{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.181097.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/3123908"}}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2026","description":"Measurements of the production of the W$^{\\pm}$ and Z$^0$ bosons at midrapidity in pp collisions at $\\sqrt{s} = 13$ TeV with ALICE at the Large Hadron Collider (LHC) are presented. The W$^{\\pm}$ and Z$^0$ bosons are detected via their (di)electronic decay channels, with the electron reconstruction performed in the midrapidity region ($|y|< 0.6$). The $p_{\\rm T}$-integrated and $p_{\\rm T}$-differential production cross sections of electrons from W$^{\\pm}$ decays in the interval $30 < p_{\\rm T} < 60$ GeV/$c$, as well as the $p_{\\rm T}$-integrated production cross section of Z$^0$ bosons, are measured. The results are described by perturbative QCD calculations using different sets of parton distribution functions. The production of W$^{\\pm}$ bosons and azimuthally correlated associated hadrons is also measured as a function of the charged-particle multiplicity for the first time at the LHC. The former increases approximately linearly with the charged-particle multiplicity, while for the latter, there are hints of a faster-than-linear increase. These observations are compared with theoretical calculations.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.181097.v1/t1","@type":"Dataset","description":"Production cross section of $Z^{0}$ bosons in pp collisions at $\\sqrt{s}=$ 13 TeV within the acceptance of the ALICE central...","name":"Fig3"},{"@id":"https://doi.org/10.17182/hepdata.181097.v1/t2","@type":"Dataset","description":"Production cross section of electrons from W$^{-}$ decays as a function of $p_{\\rm T}$ at midrapidity in pp collisions at...","name":"Fig4"},{"@id":"https://doi.org/10.17182/hepdata.181097.v1/t3","@type":"Dataset","description":"Production cross section of positrons from W$^{+}$ decays as a function of $p_{\\rm T}$ at midrapidity in pp collisions at...","name":"Fig5"},{"@id":"https://doi.org/10.17182/hepdata.181097.v1/t4","@type":"Dataset","description":"Ratio of the W$^+$ to W$^-$ production cross section as a function of $p_{\\textrm{T}}$ at midrapidity in pp collisions at...","name":"Fig6"},{"@id":"https://doi.org/10.17182/hepdata.181097.v1/t5","@type":"Dataset","description":"Production cross section of positrons from W$^{+}$ decays at midrapidity in pp collisions at $\\sqrt{s}=$13 TeV. The production cross sections...","name":"Fig7_pos"},{"@id":"https://doi.org/10.17182/hepdata.181097.v1/t6","@type":"Dataset","description":"Production cross section of electrons from W$^{-}$ decays at midrapidity in pp collisions at $\\sqrt{s}=$13 TeV. The production cross sections...","name":"Fig7_ele"},{"@id":"https://doi.org/10.17182/hepdata.181097.v1/t7","@type":"Dataset","description":"Self-normalised yields of e$^{\\pm}$ $\\leftarrow$ W$^{\\pm}$ and associated hadrons as a function of the normalised charged-particle pseudorapidity density.","name":"Fig8"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins3123908?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/181097"}],"inLanguage":"en","name":"Measurements of the production of W$^{\\pm}$ and Z$^0$ bosons in pp collisions at $\\sqrt{s} = 13$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins3123908?version=1","version":1}