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).

Normalised differential cross-section in the fiducial region as a function of lepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of lepton eta. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of lepton eta. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of lepton eta. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of lepton eta. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of dilepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of dilepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of dilepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of dilepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of dilepton invariant mass. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of dilepton invariant mass. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of dilepton invariant mass. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of dilepton invariant mass. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of dilepton rapidity. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of dilepton rapidity. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of dilepton rapidity. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of dilepton rapidity. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of the azimuthal angle between the leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of the azimuthal angle between the leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of the azimuthal angle between the leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of the azimuthal angle between the leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of the sum of pT of the two leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of the sum of pT of the two leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of the sum of pT of the two leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of the sum of pT of the two leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of the sum of the energies of the two leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Absolute differential cross-section in the fiducial region as a function of the sum of the energies of the two leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of the sum of the energies of the two leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Normalised differential cross-section in the fiducial region as a function of the sum of the energies of the two leptons. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb).

Reconstructed mass $m_\beta$ in observed data, background estimate and expected signal ($\tilde{\chi}^{\pm}_1$ masses of 400 and 600 GeV) in the chargino search for the lower of the two masses ($m$) in the two-candidate signal region.

Reconstructed mass $m_\beta$ in observed data, background estimate and expected signal ($\tilde{\chi}^{\pm}_1$ masses of 400 and 600 GeV) in the chargino search for the one-loose-candidate signal region.

Reconstructed mass $m_\beta$ in observed data, background estimate and expected signal ($\tilde{\chi}^{\pm}_1$ masses of 400 and 600 GeV) in the chargino search for the one-candidate signal region.

Data and background estimates for the reconstructed mass based on time-of-flight, $m_{\beta}$, for combined candidates in the full-detector 500 GeV gluino R-Hadron search (SR-RH-FD).

Data and background estimates for the reconstructed mass based on specific energy loss, $m_{\beta\gamma}$, for combined candidates in the full-detector 500 GeV gluino R-Hadron search (SR-RH-FD).

Data and background estimates for the reconstructed mass based on time-of-flight, $m_{\beta}$, for the MS-agnostic 500 GeV sbottom and $m_{\beta\gamma}$ R-Hadron search (SR-RH-MA).

Data and background estimates for the reconstructed mass based on specific energy loss, $m_{\beta\gamma}$, for the MS-agnostic 500 GeV stop R-Hadron search (SR-RH-MA).

Cross-section upper limits as a function of the mass of the lightest stau for the GMSB models with $\tan\beta = 10$. 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 $\tan\beta = 20$. 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 $\tan\beta = 30$. 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 $\tan\beta = 40$. 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.

Observed 95% CL exclusion contour for directly produced sleptons in the plane $\Delta=m(\tilde{\ell})-m(\tilde{\tau}_1)$ vs. $m(\tilde{\tau}_1)$.

Expected 95% CL exclusion contour for directly produced sleptons in the plane $\Delta=m(\tilde{\ell})-m(\tilde{\tau}_1)$ vs. $m(\tilde{\tau}_1)$.

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.

Observed 95% CL exclusion contour for the LeptoSUSY model.

Expected 95% CL exclusion contour for the LeptoSUSY model.

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.

Summary of systematic uncertainties for the slepton searches (given in percent). Ranges indicate a mass dependence for the given uncertainty (low mass to high mass).

Summary of systematic uncertainties for the chargino and R-Hadron searches (given in percent). Ranges indicate a mass dependence for the given uncertainty (low mass to high mass).

Observed and expected event yields, as well as efficiencies and uncertainties for three MC simulation signal samples, in the two signal regions used in the GMSB slepton search. Cross-section upper limits are stated at 95% CL.

Observed and expected event yields, as well as efficiencies and uncertainties for three MC simulation signal samples, in the three signal regions used in the LeptoSUSY slepton search. Cross-section upper limits are stated at 95% CL.

Observed and expected event yields, as well as efficiencies and uncertainties for three MC simulation signal samples, in the three signal regions used in the chargino search. Cross-section upper limits are stated at 95% CL.

Observed and expected event yields, as well as efficiencies and uncertainties for three MC simulation signal samples, in the R-Hadron searches. Cross-section upper limits are stated at 95% CL.

Mass of the $\tilde{\tau}_1$; cross-section; minimum $p_T$, maximum $\beta$ and minimum $m_{\beta}$ requirements; expected number of signal events (exp.); signal selection efficiency (eff.); background estimate (est.); observed number of events (obs.); expected upper cross-section limit ($\sigma^\mathrm{exp}$); and observed upper cross-section limit ($\sigma^\mathrm{obs}$) for the two signal regions used in the GMSB slepton search.

Mass of the $\tilde{\tau}_1$; cross-section; minimum \pt, maximum $\beta$ and minimum $m_{\beta}$ requirements; expected number of signal events (exp.); signal selection efficiency (eff.); background estimate (est.); observed number of events (obs.); expected upper cross-section limit ($\sigma^\mathrm{exp}$); and observed upper cross-section limit ($\sigma^\mathrm{obs}$) for the two signal regions used in the directly produced $\tilde{\tau}_1$ search.

Masses of the $\tilde{g}$ and $\tilde{q}$; cross-section; minimum \pt, maximum $\beta$ and minimum $m_{\beta}$ requirements; expected number of signal events (exp.); signal selection efficiency (eff.); background estimate (est.); observed number of events (obs.); expected upper cross-section limit ($\sigma^\mathrm{exp}$); and observed upper cross-section limit ($\sigma^\mathrm{obs}$) for the two signal regions used in the LeptoSUSY search.

Slepton search candidate requirements and example candidate selection flow for loose and tight selections.

Mass of the $\tilde{\chi}^{\pm}_{1}$; cross-section; minimum $p_T$, maximum $\beta$ and minimum $m_{\beta}$ requirements; expected number of signal events (exp.); signal selection efficiency (eff.); background estimate (est.); observed number of events (obs.); expected upper cross-section limit ($\sigma^\mathrm{exp}$); and observed upper cross-section limit ($\sigma^\mathrm{obs}$) for the three signal regions used in the chargino search.

Chargino search candidate requirements and example candidate selection flow for the total production as well as chargino-neutralino (CN) and chargino-pair (CC) production separately.

Mass of the LLP; cross-section; minimum $p$, maximum $\beta\gamma$, maximum $\beta$, minimum $m_{\beta\gamma}$ and minimum $m_{\beta}$ requirements; expected signal (exp.); signal efficiency (eff.); background estimate (est.); observed number of events (obs.); expected upper cross-section limit ($\sigma^\mathrm{exp}$); and observed upper cross-section limit ($\sigma^\mathrm{obs}$) for all R-Hadron models considered in the R-Hadron MS-agnostic (SR-RH-MA) search.

Mass of the LLP; cross-section; minimum $p$, maximum $\beta\gamma$, maximum $\beta$, minimum $m_{\beta\gamma}$ and minimum $m_{\beta}$ requirements; expected signal (exp.); signal efficiency (eff.); background estimate (est.); observed number of events (obs.); expected upper cross-section limit ($\sigma^\mathrm{exp}$); and observed upper cross-section limit ($\sigma^\mathrm{obs}$) for all R-Hadron models considered in the R-Hadron full-detector (SR-RH-FD) search. In cases where two numbers are stated, these reflect the values in the ID+calorimeter and combined selection, respectively, used in this search.

Muon-agnostic search R-Hadron candidate requirements and example candidate selection flow for ID+calorimeter selection.

Full-detector search R-Hadron candidate requirements and example candidate selection flow for combined selection.