Ratio of fiducial cross sections measured for $W^{\pm} Z$ production at $\sqrt{s}=13$ TeV and $\sqrt{s}=8$ TeV. The first systematic uncertainty is the combined systematic uncertainty excluding the luminosity uncertainty, the second is the luminosity uncertainty.

Ratio of fiducial cross sections measured for $W^{+} Z$ and $W^{-} Z$ production.

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 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.

Measured fiducial cross section as a function of the exclusive jet multiplicity, where jets are particle level jets with anti-kt R=0.4. 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.

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

Correlation matrix for the total uncertainties, including all sources of systematic and statistical uncertainties, for the differential cross section as a function of the exclusive jet multiplicity.

All correlated systematic relative uncertainties in percent on measured differential cross section as a function of the exclusive jet multiplicity.

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

Measured fiducial cross section times leptonic branching ratio for W+ production in the W+ -> mu+ nu final state.

Measured fiducial cross section times leptonic branching ratio for W- production in the W- -> mu- nubar final state.

Measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> mu+ mu- final state.

Measured fiducial cross-section ratios (lepton universality) R_{W} = sigma(W+/- -> e+/- nu/nubar)/sigma (W+/- -> mu+/- nu/nubar) and R_{Z} = sigma (Z/gamma^* -> e+ e-)/sigma (Z/gamma* -> mu+ mu-), and the correlation coefficient.

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

Measured fiducial cross section times leptonic branching ratio for W- production in the combined W- -> l- nubar (l = e, mu) final state.

Measured fiducial cross section times leptonic branching ratio for W+/- production in the combined W+ -> l+ nu and W- -> l- nubar (l = e, mu) final state.

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 W+ production in the W+ -> e+ nu final state.

Measured total cross section times leptonic branching ratio for W- production in the W- -> e- nubar final state.

Measured total cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> e+ e- final state.

Measured total cross section times leptonic branching ratio for W+ production in the W+ -> mu+ nu final state.

Measured total cross section times leptonic branching ratio for W- production in the W- -> mu- nubar final state.

Measured total cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> mu+ mu- final state.

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

Measured total cross section times leptonic branching ratio for W- production in the combined W- -> l- nubar (l = e, mu) final state.

Measured total cross section times leptonic branching ratio for W+/- production in the combined W+ -> l+ nu and W- -> l- nubar (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 fiducial cross-section ratio R_{W+-/Z} = sigma (W+/- -> l+/- nu/nubar) / sigma (Z/gamma^* -> l+ l-) where (l = e, mu).

Measured fiducial cross-section ratio R_{W+/W-} = sigma (W+ -> l+ nu) / sigma (W- -> l- nubar) where (l = e, mu).

Correlation coefficients among (W- -> l- nubar), (W+ -> l+ nu), (Z/gamma^* -> l+ l-) where (l = e, mu) excluding the common normalisation uncertainty due to the luminosity calibration.

Measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> e+e- final state.

Measured fiducial cross section times leptonic branching ratio for W+ production in the W+ -> mu+ nu final state.

Measured fiducial cross section times leptonic branching ratio for W- production in the W- -> mu- nubar final state.

Measured fiducial cross section times leptonic branching ratio for W+/- production in the combined W+ -> mu+ nu and W- -> mu- nubar final state.

Measured fiducial cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> mu+ mu- final state.

Measured total cross section times leptonic branching ratio for W+ production in the W+ -> e+ nu final state.

Measured total cross section times leptonic branching ratio for W- production in the W- -> e- nubar final state.

Measured total cross section times leptonic branching ratio for W+/- production in the combined W+ -> e+ nu and W- -> e- nubar final state.

Measured total cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> e+ e- final state.

Measured total cross section times leptonic branching ratio for W+ production in the W+ -> mu+ nu final state.

Measured total cross section times leptonic branching ratio for W- production in the W- -> mu- nubar final state.

Measured total cross section times leptonic branching ratio for W+/- production in the combined W+ -> mu+ nu and W- -> mu- nubar final state.

