{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.83737.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1666817"}},{"@id":"https://doi.org/10.1007/JHEP07(2018)103","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2018","description":"Measurements of anisotropic flow coefficients with two- and multi-particle cumulants for inclusive charged particles in Pb--Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ and 2.76 TeV are reported in the pseudorapidity range $|\\eta| < 0.8$ and transverse momentum $0.2 < p_\\text{T} < 50$ GeV/$c$. The full data sample collected by the ALICE detector in 2015 (2010), corresponding to an integrated luminosity of 12.7 (2.0) $\\mu$b$^{-1}$ in the centrality range 0-80$\\%$, is analysed. Flow coefficients up to the sixth flow harmonic ($v_6$) are reported and a detailed comparison among results at the two energies is carried out. The $p_\\text{T}$ dependence of anisotropic flow coefficients and its evolution with respect to centrality and harmonic number $n$ are investigated. An approximate power-law scaling of the form $v_n(p_\\text{T}) \\sim p_\\text{T}^{n/3}$ is observed for all flow harmonics at low $p_\\text{T}$ ($0.2 < p_\\text{T} < 3$ GeV/$c$). At the same time, the ratios $v_n/v_m^{n/m}$ are observed to be essentially independent of $p_\\text{T}$ for most centralities up to about $p_\\text{T} = 10$ GeV/$c$. Analysing the differences among higher-order cumulants of elliptic flow ($v_2$), which have different sensitivities to flow fluctuations, a measurement of the standardised skewness of the event-by-event $v_2$ distribution $P(v_2)$ is reported and constraints on its higher moments are provided. The Elliptic Power distribution is used to parametrise $P(v_2)$, extracting its parameters from fits to cumulants. The measurements are compared to different model predictions in order to discriminate among initial-state models and to constrain the temperature dependence of the shear viscosity to entropy-density ratio.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t1","@type":"Dataset","description":"$v_2\\{2,|\\Delta\\eta| > 1.\\}$ as a function of centrality for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t2","@type":"Dataset","description":"$v_2\\{4\\}$ as a function of centrality for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t3","@type":"Dataset","description":"$v_3\\{2,|\\Delta\\eta| > 1.\\}$ as a function of centrality for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t4","@type":"Dataset","description":"$v_4\\{2,|\\Delta\\eta| > 1.\\}$ as a function of centrality for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t5","@type":"Dataset","description":"$v_5\\{2,|\\Delta\\eta| > 1.\\}$ as a function of centrality for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t6","@type":"Dataset","description":"$v_6\\{2,|\\Delta\\eta| > 1.\\}$ as a function of centrality for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t7","@type":"Dataset","description":"$v_2\\{2,|\\Delta\\eta| > 1.\\}$ as a function of centrality for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t8","@type":"Dataset","description":"$v_2\\{4\\}$ as a function of centrality for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV.","name":"Table 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$v_3\\{2,|\\Delta\\eta| > 1.\\}$ at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and 2.76 TeV as a function of centrality.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t14","@type":"Dataset","description":"ratio of $v_4\\{2,|\\Delta\\eta| > 1.\\}$ at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and 2.76 TeV as a function of centrality.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t15","@type":"Dataset","description":"$v_2\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 0-5$\\%$ as a function of $p_\\text{T}$.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t16","@type":"Dataset","description":"$v_2\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 0-5$\\%$ as a function of $p_\\text{T}$.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t17","@type":"Dataset","description":"$v_3\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb 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1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 0-5$\\%$ as a function of $p_\\text{T}$.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t22","@type":"Dataset","description":"$v_6\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 0-5$\\%$ as a function of $p_\\text{T}$.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t23","@type":"Dataset","description":"$v_2\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 5-10$\\%$ as a function of $p_\\text{T}$.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t24","@type":"Dataset","description":"$v_2\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 5-10$\\%$ as a function of $p_\\text{T}$.","name":"Table 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$p_\\text{T}$.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t29","@type":"Dataset","description":"$v_5\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 5-10$\\%$ as a function of $p_\\text{T}$.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t30","@type":"Dataset","description":"$v_6\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 5-10$\\%$ as a function of $p_\\text{T}$.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t31","@type":"Dataset","description":"$v_2\\{4\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 5-10$\\%$ as a function of $p_\\text{T}$.