured cross section times branching fractions as a function of pT for prompt X(3872) production.

Measured cross section times branching fractions as a function of pT for non-prompt X(3872) production.

Measured non-prompt fraction for $\psi(2S)$ production.

Measured non-prompt fraction for X(3872) production.

Normalised differential decay width of $\psi(2S) \rightarrow J/\psi \pi\pi$ in bins of $m_{\pi\pi}$.

Normalised differential decay width of $X(3872) \rightarrow J/\psi \pi\pi$ in bins of $m_{\pi\pi}$.

Measured fiducial cross section in fb as a function of Yll.

Measured fiducial cross section in fb/GeV as a function of the leading jet pT, PT(JET1).

Measured normalised fiducial cross section as a function of Njet. Jet PT>25 GeV for |eta|<2.4 and PT>30 GeV for 2.4<|eta|<4.5.

Measured normalised fiducial cross section in 1/GeV as a function of pTH.

Measured normalised fiducial cross section as a function of Yll.

Measured normalised fiducial cross section in 1/GeV as a function of the leading jet pT, PT(JET1).

Jet veto efficiency as a function of PT(JET1) pT threshold.

Full correlation matrix for the measured differential cross section as a function of Njet, taking into account statistical and systematic uncertainties.

Full correlation matrix for the measured differential cross section as a function of pTH, taking into account statistical and systematic uncertainties.

Full correlation matrix for the measured differential cross section as a function of Yll, taking into account statistical and systematic uncertainties.

Full correlation matrix for the measured differential cross section as a function of the leading jet pT, taking into account statistical and systematic uncertainties.

Full correlation matrix for the measured normalised differential cross section as a function of Njet, taking into account statistical and systematic uncertainties.

Full correlation matrix for the measured normalised differential cross section as a function of pTH, taking into account statistical and systematic uncertainties.

Full correlation matrix for the measured normalised differential cross section as a function of Yll, taking into account statistical and systematic uncertainties.

Full correlation matrix for the measured normalised differential cross section as a function of the leading jet pT, taking into account statistical and systematic uncertainties.

Fiducial cross section of H+0-jet events in femtobarn for different values of PT(JET1) pT threshold with the uncertainties for each bin given in absolute values and in percent. The asterisk for the 25 GeV column header indicates that the results are for a mixed jet pT threshold, which is raised from 25 GeV to 30 GeV for jets with 2.5 < |eta| < 4.5.

Correction factors from inclusive parton level to fiducial particle level for bins of Njet derived with POWHEG NNLOPS+Pythia8. Uncertainties due to the non-perturbative correction are dominant for the correction factors.

Correction factors from inclusive parton level to fiducial particle level for bins of the leading jet pT derived with POWHEG NNLOPS+Pythia8. Uncertainties due to the non-perturbative correction are dominant for the correction factors.

Correction factors from inclusive parton level to fiducial particle level for the jet-veto efficiency with different jet pT thresholds derived with POWHEG NNLOPS+Pythia8. The asterisk on the 25 GeV bin label indicates that the results are for a mixed pT threshold, which is raised from 25 GeV to 30 GeV for jets with 2.5 < |eta| < 4.5, corresponding to the selection used to define the signal regions for the analysis.

The cross-section in bins of the di-$J/\psi$ transverse momentum in the forward rapidity region, assuming unpolarised $J/\psi$ mesons and excluding the $J/\psi$ spin-alignment systematic uncertainty. The branching fraction and luminosity uncertainties are not included in the systematic uncertainty as they are constant at 1.1$\%$ and 1.9$\%$ respectively.

The cross-section in bins of the di-$J/\psi$ invariant mass in the central rapidity region, assuming unpolarised $J/\psi$ mesons and excluding the $J/\psi$ spin-alignment systematic uncertainty. The branching fraction and luminosity uncertainties are not included in the systematic uncertainty as they are constant at 1.1$\%$ and 1.9$\%$ respectively.

