{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.144264.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2693062"}},{"@id":"https://doi.org/10.1103/8b8y-98yh","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2025","description":"The STAR experiment at RHIC reports new measurements of jet quenching based on the semi-inclusive distribution of charged-particle jets recoiling from direct photon ($\\gamma_{\\rm dir}$) and neutral pion ($\\pi^{0}$) triggers in pp and central Au+Au collisions at $\\sqrt{s_{\\rm NN}}=200$ GeV, for triggers in the range $9<E_{\\rm T}^{\\rm trig}<20$ GeV. The datasets have integrated luminosities of 3.9$ {\\rm nb}^{-1}$ for Au+Au and 23$ {\\rm pb}^{-1}$ for pp collisions. Jets are reconstructed using the anti-$k_{\\rm T}$ algorithm with resolution parameters $R$=0.2 and 0.5. The large uncorrelated jet background in central Au+Au collisions is corrected using a mixed-event approach, which enables precise charged-particle jet measurements at low transverse momentum $p_{\\rm T,jet}^{\\rm ch}$ and large $R$. Recoil-jet distributions are reported in the range $p_{\\rm T,jet}^{\\rm ch}<25$\\gev. Comparison of the distributions measured in pp and Au+Au collisions reveals strong medium-induced jet yield suppression for $R=0.2$, with markedly less suppression for $R=0.5$. Comparison is also made to theoretical models incorporating jet quenching. These data provide new insight into the mechanisms underlying jet quenching and the angular dependence of medium-induced jet-energy transport, and provide new constraints on modelling such effects.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.144264.v1/t1","@type":"Dataset","description":"Rho distribution of SE recoil jet R=0.5 for AuAu 0-15% at sqrt{s_{NN}}=200 GeV from gamma_{rich}+jet event sample.","name":"Table1"},{"@id":"https://doi.org/10.17182/hepdata.144264.v1/t2","@type":"Dataset","description":"Rho distribution of ME recoil jet R=0.5 for AuAu 0-15% at sqrt{s_{NN}}=200 GeV from MB event sample.","name":"Table2"},{"@id":"https://doi.org/10.17182/hepdata.144264.v1/t3","@type":"Dataset","description":"Rho distribution of ME-30MeV recoil jet R=0.5 for AuAu 0-15% at sqrt{s_{NN}}=200 GeV from MB event sample.","name":"Table3"},{"@id":"https://doi.org/10.17182/hepdata.144264.v1/t4","@type":"Dataset","description":"Rho distribution of ME+30MeV recoil jet R=0.5 for AuAu 0-15% 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GeV.","name":"Table12"},{"@id":"https://doi.org/10.17182/hepdata.144264.v1/t13","@type":"Dataset","description":"Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 11-15 GeV.","name":"Table13"},{"@id":"https://doi.org/10.17182/hepdata.144264.v1/t14","@type":"Dataset","description":"Per trigger recoil jet distribution for pp at sqrt{s}=200 GeV with jet R=0.5 and gamma_{rich} E_{T,trig}= 15-20 GeV.","name":"Table14"},{"@id":"https://doi.org/10.17182/hepdata.144264.v1/t15","@type":"Dataset","description":"Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 9-11 GeV.","name":"Table15"},{"@id":"https://doi.org/10.17182/hepdata.144264.v1/t16","@type":"Dataset","description":"Per trigger SE recoil jet distribution for AuAu 0-15% at sqrt{s_{NN}}=200 GeV with jet R=0.2 and gamma_{rich} E_{T,trig}= 11-15 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