{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.57048.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/882534"}},{"@id":"https://doi.org/10.1016/j.physletb.2011.03.012","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2011","description":"CERN-LHC.  Measurement of the inclusive W+jets cross section in proton-proton collisions at centre-of-mass enrgy 7 TeV. The data, collected from March to August 2010 have an integrated luminosity of 1.3 pb-1, and have been corrected for all known detector effects and are quoted within limited and well defined ranges of jet and lepton kinematics.  Jets were reconstructed using the  anti-kT algoithm with radius parameter R = 0.4. The lepton energy is defined as the energy of the lepton after radiation plus the energy of all radiated photons within DeltaR=0.1 around the lepton.   Additionally the distance from the lepton to the jet axis was required to have DeltaR=>0.5 and muons were isolated with DeltaR>0.2. Cross sections are presented, in both the electron and muon decay modes of the W, as a function of jet multiplicity and transverse momentum of both the leading and next-to-leading jets in the event. Where appropriate in the tables the second DSYS error is the luminosity uncertainty.  Numerical values supplied by M Dunford.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.57048.v1/t1","@type":"Dataset","description":"The measured cross section times branching ratio for W+jets in the electron channel as a function of corrected jet multiplicity.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.57048.v1/t2","@type":"Dataset","description":"The measured cross section times branching ratio for W+jets in the muon channel as a function of corrected jet multiplicity.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.57048.v1/t3","@type":"Dataset","description":"The measured cross section ratio for W+jets in the electron channel as a function of corrected jet multiplicity.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.57048.v1/t4","@type":"Dataset","description":"The measured cross section ratio for W+jets in the muon channel as a function of corrected jet multiplicity.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.57048.v1/t5","@type":"Dataset","description":"The cross section times branching ratio for W+jets in the electron channel as a function of the leading jet PT.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.57048.v1/t6","@type":"Dataset","description":"The cross section times branching ratio for W+jets in the muon channel as a function of the leading jet PT.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.57048.v1/t7","@type":"Dataset","description":"The cross section times branching ratio for W+jets in the electron channel as a function of the next-to-leading jet PT.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.57048.v1/t8","@type":"Dataset","description":"The cross section times branching ratio for W+jets in the muon channel as a function of the next-to-leading jet PT.","name":"Table 8"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins882534?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/57048"}],"inLanguage":"en","name":"Measurement of the production cross section for W-bosons in association with jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins882534?version=1","version":1}