The cross-section in bins of the di-$J/\psi$ invariant mass in the forward rapidity region, assuming unpolarised $J/\psi$ mesons and excluding the $J/\psi$ spin-alignment systematic uncertainty. The branching fraction and luminosity uncertainties are not included in the systematic uncertainty as they are constant at 1.1$\%$ and 1.9$\%$ respectively.

The total cross-section, DPS cross-section, $f_{\mathrm{DPS}}$, and average acceptance correction in the muon fiducial volume for the $\Delta y$ distribution. The branching fraction and luminosity uncertainties are not included in the systematic uncertainty as they are constant at 1.1$\%$ and 1.9$\%$ respectively.

The total cross-section, DPS cross-section, $f_{\mathrm{DPS}}$, and average acceptance correction in the muon fiducial volume for the $\Delta \phi$ distribution. The branching fraction and luminosity uncertainties are not included in the systematic uncertainty as they are constant at 1.1$\%$ and 1.9$\%$ respectively.

The total cross-section, DPS cross-section, $f_{\mathrm{DPS}}$, and average acceptance correction in the muon fiducial volume for the $m$($J/\psi$ $J/\psi$) distribution. The branching fraction and luminosity uncertainties are not included in the systematic uncertainty as they are constant at 1.1$\%$ and 1.9$\%$ respectively.

The total cross-section, DPS cross-section, $f_{\mathrm{DPS}}$, and average acceptance correction in the muon fiducial volume for the $p_{\mathrm{T}}$($J/\psi$ $J/\psi$) distribution. The branching fraction and luminosity uncertainties are not included in the systematic uncertainty as they are constant at 1.1$\%$ and 1.9$\%$ respectively.

The average acceptance weight for each spin-alignment scenario relative to the unpolarised case in bins of the sub-leading $J/\psi$ transverse momentum in the central rapidity region.

The average acceptance weight for each spin-alignment scenario relative to the unpolarised case in bins of the sub-leading $J/\psi$ transverse momentum in the forward rapidity region.

The average acceptance weight for each spin-alignment scenario relative to the unpolarised case in bins of the di-$J/\psi$ transverse momentum in the central rapidity region.

The average acceptance weight for each spin-alignment scenario relative to the unpolarised case in bins of the di-$J/\psi$ transverse momentum in the forward rapidity region.

The average acceptance weight for each spin-alignment scenario relative to the unpolarised case in bins of the di-$J/\psi$ invariant in the central rapidity region.

The average acceptance weight for each spin-alignment scenario relative to the unpolarised case in bins of the di-$J/\psi$ invariant in the forward rapidity region.

The measured fiducial cross sections are corrected to the dressed level. The ratio of $C_{WZ}^{\textrm{dressed}}/C_{WZ}^{\textrm{Born}}$ factors presented in this table can be used to correct fiducial integrated cross sections from dressed to Born level.

Cross section extrapolated to total phase space and all W and Z boson decays. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the theory uncertainty and the third is the luminosity uncertainty.

The total cross section is measured at dressed level and can also be corrected to Born level use this acceptance correction factor.

Ratio of fiducial cross sections measured for $W^{+} Z$ and $W^{-} Z$ production. The first systematic uncertainty is the combined systematic uncertainty excluding the luminosity uncertainty, the second is the luminosity uncertainty.

Observed and expected upper limits at $95\%$ CL in fb on the fiducial cross section $\sigma^{\mathrm{fid.}}_{W^{\pm} Zjj \textrm{-EW} \rightarrow \ell^{'} \nu \ell \ell}$, multiplied by the $W$ and $Z$ branching ratios in a single leptonic channel with muons or electrons in the VBS fiducial phase space. Values obtained with or without subtraction of the $tZj$ contribution are presented. The $1$ $\sigma$ and $2$ $\sigma$ uncertainty intervals around the expected limits are also indicated.

