{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.139080.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2641480"}},{"@id":"https://doi.org/10.1007/JHEP06(2023)176","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2023","description":"We report a new measurement of the production of electrons from open heavy-flavor hadron decays (HFEs) at mid-rapidity ($|y|<$ 0.7) in Au+Au collisions at $\\sqrt{s_{\\rm NN}}=200$ GeV. Invariant yields of HFEs are measured for the transverse momentum range of $3.5 < p_{\\rm T} < 9$ GeV/$c$ in various configurations of the collision geometry. The HFE yields in head-on Au+Au collisions are suppressed by approximately a factor of 2 compared to that in $p$+$p$ collisions scaled by the average number of binary collisions, indicating strong interactions between heavy quarks and the hot and dense medium created in heavy-ion collisions. Comparison of these results with models provides additional tests of theoretical calculations of heavy quark energy loss in the quark-gluon plasma.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.139080.v1/t1","@type":"Dataset","description":"Ratios of NPE (non-photonic electron) to PHE (photonic electron) as a function of $p_{\\rm T}$ in 0-10% central (yellow circles)...","name":"Figure 3a"},{"@id":"https://doi.org/10.17182/hepdata.139080.v1/t2","@type":"Dataset","description":"Invariant yields of electrons from decays of prompt $J/\\psi$ (dot-dashed line), $\\Upsilon$ (dotted line), Drell-Yan (long dash-dotted line), light vector...","name":"Figure 4a"},{"@id":"https://doi.org/10.17182/hepdata.139080.v1/t3","@type":"Dataset","description":"Invariant yields of electrons from decays of prompt $J/\\psi$ (dot-dashed line), $\\Upsilon$ (dotted line), Drell-Yan (long dash-dotted line), light vector...","name":"Figure 4b"},{"@id":"https://doi.org/10.17182/hepdata.139080.v1/t4","@type":"Dataset","description":"HFE (electrons from semileptonic decays of heavy-flavor hadrons) invariant yields in different centrality intervals of Au+Au collisions at $\\sqrt{s_{\\rm NN}}=200$...","name":"Figure 5"},{"@id":"https://doi.org/10.17182/hepdata.139080.v1/t5","@type":"Dataset","description":"HFE (electrons from semileptonic decays of heavy-flavor hadrons) $R_{\\rm AA}$ (red circles) as a function of $p_{\\rm T}$ in different...","name":"Figure 6"},{"@id":"https://doi.org/10.17182/hepdata.139080.v1/t6","@type":"Dataset","description":"HFE (electrons from semileptonic decays of heavy-flavor hadrons) $R_{\\rm AA}$ (red circles) as a function of $N_{\\rm part}$ in Au+Au...","name":"Figure 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2641480?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/139080"}],"inLanguage":"en","name":"Measurement of electrons from open heavy-flavor hadron decays in Au+Au collisions at $\\sqrt{s_{\\rm NN}}=200$ GeV with the STAR detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2641480?version=1","version":1}