{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.85696.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1663958"}},{"@id":"https://doi.org/10.1103/PhysRevD.97.112003","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"Differential and double-differential cross sections for the production of top quark pairs in proton-proton collisions at sqrt{s} = 13 TeV are measured as a function of kinematic variables of the top quarks and the top quark-antiquark (ttbar) system. In addition, kinematic variables and multiplicities of jets associated with the ttbar production are measured. This analysis is based on data collected by the CMS experiment at the LHC in 2016 corresponding to an integrated luminosity of 35.8/fb. The measurements are performed in the lepton+jets decay channels with a single muon or electron and jets in the final state. The differential cross sections are presented at the particle level, within a phase space close to the experimental acceptance, and at the parton level in the full phase space. The results are compared to several standard model predictions that use different methods and approximations. The kinematic variables of the top quarks and the ttbar system are reasonably described in general, though none predict all the measured distributions. In particular, the transverse momentum distribution of the top quarks is more steeply falling than predicted. The kinematic distributions and multiplicities of jets are adequately modeled by certain combinations of next-to-leading-order calculations and parton shower models.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t1","@type":"Dataset","description":"Absolute cross section at particle level as a function of $p_\\text{T}(\\text{t}_\\text{h})$.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t2","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level as a function of $p_\\text{T}(\\text{t}_\\text{h})$.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t3","@type":"Dataset","description":"Absolute cross section at particle level as a function of $|y(\\text{t}_\\text{h})|$.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t4","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level as a function of $|y(\\text{t}_\\text{h})|$.","name":"Table 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$M(\\text{t}\\bar{\\text{t}})$.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t10","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level as a function of $M(\\text{t}\\bar{\\text{t}})$.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t11","@type":"Dataset","description":"Absolute cross section at particle level as a function of $p_\\text{T}(\\text{t}\\bar{\\text{t}})$.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t12","@type":"Dataset","description":"Covariance matrix of absolute cross section at particle level as a function of $p_\\text{T}(\\text{t}\\bar{\\text{t}})$.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t13","@type":"Dataset","description":"Absolute cross section at particle level as a function of $|y(\\text{t}\\bar{\\text{t}})|$.","name":"Table 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$p_\\text{T}(\\text{t}_\\text{h})$.","name":"Table 194"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t195","@type":"Dataset","description":"Absolute cross section at the parton level as a function of $|y(\\text{t}_\\text{h})|$ vs. $p_\\text{T}(\\text{t}_\\text{h})$.","name":"Table 195"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t196","@type":"Dataset","description":"Covariance matrix of absolute cross section at the parton level as a function of $|y(\\text{t}_\\text{h})|$ vs. $p_\\text{T}(\\text{t}_\\text{h})$.","name":"Table 196"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t197","@type":"Dataset","description":"Absolute cross section at the parton level as a function of $M(\\text{t}\\bar{\\text{t}})$ vs. $|y(\\text{t}\\bar{\\text{t}})|$.","name":"Table 197"},{"@id":"https://doi.org/10.17182/hepdata.85696.v2/t198","@type":"Dataset","description":"Absolute cross section at the parton level as a function of $M(\\text{t}\\bar{\\text{t}})$ vs. 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