{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.72886.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1419244"}},{"@id":"https://doi.org/10.1103/PhysRevLett.116.132302","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2017","description":"CERN-LHC. The anisotropic flow coefficients relative to the second, third and fourth harmonic ($v_2$, $v_3$ and $v_4$, respectively) are measured with two- and multi-particle correlation techniques in Pb-Pb collisions at 5.02 TeV, recorded in November 2015 with the ALICE detector at the CERN Large Hadron Collider.  The measurements are performed in the central pseudorapidity region (|$\\eta$| < 0.8) and transverse momentum range 0.2 < $p_{\\rm T}$ < 5.0 GeV/$c$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t1","@type":"Dataset","description":"Centrality dependence of $v_2$, with two- and multi-particle correlations, integrated over the $p_{\\rm T}$ range 0.2 < $p_{\\rm T}$ <...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t2","@type":"Dataset","description":"Centrality dependence of $v_3$ and $v_4$, with two-particle correlations, integrated over the $p_{\\rm T}$ range 0.2 < $p_{\\rm T}$ <...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t3","@type":"Dataset","description":"Centrality dependence of $v_2$, with two- and multi-particle correlations, integrated over the $p_{\\rm T}$ range 0.2 < $p_{\\rm T}$ <...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t4","@type":"Dataset","description":"Centrality dependence of $v_3$ and $v_4$, with two-particle correlations, integrated over the $p_{\\rm T}$ range 0.2 < $p_{\\rm T}$ <...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t5","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-integrated $v_2$ between $\\sqrt{s_{\\rm NN}}$ = 5.02 and 2.76 TeV.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t6","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-integrated $v_3$ and $v_4$ between $\\sqrt{s_{\\rm NN}}$ = 5.02 and 2.76 TeV.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t7","@type":"Dataset","description":"$p_{\\rm T}$ dependence of $v_2$, $v_3$ and $v_4$ for centrality 0-5%.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t8","@type":"Dataset","description":"$p_{\\rm T}$ dependence of $v_2$, $v_3$ and $v_4$ for centrality 30-40%.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t9","@type":"Dataset","description":"$p_{\\rm T}$ dependence of $v_2${4} for centralities 10-20%, 20-30% and 30-40%.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t10","@type":"Dataset","description":"Ratio of $p_{\\rm T}$-differential $v_2${4} between $\\sqrt{s_{\\rm NN}}$ = 5.02 and 2.76 TeV, for centrality 20-30%.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.72886.v2/t11","@type":"Dataset","description":"Fully $p_{\\rm T}$-integrated $v_2${4} at $\\sqrt{s_{\\rm NN}}$ = 2.76 and 5.02 TeV, for centrality 20-30%.","name":"Table 11"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1419244?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/72886"}],"inLanguage":"en","name":"Anisotropic flow of charged particles in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}=5.02$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1419244?version=2","version":2}