{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89879.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1705068"}},{"@id":"https://doi.org/10.1140/epjc/s10052-019-6752-1","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2020","description":"CERN-LHC. Measurements are presented of associated production of a W boson and a charm quark (W + c) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data correspond to an integrated luminosity of 35.7 fb\u22121 collected by the CMS experiment at the CERN LHC. The W bosons are identified by their decay into a muon and a neutrino. The charm quarks are tagged via the full reconstruction of D\u2217(2010) mesons that decay via D\u2217(2010) --> D0 + pi \\to K + pi + pi. A cross section is measured in the fiducial region defined by the muon transverse momentum pT(\\mu) > 26 GeV, muon pseudorapidity |\\eta(\\mu)| < 2.4, and charm quark transverse momentum pT(c) > 5 GeV. The cross section is also measured differentially as a function of the pseudorapidity of the muon from the W boson decay, presented separately for W+, W- and the combination. The W + D\u2217(2010) cross section is determined with the additional constraint of |\\eta(D*)| < 2.4 and without imposing restrictions on the origin of the D\u2217(2010) meson.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.89879.v1/t1","@type":"Dataset","description":"The differential measurement of W + charm as a function of the absolute peudorapidity of the muon originating from the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.89879.v1/t2","@type":"Dataset","description":"The differential measurement of W+ + cbar as a function of the absolute peudorapidity of the muon originating from the...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.89879.v1/t3","@type":"Dataset","description":"The differential measurement of W- + c as a function of the absolute peudorapidity of the muon originating from the...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.89879.v1/t4","@type":"Dataset","description":"The differential measurement of W + D*(2010) as a function of the absolute peudorapidity of the muon originating from the...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.89879.v1/t5","@type":"Dataset","description":"The differential measurement of W+ + D*(2010)- as a function of the absolute peudorapidity of the muon originating from the...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.89879.v1/t6","@type":"Dataset","description":"The differential measurement of W- + D*(2010)+ as a function of the absolute peudorapidity of the muon originating from the...","name":"Table 6"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1705068?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/89879"}],"inLanguage":"en","name":"Measurement of associated production of a W boson and a charm quark in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1705068?version=1","version":1}