Measured total cross section times leptonic branching ratio for Z/gamma* production in the Z/gamma* -> mu+ mu- final state.

Measured total cross section times leptonic branching ratio for W+ production in the W+ -> l+ nu (l = e, mu) final states.

Measured total cross section times leptonic branching ratio for W- production in the W- -> l- nubar (l = e, mu) final states.

Measured total cross section times leptonic branching ratio for W+/- production in the combined W+ -> l+ nu and W- -> l- nubar (l = e, mu) final states.

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

Measured total cross-section ratio R_{W+/Z} = sigma (W+ -> e+ nu) / sigma (Z/gamma^* -> e+ e-).

Measured total cross-section ratio R_{W-/Z} = sigma (W- -> e- nubar) / sigma (Z/gamma^* -> e+ e-).

Measured total cross-section ratio R_{W+-/Z} = sigma (W+/- -> e+/- nu/nubar) / sigma (Z/gamma^* -> e+ e-).

Measured total cross-section ratio R_{W+/Z} = sigma (W+ -> mu+ nu) / sigma (Z/gamma^* -> mu+ mu-).

Measured total cross-section ratio R_{W-/Z} = sigma (W- -> mu- nubar) / sigma (Z/gamma^* -> mu+ mu-).

Measured total cross-section ratio R_{W+-/Z} = sigma (W+/- -> mu+/- nu/nubar) / sigma (Z/gamma^* -> mu+ mu-).

Measured total cross-section ratio R_{W+/Z} = sigma (W+ -> l+ nu) / sigma (Z/gamma^* -> l+ l-) where (l = e, mu).

Measured total cross-section ratio R_{W-/Z} = sigma (W- -> l- nubar) / sigma (Z/gamma^* -> l+ l-) where (l = e, mu).

Measured total cross-section ratio R_{W+-/Z} = sigma (W+/- -> l+/- nu/nubar) / sigma (Z/gamma^* -> l+ l-) where (l = e, mu).

Measured lepton asymmetry from W+ -> e+ nu and W- -> e- nubar, binned as a function pseudorapidity.

Measured lepton asymmetry from W+ -> e+ nu and W- -> e- nubar.

Measured lepton asymmetry from W+ -> mu+ nu and W- -> mu- nubar, binned as a function pseudorapidity.

Measured lepton asymmetry from W+ -> mu+ nu and W- -> mu- nubar.

Measured lepton asymmetry from W+ -> l+ nu and W- -> l- nubar (l = e, mu), binned as a function pseudorapidity.

Measured lepton asymmetry from W+ -> l+ nu and W- -> l- nubar (l = e, mu).

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

.

The measured W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 3 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 4 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 3 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 4 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the third jet in the event for jet multiplicities >= 3 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the third jet in the event for jet multiplicities >= 4 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the fourth jet in the event for jet multiplicities >= 4 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of HT for jet multiplicities >= 1 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of HT for jet multiplicities >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of HT for jet multiplicities >= 3 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of HT for jet multiplicities >= 4 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the invariant mass of the first+second jets for jet multiplicites >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the invariant mass of the first+second+third jets for jet multiplicites >= 3 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the invariant mass of the first+second+third+fourth jets for jet multiplicites >= 4 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the rapidity of the first jet in the event for jet multiplicities >= 1 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the DeltaR(first jet,second jet) for jet multiplicites >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the |y(lepton)-y(first jet)| for jet multiplicites >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the |y(first jet)+y(second jet)| for jet multiplicites >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the |y(first jet)-y(second jet)| for jet multiplicites >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the |phi(first jet)-phi(second jet)| for jet multiplicites >= 2 and jet PT > 30 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The predicted W+jets cross section as a function of the jet multiplicity for jet PT > 30 GeV.

