{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.61813.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1221252"}},{"@id":"https://doi.org/10.1103/PhysRevD.88.092001","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"D0 Collaboration"},"creator":{"@type":"Organization","name":"D0 Collaboration"},"datePublished":"2013","description":"Fermilab Tevatron. Comprehensive measurements of W ( via the e-nu decay mode ) + njet cross sections  from proton-antiproton interactions at a centre-of-mass energy of 1.96 TeV.  The  data used  has an integrated luminosity of 3.7 fb-1 with up to the production for 4 jets being studied for a wide range  of variables including transverse momentum, rapidity of the jets, dijet combinations, W boson and lepton.   As well as the tabulated cross sections, non-perturbative corrections to pQCD are given and also correlation  and covariance matrices for each table.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t1","@type":"Dataset","description":"Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of leading jet rapidity for events...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t2","@type":"Dataset","description":"Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of second jet rapidity for events...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t3","@type":"Dataset","description":"Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of third jet rapidity for events...","name":"Table 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normalized to the measured inclusive W boson cross-section, as a function of HT for events with two...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t32","@type":"Dataset","description":"Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of HT for events with three...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t33","@type":"Dataset","description":"Differential production cross-section, normalized to the measured inclusive W boson cross-section, as a function of HT for events with four...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t34","@type":"Dataset","description":"Average number of jets as a function of HT for events with one or more jets produced in association with...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t35","@type":"Dataset","description":"Average number of jets as a function of HT for events with two or more jets produced in association with...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t36","@type":"Dataset","description":"Average number of jets as a function of the rapidity separation between the two highest pT jets for events with...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t37","@type":"Dataset","description":"Average number of jets as a function of the rapidity separation between the two most rapidity separated jets for events...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t38","@type":"Dataset","description":"Probability of third jet emission as a function of the rapidity separation of the two highest pT jets for events...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.61813.v1/t39","@type":"Dataset","description":"Probability of third jet emission as a function of the rapidity separation of the two most rapidity-separated hard (pT>20 GeV)...","name":"Table 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at sqrt(s)=1.96 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1221252?version=1","version":1}