Fiducial differential cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $N_{\mathrm{gap}\,\mathrm{jets}}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 14.

Fiducial differential cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 15.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\ell\ell}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 16.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{T}}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 17.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{jj}}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 18.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $N_{\mathrm{gap}\,\mathrm{jets}}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 19.

Fiducial differential cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$. The correlation of uncertainties of the measured cross section across bins is presented in Table 20.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\ell\ell}$. See Table 1.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{T}}$. See Table 2.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{jj}}$. See Table 3.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $N_{\mathrm{gap}\,\mathrm{jets}}$. See Table 4.

Observed correlations between the bins of the LH-unfolded cross section of the electroweak $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$. See Table 5.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\ell\ell}$. See Table 6.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{T}}$. See Table 7.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $m_{\mathrm{jj}}$. See Table 8.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $N_{\mathrm{gap}\,\mathrm{jets}}$. See Table 9.

Observed correlations between the bins of the LH-unfolded cross section of the inclusive $W^\pm W^\pm jj$ production as a function of $\xi_{\mathrm{j}3}$. See Table 10.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label M0 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label M1 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label M7 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient. The limits on M7 were obtained without taking into account the SM-EFT interference for the EW W$^\pm$Zjj final state.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label S02 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label S1 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label T0 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label T1 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Evolution of the one-dimensional expected and observed limits at 95% CL on the parameters corresponding to the quartic operators with label T2 as a function of the cut-off scale. The unitarity bounds as a function of the cut-off scale are defined for one non-zero Wilson coefficient.

Expected and observed exclusion limits at 95% CL for $\sigma_{\mathrm{VBF}}(\mathrm{H}^{\pm\pm}_5) \times \mathcal{B}(\mathrm{H}^{\pm\pm}_5 \rightarrow W^{\pm}W^{\pm})$ as a function of the doubly-charged Higgs mass.

Expected and observed exclusion limits at 95% CL for $\sin\theta_{\mathrm{H}}$ as a function of the doubly-charged Higgs mass in the Georgi-Machacek model.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the inclusive jet multiplicity.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the inclusive jet multiplicity.

Differential cross section for the production of W bosons as a function of H_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of H_T for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the H_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the H_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the H_T for events with N_jets ≥ 1.

Differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the W p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the W p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the W p_T for events with N_jets ≥ 1.

Differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the leading jet p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the leading jet rapidity for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Differential cross section for the production of W bosons as a function of second leading jet p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of second leading jet p_T for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of Δ R_jet1,jet2 for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of Δ R_jet1,jet2 for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of dijet invariant mass for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of dijet invariant mass for events with N_jets ≥ 2.

Cross section for the production of W bosons as a function of exclusive jet multiplicity.

Statistical correlation between bins in data for the cross section for the production of W bosons as a function of exclusive jet multiplicity.

Differential cross section for the production of W bosons as a function of the H_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the H_T for events with N_jets ≥ 2.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the H_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the H_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the H_T for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 2.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the W p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the W p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the W p_T for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the leading jet p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Differential cross section for the production of W bosons as a function of the electron η for events with N_jets ≥ 0.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the electron η for events with N_jets ≥ 0.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the electron η for events with N_jets ≥ 0.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the electron η for events with N_jets ≥ 0.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the electron η for events with N_jets ≥ 0.

Differential cross section for the production of W bosons as a function of the electron η for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross section for the production of W bosons as a function of the electron η for events with N_jets ≥ 1.

Differential cross sections for the production of W⁺ bosons, W^- bosons and the W⁺/W^- cross section ratio as a function of the electron η for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W⁺ bosons as a function of the electron η for events with N_jets ≥ 1.

Statistical correlation between bins in data for the differential cross sections for the production of W^- bosons as a function of the electron η for events with N_jets ≥ 1.

List of experimentally considered systematic uncertainties for the W+jets cross section measurement

Non-perturbative corrections for the cross section for the production of W bosons for different inclusive jet multiplicities.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the inclusive jet multiplicity.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of H_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the H_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the W p_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet rapidity for events with N_jets ≥ 1.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of second leading jet p_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of second leading jet rapidity for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of Δ R_jet1,jet2 for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of dijet invariant mass for events with N_jets ≥ 2.

Non-perturbative corrections for the cross section for the production of W bosons as a function of exclusive jet multiplicity.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the H_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the H_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the W p_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the W p_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross section for the production of W bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

Non-perturbative corrections for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 2.

NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the H_T for events with N_jets ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].

NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the W p_T for events with N_jets ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].

NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet p_T for events with N_jets ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].

NNLO/NLO k-factors determined with NNLO Njetti for the differential cross sections for the production of W⁺ bosons and W^- bosons as a function of the leading jet rapidity for events with N_jets ≥ 1. These numbers were obtained with code described in Phys. Rev. Lett. 115 (2015) 062002 [arXiv:1504.02131].

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.

Correlated Systematic Uncertainties for W- production.

Cross sections for W+ production from the combined electron and muon data sets in the defined fiducial regions. The first (sys) error is the uncorrelated systematic error and the second is the correlated systematic error.

Correlated Systematic Uncertainties for W+ production.

Combined lepton charge asymmetry from W boson decays.

Fiducial cross sections of Z0 versus W+ from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W+ space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Fiducial cross sections of Z0 versus W- from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W- space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Fiducial cross sections of Z0 versus W+- from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W+- space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Fiducial cross sections of W- versus W+ from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in W- W+ space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Total cross sections of Z0 versus W+ from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W+ space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Total cross sections of Z0 versus W- from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W- space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Total cross sections of Z0 versus W+- from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in Z0 W+- space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Total cross sections of W- versus W+ from fitting the combined electron and muon decay data sets. The table shows the fitted ellipse centre in W- W+ space plus the ellipse radii and angle using the total uncertainties and only the experimental uncertainties.

Factors to correct the measured cross-sections for different treatments of photon final-state radiation (QED FSR) to: - dressed leptons, recombined with FSR photons in a cone of DeltaR < 0.1 and - bare leptons, defined after FSR. These correction factors are found to be (pseudo)-rapidity independent.

Theory prediction from FEWZ program at NNLO QCD for fiducial Z0 production cross section times leptonic branching using different PDF sets. The first error (stat) is the numerical statistical uncertainty of the calculation, while second and third give the asymmetric uncertainty from the PDF set.

Theory prediction from FEWZ program at NNLO QCD for total Z0 production cross section times leptonic branching using different PDF sets. The first error (stat) is the numerical statistical uncertainty of the calculation, while second and third give the asymmetric uncertainty from the PDF set.

Theory prediction from FEWZ program at NNLO QCD for fiducial W+ + W- production cross section times leptonic branching using different PDF sets. The first error (stat) is the numerical statistical uncertainty of the calculation, while second and third give the asymmetric uncertainty from the PDF set.

Theory prediction from FEWZ program at NNLO QCD for total W+ + W- production cross section times leptonic branching using different PDF sets. The first error (stat) is the numerical statistical uncertainty of the calculation, while second and third give the asymmetric uncertainty from the PDF set.

The measured cross section ratio for W+jets in the muon channel as a function of corrected jet multiplicity.

The cross section times branching ratio for W+jets in the electron channel as a function of the leading jet PT.

The cross section times branching ratio for W+jets in the muon channel as a function of the leading jet PT.

The cross section times branching ratio for W+jets in the electron channel as a function of the next-to-leading jet PT.

The cross section times branching ratio for W+jets in the muon channel as a function of the next-to-leading jet PT.

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).