{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.139723.v1/t5","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2648097"}},{"@id":"https://doi.org/10.1016/j.physletb.2024.138998","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"The double $R_{\\mathrm{AA}}$ ratio of $R_{\\mathrm{AA}}^{\\gamma\\text{-jet}}/R_{\\mathrm{AA}}^{\\text{inclusive jet}}$ as a function of jet $p_{\\mathrm{T}}$.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1485538/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1485538/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1485538/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1485538/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1485538/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2648097?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/139723"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.139723.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins2648097?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.139723.v1","@type":"Dataset","description":"Parton energy loss in the quark-gluon plasma (QGP) is studied with a measurement of photon-tagged jet production in 1.7 nb$^{-1}$ of Pb+Pb data and 260 pb$^{-1}$ of $pp$ data, both at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV, with the ATLAS detector. The process $pp \\to \\gamma$+jet+$X$ and its analogue in Pb+Pb collisions is measured in events containing an isolated photon with transverse momentum ($p_\\mathrm{T}$) above $50$ GeV and reported as a function of jet $p_\\mathrm{T}$. This selection results in a sample of jets with a steeply falling $p_\\mathrm{T}$ distribution that are mostly initiated by the showering of quarks. The $pp$ and Pb+Pb measurements are used to report the nuclear modification factor, $R_\\mathrm{AA}$, and the fractional energy loss, $S_\\mathrm{loss}$, for photon-tagged jets. In addition, the results are compared with the analogous ones for inclusive jets, which have a significantly smaller quark-initiated fraction. The $R_\\mathrm{AA}$ and $S_\\mathrm{loss}$ values are found to be significantly different between those for photon-tagged jets and inclusive jets, demonstrating that energy loss in the QGP is sensitive to the colour-charge of the initiating parton. The results are also compared with a variety of theoretical models of colour-charge-dependent energy loss.","name":"Comparison of inclusive and photon-tagged jet suppression in 5.02 TeV Pb+Pb collisions with ATLAS","url":"https://www.hepdata.net/record/ins2648097?version=1"},"keywords":"Pb Pb --> $\\gamma$ + jet + X, P P --> $\\gamma$ + jet + X, 5020.0, Photon-tagged jets, Inclusive jets","name":"Figure 9","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/145381","version":1}