{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.102941.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1486427"}},{"@id":"https://doi.org/10.1103/PhysRevLett.119.062301","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2021","description":"We report the first di-jet transverse momentum asymmetry measurements from Au+Au and p+p collisions at RHIC. The two highest-energy back-to-back jets reconstructed from fragments with transverse momenta above 2 GeV/c display a significantly stronger momentum imbalance in heavy-ion collisions than in the p+p reference. When re-examined with correlated soft particles included, we observe that these di-jets then exhibit a unique new feature -- momentum balance is restored to that observed in p+p for a jet resolution parameter of R=0.4, while re-balancing is not attained with a smaller value of R=0.2.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t1","@type":"Dataset","description":"Normalized AJ distributions for Au+Au HT data (filled symbols) and p+p HT $\\oplus$ Au+Au MB (open symbols). The red circles...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t2","@type":"Dataset","description":"$p_{T}^{Part}$ vs. $p_{T}^{Det}$ for Leading jets with $R = 0.4$.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t3","@type":"Dataset","description":"$p_{T}^{Part}$ vs. $p_{T}^{Det}$ for Leading jets with $R = 0.2$.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t4","@type":"Dataset","description":"$p_{T}^{Part}$ vs. $p_{T}^{Det}$ for SubLeading jets with $R = 0.4$.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t5","@type":"Dataset","description":"$p_{T}^{Part}$ vs. $p_{T}^{Det}$ for SubLeading jets with $R = 0.2$.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t6","@type":"Dataset","description":"$A_{J}$ distributions for Au+Au data (filled symbols) and p+p HT $\\oplus$ Au+Au MB (open symbols) for low constituent $p_{T}^{Cut}$ di-jets...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t7","@type":"Dataset","description":"$dN/d\\delta p_{T}$ vs. $\\delta p_{T}$ for $p_{T}^{Cut} > 2$ GeV/$c$ jets with $R = 0.4$.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t8","@type":"Dataset","description":"$dN/d\\delta p_{T}$ vs. $\\delta p_{T}$ for $p_{T}^{Cut} > 0.2$ GeV/$c$ matched jets with $R = 0.4$.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t9","@type":"Dataset","description":"$dN/d\\delta p_{T}$ vs. $\\delta p_{T}$ for $p_{T}^{Cut} > 2$ GeV/$c$ jets with $R = 0.2$.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t10","@type":"Dataset","description":"$dN/d\\delta p_{T}$ vs. $\\delta p_{T}$ for $p_{T}^{Cut} > 0.2$ GeV/$c$ matched jets with $R = 0.2$.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.102941.v1/t11","@type":"Dataset","description":"Repetition of the analysis shown in Fig. 1 with a smaller resolution parameter $R = 0.2$. Normalized $A_{J}$ distributions for...","name":"Table 11"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1486427?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/102941"}],"inLanguage":"en","name":"Di-Jet Imbalance Measurements at $\\sqrt{s_{NN}} = 200$ GeV at STAR","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1486427?version=1","version":1}