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.

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 $\ell, \ell' = e, \mu$.

Kinematic distributions for "extended SR selections" of the 2-tau channel, for mTsum in the Compressed SR selection without the mTsum>1400 GeV requirement. The last bin includes overflow events. Cited uncertainties are statistical uncertainties only. Signal predictions are overlaid for several benchmark models, normalised to their predicted cross sections. For the simplified model, "MM" refers to a medium mass splitting, with m(gluino)=1145 GeV and m(neutralino)=265 GeV; "HM" denotes a high mass splitting scenario, with m(gluino)=1305 GeV and m(neutralino)=105 GeV. The GMSB benchmark model corresponds to Lambda = 90 TeV and tanbeta = 40.

Kinematic distributions for "extended SR selections" of the 2-tau channel, for mTtau1+mTtau2 in the High-Mass SR selection without the mTtau1+mTtau2>350GeV requirement. The last bin includes overflow events. Cited uncertainties are statistical uncertainties only. Signal predictions are overlaid for several benchmark models, normalised to their predicted cross sections. For the simplified model, "MM" refers to a medium mass splitting, with m(gluino)=1145 GeV and m(neutralino)=265 GeV; "HM" denotes a high mass splitting scenario, with m(gluino)=1305 GeV and m(neutralino)=105 GeV. The GMSB benchmark model corresponds to Lambda = 90 TeV and tanbeta = 40.

Kinematic distributions for "extended SR selections" of the 2-tau channel, for HT in the GMSB SR selection without the HT > 1700 GeV requirement. The last bin includes overflow events. Cited uncertainties are statistical uncertainties only. Signal predictions are overlaid for several benchmark models, normalised to their predicted cross sections. For the simplified model, "MM" refers to a medium mass splitting, with m(gluino)=1145 GeV and m(neutralino)=265 GeV; "HM" denotes a high mass splitting scenario, with m(gluino)=1305 GeV and m(neutralino)=105 GeV. The GMSB benchmark model corresponds to Lambda = 90 TeV and tanbeta = 40.

Expected exclusion contour at the 95% confidence level for the simplified model of gluino pair production, based on the combined results from the 1tau and 2tau channel. The result is obtained using 3.2 fb-1 of sqrt(s) = 13 TeV ATLAS data.

Observed exclusion contour at the 95% confidence level for the simplified model of gluino pair production, based on the combined results from the 1tau and 2tau channel. The result is obtained using 3.2 fb-1 of sqrt(s) = 13 TeV ATLAS data.

Expected exclusion contour at the 95% confidence level for the simplified model of gluino pair production, based on results from the 2tau channel. The result is obtained using 3.2 fb-1 of sqrt(s) = 13 TeV ATLAS data.

Expected exclusion contour at the 95% confidence level for the simplified model of gluino pair production, based on results from the 1tau channel. The result is obtained using 3.2 fb-1 of sqrt(s) = 13 TeV ATLAS data.

Observed exclusion contours at the 95% confidence level for the gauge-mediated supersymmetry-breaking model, based on results from the 2 tau channel. The result is obtained using 3.2 fb-1 of sqrt(s) = 13 TeV ATLAS data. Additional model parameters are M(mess) = 250 TeV, N5 = 3, mu>0 and Cgrav =1.

Expected exclusion contours at the 95% confidence level for the gauge-mediated supersymmetry-breaking model, based on results from the 2 tau channel. The result is obtained using 3.2 fb-1 of sqrt(s) = 13 TeV ATLAS data. Additional model parameters are M(mess) = 250 TeV, N5 = 3, mu>0 and Cgrav =1.

Observed upper cross section limits in pb for the simplified model of gluino pair production for the combination of all SRs.

Best expected signal region for the simplified model of gluino pair production. The respective SR has been used in the combination of the results.

Acceptance for the gluino production simplified model grid in the Compressed 1tau signal region.

Efficiency for the gluino production simplified model grid in the Compressed 1tau signal region.

Acceptance times Efficiency for the gluino production simplified model grid in the Compressed 1tau signal region.

Acceptance for the gluino production simplified model grid in the medium mass 1tau signal region.

Efficiency for the gluino production simplified model grid in the medium mass 1tau signal region.

Acceptance times Efficiency for the gluino production simplified model grid in the medium mass 1tau signal region.

Acceptance for the gluino production simplified model grid in the high mass 1tau signal region.

Efficiency for the gluino production simplified model grid in the high mass 1tau signal region.

Acceptance times Efficiency for the gluino production simplified model grid in the high mass 1tau signal region.

Acceptance for the gluino production simplified model grid in the compressed 2tau signal region.

Efficiency for the gluino production simplified model grid in the compressed 2tau signal region.

Acceptance times Efficiency for the gluino production simplified model grid in the compressed 2tau signal region.

Acceptance for the gluino production simplified model grid in the high mass 2tau signal region.

Efficiency for the gluino production simplified model grid in the high mass 2tau signal region.

Acceptance times Efficiency for the gluino production simplified model grid in the high mass 2tau signal region.

Acceptance for the GMSB model grid in the 2tau signal region.

Efficiency for the GMSB model grid in the 2tau signal region.

Acceptance times Efficiency for the GMSB model grid in the 2tau signal region.

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.