{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.73493.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1315466"}},{"@id":"https://doi.org/10.1016/j.physletb.2015.04.033","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2016","description":"BNL-RHIC.  A data-driven method was applied to measurements of Au+Au collisions at $\\sqrt{s_{_{\\rm NN}}} =$ 200 GeV made with the STAR detector at RHIC to isolate pseudorapidity distance $\\Delta\\eta$-dependent and $\\Delta\\eta$-independent correlations by using two- and four-particle azimuthal cumulant measurements. We identified a component of the correlation that is $\\Delta\\eta$-independent, which is likely dominated by anisotropic flow and flow fluctuations. It was also found to be independent of $\\eta$ within the measured range of pseudorapidity $|\\eta|<1$. The relative flow fluctuation was found to be $34\\% \\pm 2\\% (stat.) \\pm 3\\% (sys.)$ for particles of transverse momentum $p_{T}$ less than $2$ GeV/$c$. The $\\Delta\\eta$-dependent part may be attributed to nonflow correlations, and is found to be $5\\% \\pm 2\\% (sys.)$ relative to the flow of the measured second harmonic cumulant at $|\\Delta\\eta| > 0.7$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t1","@type":"Dataset","description":"The second harmonic two-particle cumulants for ($\\eta_{\\alpha}$, $\\eta_{\\beta}$ pairs for 20-30% central Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t2","@type":"Dataset","description":"The third harmonic two-particle cumulants for ($\\eta_{\\alpha}$, $\\eta_{\\beta}$ pairs for 20-30% central Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t3","@type":"Dataset","description":"The second harmonic four-particle cumulant for ($\\eta_{\\alpha}$, $\\eta_{\\alpha}$, $\\eta_{\\beta}$, $\\eta_{\\beta}$) quadruplets for 20-30% central Au+Au collisions at $\\sqrt{s_{NN}}$ = 200...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t4","@type":"Dataset","description":"The $V_2${2} and difference between the pairs at ($\\eta_{\\alpha}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, -$\\eta_{\\beta}$). The data are from 20-30% central Au+Au...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t5","@type":"Dataset","description":"The $V_2${2} and difference between the pairs at ($\\eta_{\\alpha}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, -$\\eta_{\\beta}$). The data are from 20-30% central Au+Au...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t6","@type":"Dataset","description":"The $V_2${2} and difference between the pairs at ($\\eta_{\\alpha}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, -$\\eta_{\\beta}$). The data are from 20-30% central Au+Au...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t7","@type":"Dataset","description":"The $V_2${2} and difference between the pairs at ($\\eta_{\\alpha}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, -$\\eta_{\\beta}$). The data are from 20-30% central Au+Au...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t8","@type":"Dataset","description":"The $V_3${2} and difference between the pairs at ($\\eta_{\\alpha}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, -$\\eta_{\\beta}$). The data are from 20-30% central Au+Au...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t9","@type":"Dataset","description":"The $V_3${2} and difference between the pairs at ($\\eta_{\\alpha}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, -$\\eta_{\\beta}$). The data are from 20-30% central Au+Au...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t10","@type":"Dataset","description":"The $V_3${2} and difference between the pairs at ($\\eta_{\\alpha}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, -$\\eta_{\\beta}$). The data are from 20-30% central Au+Au...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t11","@type":"Dataset","description":"The $V_3${2} and difference between the pairs at ($\\eta_{\\alpha}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, -$\\eta_{\\beta}$). The data are from 20-30% central Au+Au...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t12","@type":"Dataset","description":"The $V_2^{1/2}$ difference between quadruplets at ($\\eta_{\\alpha}$, $\\eta_{\\alpha}$, $\\eta_{\\beta}$, $\\eta_{\\beta}$) and ($\\eta_{\\alpha}$, $\\eta_{\\alpha}$, -$\\eta_{\\beta}$, -$\\eta_{\\beta}$).","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t13","@type":"Dataset","description":"The two-particle cumulants, V2{2} as a function of $\\eta$ for one particle while averaged over $\\eta$ of the partner particle.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t14","@type":"Dataset","description":"The two-particle cumulants, V2{2} as a function of $\\eta$.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t15","@type":"Dataset","description":"The two-particle cumulants, V2{2} as a function of $\\eta$ for one particle while averaged over $\\eta$ of the partner particle.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t16","@type":"Dataset","description":"The difference in two-particle cumulants, V2{2} as a function of $\\eta$ for one particle while averaged over $\\eta$ of the...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t17","@type":"Dataset","description":"No description provided.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t18","@type":"Dataset","description":"V3{2} as a function of $\\eta$.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t19","@type":"Dataset","description":"<$V_3^2$> as a function of $\\eta$.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t20","@type":"Dataset","description":"The $\\Delta\\eta$-dependent component of the two-particle cumulant with $\\Delta\\eta$-gap, $D^-$ in Eq. (11), of the second harmonic is shown as...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t21","@type":"Dataset","description":"The $\\Delta\\eta$-dependent component of the two-particle cumulant with $\\Delta\\eta$-gap, $D^-$ in Eq. (11), of the third harmonic is shown as...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t22","@type":"Dataset","description":"The nonflow, $\\sqrt{\\bar{D}_2}$, $\\sqrt{\\delta_2}$, $\\sqrt{\\bar{D}_3}$ and flow, $\\sqrt{v_2^2/2}$, $\\sqrt{}$ results are shown as a function of centrality percentile for the...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t23","@type":"Dataset","description":"The nonflow, $\\sqrt{\\bar{D}_2}$, $\\sqrt{\\delta_2}$, $\\sqrt{\\bar{D}_3}$ and flow, $\\sqrt{v_2^2/2}$, $\\sqrt{}$ results are shown as a function of centrality percentile for the...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t24","@type":"Dataset","description":"The nonflow, $\\sqrt{\\bar{D}_2}$, $\\sqrt{\\delta_2}$, $sqrt{\\bar{D}_3}$ and flow, $\\sqrt{v_2^2/2}$, $\\sqrt{}$ results are shown as a function of centrality percentile for the...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t25","@type":"Dataset","description":"The nonflow, $\\sqrt{\\bar{D}_2}$, $\\sqrt{\\delta_2}$, $sqrt{\\bar{D}_3}$ and flow, $\\sqrt{v_2^2/2}$, $\\sqrt{}$ results are shown as a function of centrality percentile for the...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t26","@type":"Dataset","description":"The nonflow, $\\sqrt{\\bar{D}_2}$, $sqrt{\\delta_2}$, $\\sqrt{\\bar{D}_3}$ and flow, $\\sqrt{v_2^2/2}$, $\\sqrt{}$ results are shown as a function of centrality percentile for the...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.73493.v1/t27","@type":"Dataset","description":"The relative elliptic flow fluctuation $\\sigma_2/$ centrality dependence in $\\sqrt{s_{NN}}$ = 200 GeV Au+Au collisions.","name":"Table 27"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1315466?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/73493"}],"inLanguage":"en","name":"Isolation of Flow and Nonflow Correlations by Two- and Four-Particle Cumulant Measurements of Azimuthal Harmonics in $\\sqrt{s_{_{\\rm NN}}} =$ 200 GeV Au+Au Collisions","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1315466?version=1","version":1}