Comparison of the shapes extrapolated with a linear or quadratic extrapolation of the QCD contribution in the W+ signal region.

Comparison of the shapes extrapolated with a linear or quadratic extrapolation of the QCD contribution in the W- signal region.

Post-fit distributions of the transverse mass in the W+ signal region.

Post-fit distributions of the transverse mass in the W- signal region.

Post-fit distributions of the dimuon mass in the Z boson signal region.

Example plot for the extrapolation of the QCD contribution from a region with inverted relative isolation criterion to the W+ signal region in the transverse mass bin 12 < mT < 18 GeV. The values corresponding to the smallest relative muon isolation are extrapolated with a linear (smaller value) and quadratic (larger value) function.

Example plot for the extrapolation of the QCD contribution from a region with inverted relative isolation criterion to the W- signal region in the transverse mass bin 12 < mT < 18 GeV.The values corresponding to the smallest relative muon isolation are extrapolated with a linear (smaller value) and quadratic (larger value) function.

Example plot for the extrapolation of the QCD contribution from a region with inverted relative isolation criterion to the W+ signal region in the transverse mass bin 102 < mT < 108 GeV.The values corresponding to the smallest relative muon isolation are extrapolated with a linear (larger value) and quadratic (smaller value) function.

Example plot for the extrapolation of the QCD contribution from a region with inverted relative isolation criterion to the W- signal region in the transverse mass bin 102 < mT < 108 GeV.The values corresponding to the smallest relative muon isolation are extrapolated with a linear (smaller value) and quadratic (larger value) function.

The table compares theoretical and measured values of the product of the fiducial cross sections and branching fractions. The theoretical predictions are generated with DYTurbo in combination with three different PDF sets. All values are normalized to the corresponding measured value. The relative uncertainties on the measured values are given separately with and without the contribution from the luminosity uncertainty.

The table compares theoretical and measured values of the product of the total cross sections and branching fractions. The theoretical predictions are generated with DYTurbo in combination with three different PDF sets. All values are normalized to the corresponding measured value. The relative uncertainties on the measured values are given separately with and without the contribution from the luminosity uncertainty.

The table compares theoretical and measured ratios of the product of the fiducial cross sections and branching fractions. The theoretical predictions are generated with DYTurbo in combination with three different PDF sets. All values are normalized to the corresponding measured value.

The table compares theoretical and measured ratios of the product of the total cross sections and branching fractions. The theoretical predictions are generated with DYTurbo in combination with three different PDF sets. All values are normalized to the corresponding measured value.

Comparison of the measured and theoretical cross sections for Z, W+, W-, and W production at different center-of-mass energies. The theoretical predictions are generated with DYTurbo in combination with the NNPDF 3.1 PDF set.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $180 < p_{\mathrm{T,jet}} < 200$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $120 < p_{\mathrm{T,jet}} < 140$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $140 < p_{\mathrm{T,jet}} < 160$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $160 < p_{\mathrm{T,jet}} < 180$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $180 < p_{\mathrm{T,jet}} < 200$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $120 < p_{\mathrm{T,jet}} < 140$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $140 < p_{\mathrm{T,jet}} < 160$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $160 < p_{\mathrm{T,jet}} < 180$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $180 < p_{\mathrm{T,jet}} < 200$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $120 < p_{\mathrm{T,jet}} < 140$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $140 < p_{\mathrm{T,jet}} < 160$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $160 < p_{\mathrm{T,jet}} < 180$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator distributions constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $180 < p_{\mathrm{T,jet}} < 200$ GeV. The results are shown for different centrality bins in PbPb collisions and for pp collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $120 < p_{\mathrm{T,jet}} < 140$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $140 < p_{\mathrm{T,jet}} < 160$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $160 < p_{\mathrm{T,jet}} < 180$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $180 < p_{\mathrm{T,jet}} < 200$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $120 < p_{\mathrm{T,jet}} < 140$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $140 < p_{\mathrm{T,jet}} < 160$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $160 < p_{\mathrm{T,jet}} < 180$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 1$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $180 < p_{\mathrm{T,jet}} < 200$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $120 < p_{\mathrm{T,jet}} < 140$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $140 < p_{\mathrm{T,jet}} < 160$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $160 < p_{\mathrm{T,jet}} < 180$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=1$ and jet $p_{\mathrm{T}}$ selection $180 < p_{\mathrm{T,jet}} < 200$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $120 < p_{\mathrm{T,jet}} < 140$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $140 < p_{\mathrm{T,jet}} < 160$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $160 < p_{\mathrm{T,jet}} < 180$ GeV. The results are shown for different centrality bins in PbPb collisions.

The energy-energy correlator PbPb/pp ratios constructed with charged particles with $p_{\mathrm{T}} > 2$ GeV for energy weight $n=2$ and jet $p_{\mathrm{T}}$ selection $180 < p_{\mathrm{T,jet}} < 200$ GeV. The results are shown for different centrality bins in PbPb collisions.

The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ > 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ > 1 GeV.

The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ > 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ > 1 GeV.

The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ > 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ > 1 GeV.

The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ > 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ > 1 GeV.

The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ > 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ > 1 GeV.

The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ > 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ > 1 GeV.

The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ > 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ > 1 GeV.

The double ratios of PbPb to pp single ratios with $p_{\mathrm{T}}^{\mathrm{ch}}$ > 2 GeV and $p_{\mathrm{T}}^{\mathrm{ch}}$ > 1 GeV.