{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.76554.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1491950"}},{"@id":"https://doi.org/10.1103/PhysRevD.95.092001","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2017","description":"Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at 13 TeV are measured as a function of jet multiplicity and of kinematic variables of the top quarks and the top quark-antiquark system. This analysis is based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 2.3/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron in the final state. The differential cross sections are presented at particle level, within a phase space close to the experimental acceptance, and at parton level in the full phase space. The results are compared to several standard model predictions.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t1","@type":"Dataset","description":"Absolute cross section at particle level.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t2","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t3","@type":"Dataset","description":"Absolute cross section at particle level.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t4","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t5","@type":"Dataset","description":"Absolute cross section at particle level.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t6","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t7","@type":"Dataset","description":"Absolute cross section at particle level.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t8","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t9","@type":"Dataset","description":"Absolute cross section at particle level.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t10","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t11","@type":"Dataset","description":"Absolute cross section at particle level.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t12","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level.","name":"Table 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156"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t157","@type":"Dataset","description":"Normalized cross section at parton level.","name":"Table 157"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t158","@type":"Dataset","description":"Normalized cross section at parton level.","name":"Table 158"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t159","@type":"Dataset","description":"Covariance matrix of normalized cross section at parton level.","name":"Table 159"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t160","@type":"Dataset","description":"Normalized cross section at parton level.","name":"Table 160"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t161","@type":"Dataset","description":"Normalized cross section at parton level.","name":"Table 161"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t162","@type":"Dataset","description":"Normalized cross section at parton level.","name":"Table 162"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t163","@type":"Dataset","description":"Normalized cross section at parton level.","name":"Table 163"},{"@id":"https://doi.org/10.17182/hepdata.76554.v1/t164","@type":"Dataset","description":"Covariance matrix of normalized cross section at parton level.","name":"Table 164"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1491950?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/76554"}],"inLanguage":"en","name":"Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1491950?version=1","version":1}