{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.84819.v1/t2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1673184"}},{"@id":"https://doi.org/10.1016/j.physletb.2018.10.076","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"No description provided.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/329597/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/329597/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/329597/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/329597/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/329597/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1673184?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/84819"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.84819.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1673184?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.84819.v1","@type":"Dataset","description":"CERN-LHC.  Measurements of the yield and nuclear modification factor, $R_{\\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|<2.8$. The magnitude of $R_{\\mathrm {AA}}$ increases with increasing $p_{\\mathrm {T}}$ reaching a value of $\\approx 0.6$ near the $p_{\\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\\mathrm {T}}$ but it is observed to  decrease with increasing rapidity at high $p_{\\mathrm {T}}$.","name":"Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\\sqrt{s_\\mathrm{NN}}=5.02$ TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins1673184?version=1"},"keywords":"P P --> JETS X, PTRECO / PTTRUTH, 5020.0, Inclusive, Double Differential Distribution, Transverse Momentum Dependence, Rapidity Dependence, Jet Production","name":"Table 2","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/85656","version":1}