Observed and expected upper limits at $95\%$ CL in fb on the fiducial cross section $\sigma^{\mathrm{fid.}}_{W^{\pm} Zjj \textrm{-EW} \rightarrow \ell^{'} \nu \ell \ell}$, multiplied by the $W$ and $Z$ branching ratios in a single leptonic channel with muons or electrons in the aQGC fiducial phase space. Values obtained with or without subtraction of the $tZj$ contribution are presented. The $1$ $\sigma$ and $2$ $\sigma$ uncertainty intervals around the expected limits are also indicated.

Expected and observed one-dimensional 95% Confidence Level intervals on the anomalous couplings parameters. Anomalous couplings are introduced as form factors using a cut-off scale $\Lambda_{\mathrm{co}}$.

Expected and observed one-dimensional intervals at 95% Confidence Level on the Effective Field Theory (EFT) parameters.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$.

Breakdown of systematic uncertainties in percent for the measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> mu+mu- final state at 13TeV.

Measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the combined Z/gamma* -> l+l- (l = e, mu) final state.

Measured total cross section times leptonic branching ratio for Z/gamma* production in the combined Z/gamma* -> l+ l- (l = e, mu) final state.

Measured total cross-section for ttbar events using e-mu events with b-tagged jets.

Correlation coefficients amongst the combined (Z/gamma^* -> l+ l-) where (l = e, mu) fiducial cross section and ttbar total cross section at 13, 8, and 7TeV.

Correlation coefficients amongst the combined (Z/gamma^* -> l+ l-) where (l = e, mu) fiducial cross section and ttbar total cross section at 13, 8, and 7TeV, omitting the common normalisation uncertainty due to the luminosity calibration and beam energy.

Z-boson and ttbar production cross-section single ratios at 13, 8, 7TeV. The beam-energy uncertainty, which largely cancels in the ratios, is included in the systematic uncertainty. In the first column, the total (TOT) cross sections are used for both numerator and denominator. In the second column, the total cross section is used for the numerator while the fiducial (FID) cross section is used for the denominator. In the third column, the fiducial cross sections are used for both numerator and denominator. Apart for the MZ requirement, the kinematic fiducial requirements listed below apply only to the fiducial cross sections. The luminosity uncertainty almost entirely cancels in some of the ratio measurements.

Z-boson and ttbar production cross-section double ratios at 13, 8, 7TeV. The beam-energy uncertainty, which largely cancels in the ratios, is included in the systematic uncertainty. In the first column, the total (TOT) cross sections are used for both ttbar and Z processes. In the second column, the total cross section is used for ttbar while the fiducial (FID) cross section is used for Z. In the third column, the fiducial cross sections are used for both ttbar and Z. Apart for the MZ requirement, the kinematic fiducial requirements listed below apply only to the fiducial cross sections.

Integrated fiducial cross-sections for QCD+EW and EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Integrated fiducial cross-sections for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Integrated fiducial cross-sections for QCD+EW and EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Integrated fiducial cross-sections for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Integrated fiducial cross-sections for QCD+EW $Wjj$ production in the central-jet region.

Integrated fiducial cross-sections for EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Integrated fiducial cross-sections for QCD+EW and EW-only $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the jet centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the lepton centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the number of jets in the rapidity gap for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the forward-lepton region.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the forward-lepton region.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the forward-lepton region.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the forward-lepton region.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the forward-lepton region.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the jet centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the lepton centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the number of jets in the rapidity gap for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the jet centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the lepton centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the number of jets in the rapidity gap for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of the jet centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of the lepton centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of the number of jets in the rapidity gap for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Normalised differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the central-jet region.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the central-jet region.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the central-jet region.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the central-jet region.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the central-jet region.

Normalised differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of the jet centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of the lepton centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of the number of jets in the rapidity gap for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the forward-lepton region.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the forward-lepton region.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the forward-lepton region.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the forward-lepton region.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the forward-lepton region.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the jet centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the lepton centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the number of jets in the rapidity gap for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the jet centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the lepton centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the number of jets in the rapidity gap for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of the jet centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of the lepton centrality for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of the number of jets in the rapidity gap for QCD+EW $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the forward-lepton/central-jet region.

