{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.63512.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1273625"}},{"@id":"https://doi.org/10.1103/PhysRevC.89.044905","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"PHENIX Collaboration"},"creator":{"@type":"Organization","name":"PHENIX Collaboration"},"datePublished":"2014","description":"BNL-RHIC.  Measurements of the midrapidity transverse energy distribution, dET/deta, are presented for p+p, d+Au, and Au+Au collisions at sqrt(sNN) = 200 GeV and additionally for Au+Au collisions at sqrt(sNN) = 62.4 and 130 GeV.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t1","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t2","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t3","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t4","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t5","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t6","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t7","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t8","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t9","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t10","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t11","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t12","@type":"Dataset","description":"Et EMC distributions for sqrt(sNN) = 62.4 GeV Au+Au collisions shown in 5% wide centrality bins.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t13","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in Au+Au collisions.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t14","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in p+p collisions.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t15","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in d+Au collisions.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t16","@type":"Dataset","description":"The number of quark participants as a function of the number of nucleon participants.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t17","@type":"Dataset","description":"The number of quark participants as a function of the number of nucleon participants.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t18","@type":"Dataset","description":"The number of quark participants as a function of the number of nucleon participants.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t19","@type":"Dataset","description":"The ratio of the number of quark participants to the number of nucleon participants as a function of the number...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t20","@type":"Dataset","description":"The ratio of the number of quark participants to the number of nucleon participants as a function of the number...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t21","@type":"Dataset","description":"The ratio of the number of quark participants to the number of nucleon participants as a function of the number...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t22","@type":"Dataset","description":"dE_T/deta normalized by the number of participant pairs as a function of the number of participants.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t23","@type":"Dataset","description":"dE_T/deta normalized by the number of participant pairs as a function of the number of participants.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t24","@type":"Dataset","description":"dE_T/deta normalized by the number of participant pairs as a function of the number of participants.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t25","@type":"Dataset","description":"dE_T/deta normalized by the number of participant quark pairs as a function of the number of nucleon participants.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t26","@type":"Dataset","description":"dE_T/deta normalized by the number of participant quark pairs as a function of the number of nucleon participants.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t27","@type":"Dataset","description":"dE_T/deta normalized by the number of participant quark pairs as a function of the number of nucleon participants.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t28","@type":"Dataset","description":"dE_T/deta as a function of the number of quark participants.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t29","@type":"Dataset","description":"dE_T/deta as a function of the number of quark participants.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t30","@type":"Dataset","description":"dE_T/deta as a function of the number of quark participants.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t31","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in p+p collisions.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t32","@type":"Dataset","description":"Distribution of the number of quark participants in 200 GeV Au+Au collsions.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t33","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in p+p collisions.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t34","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in Au+Au collisions.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t35","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in d+Au collisions.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t36","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in d+Au collisions.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t37","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in Au+Au collisions.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t38","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in d+Au collisions.","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t39","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in Au+Au collisions.","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t40","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in Au+Au collisions.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t41","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in d+Au collisions.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t42","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in Au+Au collisions.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.63512.v1/t43","@type":"Dataset","description":"Corrected dE_T/deta distributions at sqrt(sNN) = 200 GeV for five sectors of PbSc in p+p collisions.","name":"Table 43"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1273625?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/63512"}],"inLanguage":"en","name":"Transverse-energy distributions at midrapidity in $p$$+$$p$, $d$$+$Au, and Au$+$Au collisions at $\\sqrt{s_{_{NN}}}=62.4$--200~GeV and implications for particle-production models","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1273625?version=1","version":1}