{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.57625.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/917599"}},{"@id":"https://doi.org/10.1140/epjc/s10052-011-1763-6","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2014","description":"CERN-LHC. Study of inclusive multi-jet production in proton-proton collisions at a centre-of-mass energy of 7 TeV.  The data sample was collected from April to August 2010 and has a total integrated luminosity of 2.4 pb^{-1} with a 3.4% uncertainty.  Jets are identified using the anti-KT algorithm with results given for both R=0.4 and R=0.6.  Jet multiplicities and differential cross sections are presented together with various ratios.  The data are compared to Monte-Carlo predictions.  In the tables where two systematic (sys) errors are shown, the first is the uncertainty on the jet energy scale and the second is the unfolding uncertainty. \n\nNote added (26 JUN 2014):\nThe cross section values reported in Tables 1, 3-9 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.57625.v1/t1","@type":"Dataset","description":"Total inclusive jet cross section as a function of the jet multiplicity.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t2","@type":"Dataset","description":"Ratio of the n-jet cross section to the (n-1) jet cross section.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t3","@type":"Dataset","description":"Differential cross section as a function of the leading jet PT for events with jet multiplicity >= 2.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t4","@type":"Dataset","description":"Differential cross section as a function of the 2nd leading jet PT for events with jet multiplicity >= 2.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t5","@type":"Dataset","description":"Differential cross section as a function of the 3rd leading jet PT for events with jet multiplicity >= 3.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t6","@type":"Dataset","description":"Differential cross section as a function of the 4th leading jet PT for events with jet multiplicity >= 4.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t7","@type":"Dataset","description":"Differential cross section as a function of the scalar sum of the jet PTs (HT) for events with jet multiplicity...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t8","@type":"Dataset","description":"Differential cross section as a function of the scalar sum of the jet PTs (HT) for events with jet multiplicity...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t9","@type":"Dataset","description":"Differential cross section as a function of the scalar sum of the jet PTs (HT) for events with jet multiplicity...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t10","@type":"Dataset","description":"3-to-2 jet differential cross section ratio as a function of the leading jet PT for a minimum non-leading jet PT...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t11","@type":"Dataset","description":"3-to-2 jet differential cross section ratio as a function of the leading jet PT for a minimum non-leading jet PT...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t12","@type":"Dataset","description":"3-to-2 jet differential cross section ratio as a function of the leading jet PT for a minimum non-leading jet PT...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t13","@type":"Dataset","description":"3-to-2 jet differential cross section ratio as a function of the leading jet PT with R=0.4 for a minimum non-leading...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t14","@type":"Dataset","description":"3-to-2 jet differential cross section ratio as a function of the leading jet PT with R=0.4 for a minimum non-leading...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t15","@type":"Dataset","description":"3-to-2 jet differential cross section ratio as a function of the leading jet PT with R=0.4 for a minimum non-leading...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t16","@type":"Dataset","description":"3-to-2 jet differential cross section ratio as a function of the sum of the PTs of the two leading jets...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.57625.v1/t17","@type":"Dataset","description":"3-to-2 jet differential cross section ratio as a function of the sum of the PTs of the two leading jets...","name":"Table 17"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins917599?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/57625"}],"inLanguage":"en","name":"Measurement of multi-jet cross sections in proton-proton collisions at a 7 TeV center-of-mass energy","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins917599?version=1","version":1}