{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.91267.v1/t21","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1742785"}},{"@id":"https://doi.org/10.1140/epjc/s10052-019-7399-7","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2020","description":"Measured fiducial cross-section ratio R_{W+-/Z} = sigma (W+/- -> l+/- nu/nubar) / sigma (Z/gamma^* -> l+ l-) where l =...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/520786/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/520786/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/520786/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/520786/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/520786/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1742785?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/91267"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.91267.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1742785?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.91267.v1","@type":"Dataset","description":"CERN-LHC. The production cross-sections for W\u00b1 and Z bosons are measured using ATLAS data corresponding to an integrated luminosity of 4.0 pb\u22121\ncollected at a centre-of-mass energy sqrt(s) = 2.76 TeV. The decay channels W->lnu and Z->ll are used, where l can be an electron or a muon. \nThe cross-sections are presented for a fiducial region defined by the detector acceptance and are also extrapolated to the full phase space \nfor the total inclusive production cross-section. The combined (average) total inclusive cross-sections for the electron and muon channels are:\nsigma_tot(W^+ -> lnu) = 2312 \u00b1 26(stat.) \u00b1 27(syst.) \u00b1 72(lumi.) \u00b130 (extr.)pb,\nsigma_tot(W^- -> lnu) = 1399 \u00b1 21(stat.) \u00b1 17(syst.) \u00b1 43(lumi.) \u00b121 (extr.)pb,\nsigma_tot(Z -> ll) = 323.4 \u00b1 9.8(stat.) \u00b1 5.0(syst.) \u00b110.0(lumi.) \u00b1 5.5(extr.)pb.\nMeasured ratios and asymmetries constructed using these cross-sections are also presented. These observables benefit from full or partial cancellation \nof many systematic uncertainties that are correlated between the different measurements.\n\nW-boson fiducial region is defined as:\n- ptLepton > 20 GeV \n- |etaLepton| < 2.4\n- MET > 25 GeV\n- mT > 40GeV\n\nZ-boson fiducial region is defined as:\n- ptLepton > 20 GeV\n- |etaLepton| < 2.4\n- 66 < |mll| < 116 GeV","name":"Measurement of $W^{\\pm}$-boson and $Z$-boson production cross-sections in $pp$ collisions at $\\sqrt{s}=2.76$ TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins1742785?version=1"},"keywords":"P P --> W+ X, P P --> W- X, P P --> Z0 X, P P --> GAMMA* X, SIG, 2760.0, Inclusive, Integrated Cross Section, Cross Section, Cross-Section Ratio, Proton-Proton Scattering, W Production, Z Production","name":"Table 21","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/93204","version":1}