Absolute differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the central-jet region.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the central-jet region.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the central-jet region.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the central-jet region.

Absolute differential fiducial cross-section of the dijet mass for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the dijet $p_\text{T}$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for QCD+EW $Wjj$ production in the signal region with $m_{jj} > 0.5$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the lepton centrality for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the number of jets in the rapidity gap for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Normalised differential fiducial cross-section of the dijet mass for EW-only $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the dijet $p_\text{T}$ for EW-only $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for EW-only $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for EW-only $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for EW-only $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the dijet mass for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta y(j_1, j_2)$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the lepton centrality for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of the number of jets in the rapidity gap for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Normalised differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of the leading-jet $p_\text{T}$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of the lepton centrality for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Normalised differential fiducial cross-section of the number of jets in the rapidity gap for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of the number of jets in the rapidity gap for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.5$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for EW-only $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for EW-only $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for EW-only $Wjj$ production in the signal region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of the number of jets in the rapidity gap for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 1.0$ TeV.

Absolute differential fiducial cross-section of $\Delta\phi(j_1,j_2) / \pi$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of $\Delta y(j_1, j_2)$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of the leading-jet $p_\text{T}$ for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

Absolute differential fiducial cross-section of the number of jets in the rapidity gap for EW-only $Wjj$ production in the inclusive region with $m_{jj} > 2.0$ TeV.

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).

Cross-section upper limits as a function of the mass of the lightest stau for the GMSB models with $\tan\beta = 40$. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Cross-section upper limits as a function of the mass of the lightest stau for the GMSB models with $\tan\beta = 50$. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Cross-section upper limits as a function of the $\tilde{\tau}_1$ mass for direct $\tilde{\tau}_1$ production and three values of $\tan\beta$. Expected limits for $\tan\beta=10$ with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties observed limits for three values of $\tan\beta$ and theoretical cross-section prediction for $\tan\beta=10$ with $\pm 1\sigma$ band.

Cross-section upper limits as a function of the $\tilde{\chi}_1$ mass for $\tilde{\tau}_1$ sleptons resulting from the decay of directly produced charginos and neutralinos in GMSB. Observed limits, expected limits for $\tan\beta=10$ with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties and theoretical cross-section prediction (dominated by $\tilde{\chi}^0_1 \tilde{\chi}^+_1$ production) with $\pm 1\sigma$ uncertainty. Depending on the hypothesis and to a small extent on $\tan\beta$, in these models, the chargino mass is 210 to 260 GeV higher than the neutralino mass.

Cross-section upper limits for various chargino masses in stable-chargino models. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Cross-section upper limits as a function of the LLP mass for the gluino R-Hadron models for the MS-agnostic search. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Cross-section upper limits as a function of the LLP mass for the gluino R-Hadron models for the full-detector search. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Cross-section upper limits as a function of the LLP mass for the sbottom R-Hadron models for the MS-agnostic search. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Cross-section upper limits as a function of the LLP mass for the sbottom R-Hadron models for the full-detector search. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Cross-section upper limits as a function of the LLP mass for the stop R-Hadron models for the MS-agnostic search. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Cross-section upper limits as a function of the LLP mass for the stop R-Hadron models for the full-detector search. Expected limit with $\pm 1\sigma$ and $\pm 2\sigma$ uncertainties, observed limit and theoretical cross-section prediction with $\pm 1\sigma$ uncertainties.

Observed and expected 95% CL upper limits on the cross section times branching fraction as a function of the resonance pole mass for the G$^*$. The LO theoretical cross section for the G$^*$ production is also shown.

Observed and expected 95% CL upper limits on the cross section times branching fraction as a function of the resonance pole mass for the EGM W'. The NNLO theoretical cross section for the EGM W' production is also shown.