{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.58228.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/945498"}},{"@id":"https://doi.org/10.1103/PhysRevD.85.032009","@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 Z0/GAMMA* production plus jets in proton-proton collisions at a centre-of-mass energy of 7 TeV.  The analysis includes the full 2010 data set, collected at low rate of collisions, with a total integrated luminosity of 36 pb^{-1}.  Data are presented for Jet PT>30 GeV and |y|<4.4 with cross sections  in both the individual electron and muon decay modes of the Z0/GAMMA* as well as combined after  correction to a common lepton fiducial region of |y|<2.5 and PT>20 GeV and for QED radiation effects. \n\nNote added (26 JUN 2014):\nThe cross section values reported in Tables 1, 3-13 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.58228.v1/t1","@type":"Dataset","description":"Cross section for Inclusive Jet Multiplicity corrected to the lepton common fiducial region and for QED radiation effects.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t2","@type":"Dataset","description":"Ratio of cross sections for N/N-1 inclusive jet multiplicities corrected to the lepton common fiducial region and for QED radiation...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t3","@type":"Dataset","description":"Inclusive jet differential cross section dsigma/dpt corrected to the lepton common fiducial region and for QED radiation effects.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t4","@type":"Dataset","description":"Cross section dsigma/dpt as a function of the leading jet pt corrected to the lepton common fiducial region and for...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t5","@type":"Dataset","description":"Cross section dsigma/dpt as a function of the second-leading jet pt corrected to the lepton common fiducial region and for...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t6","@type":"Dataset","description":"Inclusive jet differential cross section dsigma/dy corrected to the lepton common fiducial region and for QED radiation effects.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t7","@type":"Dataset","description":"Jet differential cross section dsigma/dy as a function of the leading jet y corrected to the lepton common fiducial region...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t8","@type":"Dataset","description":"Jet differential cross section dsigma/dy as a function of the second-leading jet y corrected to the lepton common fiducial region...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t9","@type":"Dataset","description":"Differential cross section dsigma/dmjj as a function of the dijet invariant mass mjj corrected to the lepton common fiducial region...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t10","@type":"Dataset","description":"Differential cross section dsigma/d DeltaYjj as a function of the dijet rapidity separation DeltaYjj corrected to the lepton common fiducial...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t11","@type":"Dataset","description":"Differential cross section dsigma/d DeltaPhijj as a function of the dijet azimuthal separation DeltaPhijj corrected to the lepton common fiducial...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t12","@type":"Dataset","description":"Differential cross section dsigma/d DeltaRjj as a function of the dijet angular separation DeltaRjj corrected to the lepton common fiducial...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t13","@type":"Dataset","description":"Cross section for Inclusive Jet Multiplicity for the electron channel and the muon channel in the individual lepton fiducial regions...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t14","@type":"Dataset","description":"Ratio of cross sections for N/N-1 inclusive jet multiplicities for the electron channel and the muon channel in the individual...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t15","@type":"Dataset","description":"Measured normalized inclusive jet differential cross section 1/sigma_DY dsigma/dpt for the electron channel and the muon channel in the individual...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t16","@type":"Dataset","description":"Measured normalized leading jet differential cross section 1/sigma_DY dsigma/dpt for the electron channel and the muon channel in the individual...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t17","@type":"Dataset","description":"Measured normalized second-leading jet differential cross section 1/sigma_DY dsigma/dpt for the electron channel and the muon channel in the individual...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t18","@type":"Dataset","description":"Measured normalized inclusive jet differential cross section 1/sigma_DY dsigma/dy for the electron channel and the muon channel in the individual...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t19","@type":"Dataset","description":"Measured normalized leading jet differential cross section 1/sigma_DY dsigma/dy for the electron channel and the muon channel in the individual...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t20","@type":"Dataset","description":"Measured normalized second leading jet differential cross section 1/sigma_DY dsigma/dy for the electron channel and the muon channel in the...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t21","@type":"Dataset","description":"Measured normalized differential cross section as a function of dijet invariant mass 1/sigma_DY dsigma/dmjj for the electron channel and the...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t22","@type":"Dataset","description":"Measured normalized differential cross section as a function of dijet rapidity separation 1/sigma_DY dsigma/dDeltaYjj for the electron channel and the...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t23","@type":"Dataset","description":"Measured normalized differential cross section as a function of dijet azimuthal separation 1/sigma_DY dsigma/dDeltaPhijj (1/rad.) for the electron channel and...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.58228.v1/t24","@type":"Dataset","description":"Measured normalized differential cross section as a function of dijet angular separation 1/sigma_DY dsigma/dDeltaRjj for the electron channel and the...","name":"Table 24"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins945498?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/58228"}],"inLanguage":"en","name":"Measurement of the production cross section for Z/gamma* 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/ins945498?version=1","version":1}