{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79411.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1382594"}},{"@id":"https://doi.org/10.1140/epjc/s10052-016-4219-1","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"CERN-LHC. Measurement of the W boson pair production cross section in proton-proton collisions at sqrt(s) = 8 TeV. The data     \ncollected with the CMS detector at the LHC correspond to an integrated luminosity of 19.4/fb. The W+W- candidates are\nselected from events with two charged leptons, electrons or muons, and large missing transverse energy. The fiducial and the    \nnormalized differential cross section is also measured as a function of kinematic variables of the final-state charged leptons. \nLimits on anomalous gauge couplings associated with dimension-six operators are also given in the framework of an effective \nfield theory.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t1","@type":"Dataset","description":"The W+W- production cross section combining the four event categories (different-flavor and same-flavor in the 0-jet and 1-jet bin separately)...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t2","@type":"Dataset","description":"The W+W- production cross section in fiducial regions defined by requiring no jets at particle level with jet pT thresholds...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t3","@type":"Dataset","description":"The W+W- production cross section in fiducial regions defined by requiring zero jets at particle level with varying jet pT...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t4","@type":"Dataset","description":"Normalized differential W+W- cross section as a function of the leading lepton pT. Both statistical and systematic uncertainties are included....","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t5","@type":"Dataset","description":"Normalized differential W+W- cross section as a function of the dilepton system. Both statistical and systematic uncertainties are included. Results...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t6","@type":"Dataset","description":"Normalized differential W+W- cross section as a function of the invariant mass. Both statistical and systematic uncertainties are included. Results...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t7","@type":"Dataset","description":"Normalized differential W+W- cross section as a function of the angular separation between leptons. Both statistical and systematic uncertainties are...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t8","@type":"Dataset","description":"Measured cWWW/LAMBDA^2, cW/LAMBDA^2, and cB/LAMBDA^2 coupling constants.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.79411.v1/t9","@type":"Dataset","description":"Measured 95% CL interval of the cWWW/LAMBDA^2, cW/LAMBDA^2, and cB/LAMBDA^2 coupling constants.","name":"Table 9"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1382594?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79411"}],"inLanguage":"en","name":"Measurement of the W+ W- cross section in pp collisions at sqrt(s) = 8 TeV and limits on anomalous gauge couplings","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1382594?version=1","version":1}