{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.153468.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2816048"}},{"@id":"https://doi.org/10.1007/JHEP04(2025)162","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2024","description":"Measurements of fiducial and total inclusive cross sections for W and Z boson production are presented in proton-proton collisions at $\\sqrt{s}$ = 5.02 and 13 TeV. Electron and muon decay modes ($\\ell$ = e or $\\mu$) are studied in the data collected with the CMS detector in 2017, in dedicated runs with reduced instantaneous luminosity. The data sets correspond to integrated luminosities of 298 $\\pm$ 6 pb$^{-1}$ at 5.02 TeV and 206 $\\pm$ 5 pb$^{-1}$ at 13 TeV. Measured values of the products of the total inclusive cross sections and the branching fractions at 5.02 TeV are $\\sigma$(pp $\\to$ W+X) $\\mathcal{B}$(W $\\to$$\\ell\\nu$) = 7300 $\\pm$ 10 (stat) $\\pm$ 60 (syst) $\\pm$ 140 (lumi) pb, and $\\sigma$(pp $\\to$ Z+X) $\\mathcal{B}$(Z $\\to$$\\ell^+\\ell^-$) = 669 $\\pm$ 2 (stat) $\\pm$ 6 (syst) $\\pm$ 13 (lumi) pb for the dilepton invariant mass in the range of 60-120 GeV. The corresponding results at 13 TeV are 20480 $\\pm$ 10 (stat) $\\pm$ 170 (syst) $\\pm$ 470 (lumi) pb and 1952 $\\pm$ 4 (stat) $\\pm$ 18 (syst) $\\pm$ 45 (lumi) pb. The measured values agree with cross section calculations at next-to-next-to-leading-order in perturbative quantum chromodynamics. Fiducial and total inclusive cross sections, ratios of cross sections of W$^+$ and W$^-$ production as well as inclusive W and Z boson production, and ratios of these measurements at 5.02 and 13 TeV are reported.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.153468.v1/t1","@type":"Dataset","description":"Distributions of $m_T$ in the $W^{+}$ signal selection for e final states for the pp collisions at $\\sqrt{s}=$ 5TeV after...","name":"Figure 1-a"},{"@id":"https://doi.org/10.17182/hepdata.153468.v1/t2","@type":"Dataset","description":"Distributions of $m_T$ in the $W^{+}$ signal selection for mu final states for the pp collisions at $\\sqrt{s}=$ 5TeV after...","name":"Figure 1-b"},{"@id":"https://doi.org/10.17182/hepdata.153468.v1/t3","@type":"Dataset","description":"Distributions of $m_T$ in the $W^{+}$ signal selection for e final states for the pp collisions at $\\sqrt{s}=$ 13TeV after...","name":"Figure 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