{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.39682.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1083318"}},{"@id":"https://doi.org/10.1103/PhysRevD.85.092002","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2014","description":"CERN-LHC.  Measurements of cross sections for final states containing a W boson and hadronic jets in proton-proton collisions at a centre-of-mass energy of 7 TeV.  The data is from the full 2010 sample with a total integrated luminosity of 36 pb^{-1}.  Cross sections are measured in both the electron and muon decay modes of the W and are presented as a function of inclusive  jet multiplicity up to five jets.  For each multiplicity, cross sections are determined  as a  function of (1) each jet PT, (2) the scalar sum (HT) of the PT of the charged lepton, missing PT  and all jets, (3) the invariant mass of the jets and (4) rapidity distributions of various  combinations of leptons and jets.  The results are corrected for all detector effects and  all known backgrounds.  Comparative results are also shown for particle-level predicitions from ALPGEN, SHERPA and BLACKHAT-SHERPA.  A separate link gives the Non-Perturbative and QED correction for each table. \n\nNote added (26 JUN 2014):\nThe cross section values reported in Tables 1, 3-25, 51, 53-75 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period.  The uncertainty on the global normalisation (\"Lumi\") increases slightly from 3.4% to 3.5%.  See Eur.Phys.J. C73 (2013) 2518 for more details.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t1","@type":"Dataset","description":"The measured W+jets cross section as a function of the jet multiplicity for jet PT > 30 GeV shown for...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t2","@type":"Dataset","description":"The measured W+jets cross section ratio as a function of jet multiplicity for jet PT > 30 GeV.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t3","@type":"Dataset","description":"The measured W+jets cross section as a function of the pT of the first jet in the event for jet...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t4","@type":"Dataset","description":"The measured W+jets cross section as a function of the pT of the first jet in the event for jet...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t5","@type":"Dataset","description":"The measured W+jets cross section as a 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measured W+jets cross section as a function of the pT of the third jet in the event for jet...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t11","@type":"Dataset","description":"The measured W+jets cross section as a function of the pT of the third jet in the event for jet...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t12","@type":"Dataset","description":"The measured W+jets cross section as a function of the pT of the fourth jet in the event for jet...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t13","@type":"Dataset","description":"The measured W+jets cross section as a function of HT for jet multiplicities >= 1 and jet PT > 30...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t14","@type":"Dataset","description":"The measured W+jets cross section as a function of HT for jet multiplicities >= 2 and jet PT > 30...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t15","@type":"Dataset","description":"The measured W+jets cross section as a function of HT for jet multiplicities >= 3 and jet PT > 30...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t16","@type":"Dataset","description":"The measured W+jets cross section as a function of HT for jet multiplicities >= 4 and jet PT > 30...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t17","@type":"Dataset","description":"The measured W+jets cross section as a function of the invariant mass of the first+second jets for jet multiplicites >=...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t18","@type":"Dataset","description":"The measured W+jets cross section as a function of the invariant mass of the first+second+third jets for jet multiplicites >=...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t19","@type":"Dataset","description":"The measured W+jets cross section as a function of the invariant mass of the first+second+third+fourth jets for jet multiplicites >=...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t20","@type":"Dataset","description":"The measured W+jets cross section as a function of the rapidity of the first jet in the event for jet...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t21","@type":"Dataset","description":"The measured W+jets cross section as a function of the DeltaR(first jet,second jet) for jet multiplicites >= 2 and jet...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t22","@type":"Dataset","description":"The measured W+jets cross section as a function of the |y(lepton)-y(first jet)| for jet multiplicites >= 2 and jet PT...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t23","@type":"Dataset","description":"The measured W+jets cross section as a function of the |y(first jet)+y(second jet)| for jet 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27"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t28","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the first jet in the event for jet...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t29","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the first jet in the event for jet...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t30","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the first jet in the event for jet...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t31","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the first jet in the event for jet...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t32","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the second jet in the event for jet...","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t33","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the second jet in the event for jet...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t34","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the second jet in the event for jet...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t35","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the third jet in the event for jet...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t36","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the third jet in the event for jet...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t37","@type":"Dataset","description":"The predicted W+jets cross section as a function of the pT of the fourth jet in the event for jet...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t38","@type":"Dataset","description":"The predicted W+jets cross section as a function of HT for jet multiplicities >= 1 and jet PT > 30...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t39","@type":"Dataset","description":"The predicted W+jets cross section as a function of HT for jet multiplicities >= 2 and jet PT > 30...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t40","@type":"Dataset","description":"The predicted W+jets cross section as a function of HT for jet multiplicities >= 3 and jet PT > 30...","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.39682.v1/t41","@type":"Dataset","description":"The predicted W+jets cross section as a function of HT for jet multiplicities >= 4 and jet PT > 30...","name":"Table 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