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.

pT-differential yield of prompt D/s+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 0-10% in the rapidity interval |y|<0.5. Branching ratio of Ds->phipi->KKpi : 0.0227.

pT-differential yield of prompt D0 mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5. Branching ratio of D0->Kpi : 0.0393.

pT-differential yield of prompt D+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5. Branching ratio of D+->Kpipi : 0.0946.

pT-differential yield of prompt D*+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5. Branching ratio of D*+->D0pi->Kpipi : 0.0393*0.677.

pT-differential yield of prompt D/s+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5. Branching ratio of Ds->phipi->KKpi : 0.0227.

pT-differential yield of prompt D0 mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5. Branching ratio of D0->Kpi : 0.0393.

pT-differential yield of prompt D+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5. Branching ratio of D+->Kpipi : 0.0946.

pT-differential yield of prompt D*+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5. Branching ratio of D*+->D0pi->Kpipi : 0.0393*0.677.

pT-differential yield of prompt D/s+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5. Branching ratio of Ds->phipi->KKpi : 0.0227.

Ratio of D+ to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 0-10% centrality, in |y| < 0.5 as a function of pT. Branching ratio of D+->Kpipi : 0.0946. Branching ratio of D0->Kpi : 0.0393.

Ratio of D*+ to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 0-10% centrality, in |y| < 0.5 as a function of pT. Branching ratio of D*+->D0pi->Kpipi : 0.0393*0.677. Branching ratio of D0->Kpi : 0.0393.

Ratio of Ds to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 0-10% centrality, in |y| < 0.5 as a function of pT. Branching ratio of Ds->phipi->KKpi : 0.0227. Branching ratio of D0->Kpi : 0.0393.

Ratio of Ds to D+ meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 0-10% centrality, in |y| < 0.5 as a function of pT. Branching ratio of Ds->phipi->KKpi : 0.0227. Branching ratio of D+->Kpipi : 0.0946.

Ratio of D+ to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 30-50% centrality, in |y| < 0.5 as a function of pT. Branching ratio of D+->Kpipi : 0.0946. Branching ratio of D0->Kpi : 0.0393.

Ratio of D*+ to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 30-50% centrality, in |y| < 0.5 as a function of pT. Branching ratio of D*+->D0pi->Kpipi : 0.0393*0.677. Branching ratio of D0->Kpi : 0.0393.

Ratio of Ds to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 30-50% centrality, in |y| < 0.5 as a function of pT. Branching ratio of Ds->phipi->KKpi : 0.0227. Branching ratio of D0->Kpi : 0.0393.

Ratio of Ds to D+ meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 30-50% centrality, in |y| < 0.5 as a function of pT. Branching ratio of Ds->phipi->KKpi : 0.0227. Branching ratio of D+->Kpipi : 0.0946.

Ratio of D+ to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 60-80% centrality, in |y| < 0.5 as a function of pT. Branching ratio of D+->Kpipi : 0.0946. Branching ratio of D0->Kpi : 0.0393.

Ratio of D*+ to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 60-80% centrality, in |y| < 0.5 as a function of pT. Branching ratio of D*+->D0pi->Kpipi : 0.0393*0.677. Branching ratio of D0->Kpi : 0.0393.

Ratio of Ds to D0 meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 60-80% centrality, in |y| < 0.5 as a function of pT. Branching ratio of Ds->phipi->KKpi : 0.0227. Branching ratio of D0->Kpi : 0.0393.

Ratio of Ds to D+ meson yield in Pb-Pb collisions at sqrt{sNN}=5.02 TeV, 60-80% centrality, in |y| < 0.5 as a function of pT. Branching ratio of Ds->phipi->KKpi : 0.0227. Branching ratio of D+->Kpipi : 0.0946.

pT-differential nuclear modification factor of prompt D0 mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 0-10% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 0-10% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D*+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 0-10% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D/s+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 0-10% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of average prompt D0, D+, D*+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 0-10% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D0 mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D*+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D/s+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of average prompt D0, D+, D*+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 30-50% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D0 mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D*+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of prompt D/s+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of average prompt D0, D+, D*+ mesons in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the centrality class 60-80% in the rapidity interval |y|<0.5.

pT-differential nuclear modification factor of average prompt D0, D+, D*+ mesons in Pb-Pb collisions at sqrt{sNN}=2.76 TeV in the centrality class 0-10% in the rapidity interval |y|<0.5.

Ratio of prompt D meson (D0, D+, D*+ average) and charged particles nuclear modification factors (RAA) as a function of pT for D mesons with |y|<0.5 and charged particles with |eta|<0.8, measured in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the 0-10% centrality class.

Ratio of prompt D meson (D0, D+, D*+ average) and charged particles nuclear modification factors (RAA) as a function of pT for D mesons with |y|<0.5 and charged particles with |eta|<0.8, measured in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the 30-50% centrality class.

Ratio of prompt D meson (D0, D+, D*+ average) and charged particles nuclear modification factors (RAA) as a function of pT for D mesons with |y|<0.5 and charged particles with |eta|<0.8, measured in Pb-Pb collisions at sqrt{sNN}=5.02 TeV in the 60-80% centrality class.

$K^{0}_{S}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class I+II (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class III+IV (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class V+VI (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class VII+VIII (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class IX+X (pp at $\sqrt{s}=7$ TeV).

$2K^{0}_{S}/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Lambda+\bar{\Lambda})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Xi^{-}+\bar{\Xi}^{+})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Omega^{-}+\bar{\Omega}^{+})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$\pi^{+}+\pi^{-}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$p+\bar{p}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$K^{0}_{S}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Lambda+\bar{\Lambda}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Xi^{-}+\bar{\Xi}^{+}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Omega^{-}+\bar{\Omega}^{+}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$(\Lambda+\bar{\Lambda})/2K^{0}_{S}$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of charged particle multiplicity density at midrapidity.

$(p+\bar{p})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of charged particle multiplicity density at midrapidity.

$(2K^{0}_{S})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Lambda+\bar{\Lambda})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Xi^{-}+\bar{\Xi}^{+})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Omega^{-}+\bar{\Omega}^{+})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

Event multiplicity classes, their corresponding fraction of the INEL>0 cross-section and their corresponding average charged particle density at midrapidity ($|\eta|<0.5$). The value of in the inclusive (INEL>0) class is 5.96 $\pm$ 0.23. The uncertainties are the quadratic sum of statistical and systematic contributions.