{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.62685.v1/t2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1243871"}},{"@id":"https://doi.org/10.1140/epjc/s10052-013-2676-3","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2014","description":"Integrated jet shape as a function of the radius r for the PT range 30-40 GeV.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/55073/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/55073/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/55073/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/55073/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/55073/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1243871?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/62685"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.62685.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1243871?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.62685.v1","@type":"Dataset","description":"CERN-LHC.  Measurement of the jet shapes in top-quark pair events from proton-proton collisions at a centre-of-mass energy of 7 TeV.  The analysis uses a data sample of integrated luminosity 1.8 fb-1.  Jets are reconstructed using the anti-kT algorithm with jet radius R=0.4.  Jet shapes are presented as differential and integrated defined as:  \nDifferential (RHO) - scalar sum of jet PT in an annulus of thickness deltaR around radius r / scalar sum of jet PT in the cone of radius R.  \nIntegrated (PSI) - scalar sum of jet PT in cone radius r / scalar sum of jet PT in cone radius R.  \nData are shown separated into b-jets and light-jet events. \n\nUPDATE (22 JUL 2014): Information on the different sources of systematic uncertainty is given in the following four links, containing tables with the relative values of the uncertainty (in %) for both the differential (Diff) and integrated (Int) versions of the jet shapes for both light- (lJets) and b-jets (bJets).  The uncertainties indicated with (Up) and (Down) are asymmetric, while the rest are symmetric on each bin.","name":"Measurement of jet shapes in top pair events at sqrt(s) = 7 TeV using the ATLAS detector","url":"https://www.hepdata.net/record/ins1243871?version=1"},"keywords":"P P --> TOP TOPBAR X, P P --> TOP TOPBAR X, P P --> JET X, SHAPE, Inclusive, Top, Proton-Proton Scattering, Jet Production, 7000.0","name":"Table 2","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/62689","version":1}