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t32","@type":"Dataset","description":"$v_2\\{4\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 5-10$\\%$ as a function of 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10-20$\\%$ as a function of $p_\\text{T}$.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t37","@type":"Dataset","description":"$v_4\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 10-20$\\%$ as a function of $p_\\text{T}$.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t38","@type":"Dataset","description":"$v_4\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 10-20$\\%$ as a function of $p_\\text{T}$.","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t39","@type":"Dataset","description":"$v_5\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 10-20$\\%$ as a function of $p_\\text{T}$.","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t40","@type":"Dataset","description":"$v_6\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 10-20$\\%$ as a function of $p_\\text{T}$.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t41","@type":"Dataset","description":"$v_2\\{4\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 10-20$\\%$ as a function of $p_\\text{T}$.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t42","@type":"Dataset","description":"$v_2\\{4\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 10-20$\\%$ as a function of $p_\\text{T}$.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t43","@type":"Dataset","description":"$v_2\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t44","@type":"Dataset","description":"$v_2\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t45","@type":"Dataset","description":"$v_3\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t46","@type":"Dataset","description":"$v_3\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t47","@type":"Dataset","description":"$v_4\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t48","@type":"Dataset","description":"$v_4\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t49","@type":"Dataset","description":"$v_5\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t50","@type":"Dataset","description":"$v_6\\{2,|\\Delta\\eta| > 1.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t51","@type":"Dataset","description":"$v_2\\{4\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 20-30$\\%$ as a function of $p_\\text{T}$.","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t52","@type":"Dataset","description":"$v_2\\{4\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm 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centrality 60-70$\\%$ as a function of $p_\\text{T}$.","name":"Table 133"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t134","@type":"Dataset","description":"$v_3\\{2,|\\Delta\\eta| > 2.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV and centrality 60-70$\\%$ as a function of $p_\\text{T}$.","name":"Table 134"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t135","@type":"Dataset","description":"$v_4\\{2,|\\Delta\\eta| > 2.\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 60-70$\\%$ as a function of $p_\\text{T}$.","name":"Table 135"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t136","@type":"Dataset","description":"ratio of $v_2\\{2,|\\Delta\\eta| > 1.\\}$ at $\\sqrt{s_{\\rm NN}} = 5.02$ and 2.76 TeV and centrality 5-10$\\%$ as a function of...","name":"Table 137"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t137","@type":"Dataset","description":"ratio of $v_3\\{2,|\\Delta\\eta| > 1.\\}$ at $\\sqrt{s_{\\rm NN}} = 5.02$ and 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210"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t210","@type":"Dataset","description":"$v_2\\{8\\}/v_2\\{4\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV as a function of centrality.","name":"Table 211"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t211","@type":"Dataset","description":"$v_2\\{8\\}/v_2\\{4\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 2.76$ TeV as a function of centrality.","name":"Table 212"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t212","@type":"Dataset","description":"$v_2\\{8\\}/v_2\\{6\\}$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV as a function of centrality.","name":"Table 213"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t213","@type":"Dataset","description":"$(v_2\\{4\\}-v_2\\{6\\})/11$ for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV as a function of centrality.","name":"Table 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, for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 0-5$\\%$","name":"Table 223"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t223","@type":"Dataset","description":"Elliptic Power distribution P(v2), rescaled by , for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 10-15$\\%$","name":"Table 224"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t224","@type":"Dataset","description":"Elliptic Power distribution P(v2), rescaled by , for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 15-20$\\%$","name":"Table 225"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t225","@type":"Dataset","description":"Elliptic Power distribution P(v2), rescaled by , for Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV and centrality 20-25$\\%$","name":"Table 226"},{"@id":"https://doi.org/10.17182/hepdata.83737.v1/t226","@type":"Dataset","description":"Elliptic Power distribution P(v2), rescaled by , for Pb-Pb collisions at 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