{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.76995.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1491953"}},{"@id":"https://doi.org/10.1103/PhysRevD.95.052002","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"CERN-LHC. Differential cross sections for a W boson produced in association with jets are measured in a data sample of proton-proton collisions at a center-of-mass energy of 8 TeV recorded with the CMS detector and corresponding to an integrated luminosity of 19.6 inverse femtobarns. The W bosons are identified through their decay into a muon and a neutrino. The cross sections are reported as functions of jet multiplicity, jet transverse momenta, and the scalar sum of jet transverse momenta (HT) for different jet multiplicities. Distributions of the angular correlations between the jets and the muon are examined, as well as the average number of jets as a function of HT and as a function of angular variables. The cross sections are measured in the fiducial region defined by a muon with pT > 25 GeV and pseudorapidity |eta| < 2.1, and by a transverse mass between the muon and the missing transverse energy MT > 50 GeV. Jets are reconstructed using the anti-kT algorithm with a distance parameter R = 0.5, and only jets with pT > 30 GeV, |eta| < 2.4, and a separation of deltaR > 0.5 from the muon are considered.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t1","@type":"Dataset","description":"The cross section measurement as a function of the exclusive jet multiplicity, for jet multiplicities of up to 7.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t2","@type":"Dataset","description":"The cross section measurement as a function of the inclusive jet multiplicity, for jet multiplicities of up to 7.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t3","@type":"Dataset","description":"The differential cross section measurement as a function of the transverse momentum of the first leading jet.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t4","@type":"Dataset","description":"The differential cross section measurement as a function of the transverse momentum of the second leading jet.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t5","@type":"Dataset","description":"The differential cross section measurement as a function of the transverse momentum of the third leading jet.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t6","@type":"Dataset","description":"The differential cross section measurement as a function of the transverse momentum of the fourth leading jet.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t7","@type":"Dataset","description":"The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t8","@type":"Dataset","description":"The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t9","@type":"Dataset","description":"The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t10","@type":"Dataset","description":"The differential cross section measurement as a function of the scalar sum of the transverse momenta of jets (HT) for...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t11","@type":"Dataset","description":"The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t12","@type":"Dataset","description":"The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t13","@type":"Dataset","description":"The differential cross section measurement as a function of the transverse momentum of the dijet system of the two highest...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t14","@type":"Dataset","description":"The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t15","@type":"Dataset","description":"The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t16","@type":"Dataset","description":"The differential cross section measurement as a function of the dijet invariant mass of the two highest pT jets for...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t17","@type":"Dataset","description":"The differential cross section measurement as a function of the absolute value of the pseudorapidity of the first leading jet.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t18","@type":"Dataset","description":"The differential cross section measurement as a function of the absolute value of the pseudorapidity of the second leading jet.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t19","@type":"Dataset","description":"The differential cross section measurement as a function of the absolute value of the pseudorapidity of the third leading jet.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t20","@type":"Dataset","description":"The differential cross section measurement as a function of the absolute value of the pseudorapidity of the fourth leading jet.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t21","@type":"Dataset","description":"The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t22","@type":"Dataset","description":"The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t23","@type":"Dataset","description":"The differential cross section measurement as a function of the rapidity difference between the two highest pT jets for events...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t24","@type":"Dataset","description":"The differential cross section measurement as a function of the rapidity difference between the first and the third highest pT...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t25","@type":"Dataset","description":"The differential cross section measurement as a function of the rapidity difference between the second and the third highest pT...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t26","@type":"Dataset","description":"The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t27","@type":"Dataset","description":"The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t28","@type":"Dataset","description":"The differential cross section measurement as a function of the rapidity difference between the most forward and the most backward...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t29","@type":"Dataset","description":"The differential cross section measurement as a function of the azimuthal angle separation between the two highest pT jets for...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t30","@type":"Dataset","description":"The differential cross section measurement as a function of the azimuthal angle separation between the most forward and the most...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t31","@type":"Dataset","description":"The differential cross section measurement as a function of DeltaR separation between the two highest pT jets for events with...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t32","@type":"Dataset","description":"The differential cross section measurement as a function of the azimuthal angle separation between the first leading jet and the...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t33","@type":"Dataset","description":"The differential cross section measurement as a function of the azimuthal angle separation between the second leading jet and the...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t34","@type":"Dataset","description":"The differential cross section measurement as a function of the azimuthal angle separation between the third leading jet and the...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t35","@type":"Dataset","description":"The differential cross section measurement as a function of the azimuthal angle separation between the fourth leading jet and the...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t36","@type":"Dataset","description":"Average number of jets as a function of HT for events with one or more jets.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t37","@type":"Dataset","description":"Average number of jets as a function of HT for events with two or more jets.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t38","@type":"Dataset","description":"Average number of jets as a function of the rapidity difference between the two highest pT jets for events with...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.76995.v2/t39","@type":"Dataset","description":"Average number of jets as a function of the rapidity difference between the most forward and the most backward jets...","name":"Table 39"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1491953?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/76995"}],"inLanguage":"en","name":"Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at sqrt(s)=8 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1491953?version=2","version":2}