{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.73457.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1288917"}},{"@id":"https://doi.org/10.1103/PhysRevLett.113.052302","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2016","description":"BNL-RHIC.  Local parity-odd domains are theorized to form inside a Quark-Gluon-Plasma (QGP) which has been produced in high-energy heavy-ion collisions. The local parity-odd domains manifest themselves as charge separation along the magnetic field axis via the chiral magnetic effect (CME). The experimental observation of charge separation has previously been reported for heavy-ion collisions at the top RHIC energies. In this paper, we present the results of the beam-energy dependence of the charge correlations in Au+Au collisions at midrapidity for center-of-mass energies of 7.7, 11.5, 19.6, 27, 39 and 62.4 GeV from the STAR experiment. After background subtraction, the signal gradually reduces with decreased beam energy, and tends to vanish by 7.7 GeV. The implications of these results for the CME will be discussed.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t1","@type":"Dataset","description":"The three-point correlator, $\\gamma$, as a function of centrality for Au+Au collisions at 62.4 GeV.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t2","@type":"Dataset","description":"The three-point correlator, $\\gamma$, as a function of centrality for Au+Au collisions at 39 GeV.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t3","@type":"Dataset","description":"The three-point correlator, $\\gamma$, as a function of centrality for Au+Au collisions at 27 GeV.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t4","@type":"Dataset","description":"The three-point correlator, $\\gamma$, as a function of centrality for Au+Au collisions at 19.6 GeV.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t5","@type":"Dataset","description":"The three-point correlator, $\\gamma$, as a function of centrality for Au+Au collisions at 11.5 GeV.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t6","@type":"Dataset","description":"The three-point correlator, $\\gamma$, as a function of centrality for Au+Au collisions at 7.7.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t7","@type":"Dataset","description":"The two-particle correlation as a function of centrality for Au+Au collisions at 62.4 GeV.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t8","@type":"Dataset","description":"The two-particle correlation as a function of centrality for Au+Au collisions at 39 GeV.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t9","@type":"Dataset","description":"The two-particle correlation as a function of centrality for Au+Au collisions at 27 GeV.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t10","@type":"Dataset","description":"The two-particle correlation as a function of centrality for Au+Au collisions at 19.6 GeV.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t11","@type":"Dataset","description":"The two-particle correlation as a function of centrality for Au+Au collisions at 11.5 GeV.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t12","@type":"Dataset","description":"The two-particle correlation as a function of centrality for Au+Au collisions at 7.7 GeV.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t13","@type":"Dataset","description":"$H_{SS}-H{OS}$, as a function of beam energy for 60-80% centrality in Au+Au collisions.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t14","@type":"Dataset","description":"$H_{SS}-H{OS}$, as a function of beam energy for 30-60% centrality in Au+Au collisions.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.73457.v1/t15","@type":"Dataset","description":"$H_{SS}-H{OS}$, as a function of beam energy for 10-30% centrality in Au+Au collisions.","name":"Table 15"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1288917?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/73457"}],"inLanguage":"en","name":"Beam-energy dependence of charge separation along the magnetic field in Au+Au collisions at RHIC","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1288917?version=1","version":1}