The predicted W+jets cross section ratio as a function of jet multiplicty for jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 1 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 2 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 3 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 4 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 2 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 3 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 4 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the third jet in the event for jet multiplicities >= 3 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the third jet in the event for jet multiplicities >= 4 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the pT of the fourth jet in the event for jet multiplicities >= 4 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of HT for jet multiplicities >= 1 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of HT for jet multiplicities >= 2 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of HT for jet multiplicities >= 3 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of HT for jet multiplicities >= 4 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the invariant mass of the first+second jets for jet multiplicites >= 2 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the invariant mass of the first+second+third jets for jet multiplicites >= 3 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the invariant mass of the first+second+third+fourth jets for jet multiplicites >= 4 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the rapidity of the first jet in the event for jet multiplicities >= 1 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the DeltaR(first jet,second jet) for jet multiplicites >= 2 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the |y(lepton)-y(first jet)| for jet multiplicites >= 2 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the |y(first jet)+y(second jet)| for jet multiplicites >= 2 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the |y(first jet)-y(second jet)| for jet multiplicites >= 2 and jet PT > 30 GeV.

The predicted W+jets cross section as a function of the |phi(first jet)-phi(second jet)| for jet multiplicites >= 2 and jet PT > 30 GeV.

The measured W+jets cross section as a function of the jet multiplicity for jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section ratio as a function of jet multiplicty for jet PT > 20 GeV.

The measured W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 1 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 3 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 4 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 3 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 4 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the third jet in the event for jet multiplicities >= 3 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the third jet in the event for jet multiplicities >= 4 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the pT of the fourth jet in the event for jet multiplicities >= 4 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of HT for jet multiplicities >= 1 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of HT for jet multiplicities >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of HT for jet multiplicities >= 3 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of HT for jet multiplicities >= 4 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the invariant mass of the first+second jets for jet multiplicites >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the invariant mass of the first+second+third jets for jet multiplicites >= 3 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the invariant mass of the first+second+third+fourth jets for jet multiplicites >= 4 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the rapidity of the first jet in the event for jet multiplicities >= 1 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the DeltaR(first jet,second jet) for jet multiplicites >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the |y(lepton)-y(first jet)| for jet multiplicites >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the |y(first jet)+y(second jet)| for jet multiplicites >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the |y(first jet)-y(second jet)| for jet multiplicites >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The measured W+jets cross section as a function of the |phi(first jet)-phi(second jet)| for jet multiplicites >= 2 and jet PT > 20 GeV shown for "Born" leptons and for QED corrected "dressed" leptons.

The predicted W+jets cross section as a function of the jet multiplicity for jet PT > 20 GeV.

The predicted W+jets cross section ratio as a function of jet multiplicty for jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 1 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 2 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 3 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the first jet in the event for jet multiplicities >= 4 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 2 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 3 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the second jet in the event for jet multiplicities >= 4 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the third jet in the event for jet multiplicities >= 3 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the third jet in the event for jet multiplicities >= 4 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the pT of the fourth jet in the event for jet multiplicities >= 4 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of HT for jet multiplicities >= 1 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of HT for jet multiplicities >= 2 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of HT for jet multiplicities >= 3 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of HT for jet multiplicities >= 4 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the invariant mass of the first+second jets for jet multiplicites >= 2 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the invariant mass of the first+second+third jets for jet multiplicites >= 3 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the invariant mass of the first+second+third+fourth jets for jet multiplicites >= 4 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the rapidity of the first jet in the event for jet multiplicities >= 1 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the DeltaR(first jet,second jet) for jet multiplicites >= 2 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the |y(lepton)-y(first jet)| for jet multiplicites >= 2 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the |y(first jet)+y(second jet)| for jet multiplicites >= 2 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the |y(first jet)-y(second jet)| for jet multiplicites >= 2 and jet PT > 20 GeV.

The predicted W+jets cross section as a function of the |phi(first jet)-phi(second jet)| for jet multiplicites >= 2 and jet PT > 20 GeV.

Normalised fiducial cross section in bins of the leading lepton PT. Leading Lepton is the lepton in the final state with highest PT.

Correlations in the leading Lepton PT distribution.