{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.144263.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2693040"}},{"@id":"https://doi.org/10.1103/PhysRevLett.134.232301","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2025","description":"The STAR Collaboration presents measurements of the semi-inclusive distribution of charged-particle jets recoiling from energetic direct-photon ($\\gamma_{\\rm dir}$) and neutral-pion ($\\pi^{0}$) triggers in p+p and central Au+Au collisions at $\\sqrt{s_\\mathrm{NN}}$ GeV over a broad kinematic range, for jet resolution parameters $R$=0.2 and 0.5. Medium-induced jet yield suppression is observed to be larger for $R$=0.2 than for 0.5, reflecting the angular range of jet energy redistribution due to quenching. The predictions of model calculations incorporating jet quenching are not fully consistent with the observations. These results provide new insight into the physical origins of jet quenching.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.144263.v1/t1","@type":"Dataset","description":"I_{AA} of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV for R = 0.2 of gamma_{dir}+jet with E_{T,trig}= 15-20 GeV.","name":"Table1"},{"@id":"https://doi.org/10.17182/hepdata.144263.v1/t2","@type":"Dataset","description":"I_{AA} of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV for R = 0.5 of gamma_{dir}+jet with E_{T,trig}= 15-20 GeV.","name":"Table2"},{"@id":"https://doi.org/10.17182/hepdata.144263.v1/t3","@type":"Dataset","description":"I_{AA} of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV for R = 0.2 of pi^{0}+jet with E_{T,trig}= 11-15 GeV.","name":"Table3"},{"@id":"https://doi.org/10.17182/hepdata.144263.v1/t4","@type":"Dataset","description":"I_{AA} of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV for R = 0.5 of pi^{0}+jet with E_{T,trig}= 11-15 GeV.","name":"Table4"},{"@id":"https://doi.org/10.17182/hepdata.144263.v1/t5","@type":"Dataset","description":"Yield Ratio R=0.2/R=0.5 of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV of gamma_{dir}+jet with E_{T,trig}= 15-20 GeV.","name":"Table5"},{"@id":"https://doi.org/10.17182/hepdata.144263.v1/t6","@type":"Dataset","description":"Yield Ratio R=0.2/R=0.5 of Au+Au 0%-15% collisions at sqrt{s_{NN}} = 200 GeV of pi^{0}+jet with E_{T,trig}= 11-15 GeV.","name":"Table6"},{"@id":"https://doi.org/10.17182/hepdata.144263.v1/t7","@type":"Dataset","description":"Yield Ratio R=0.2/R=0.5 of p+p collisions at sqrt{s_{NN}} = 200 GeV of gamma_{dir}+jet with E_{T,trig}= 15-20 GeV.","name":"Table7"},{"@id":"https://doi.org/10.17182/hepdata.144263.v1/t8","@type":"Dataset","description":"Yield Ratio R=0.2/R=0.5 of p+p collisions at sqrt{s_{NN}} = 200 GeV of pi^{0}+jet with E_{T,trig}= 11-15 GeV.","name":"Table8"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2693040?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/144263"}],"inLanguage":"en","name":"Measurement of in-medium jet modification using direct photon+jet and $\\pi^{0}$+jet correlations in $p+p$ and central Au+Au collisions at $\\sqrt{s_{\\rm NN}} = 200$ GeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2693040?version=1","version":1}