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Measurements of anisotropic flow coefficients with two- and multi-particle cumulants for inclusive charged particles in Pb-Pb collisions at $\sqrt{{\textit s}_\text{NN}} = 5.02$ 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.
$v_2\{2,|\Delta\eta| > 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
$v_2\{4\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
$v_3\{2,|\Delta\eta| > 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
$v_4\{2,|\Delta\eta| > 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
$v_5\{2,|\Delta\eta| > 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
$v_6\{2,|\Delta\eta| > 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.
$v_2\{2,|\Delta\eta| > 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{4\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_3\{2,|\Delta\eta| > 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_4\{2,|\Delta\eta| > 1.\}$ as a function of centrality for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
ratio of $v_2\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ TeV and 2.76 TeV as a function of centrality.
ratio of $v_2\{4\}$ at $\sqrt{s_{\rm NN}} = 5.02$ TeV and 2.76 TeV as a function of centrality.
ratio of $v_3\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ TeV and 2.76 TeV as a function of centrality.
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.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_5\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_6\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_5\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_6\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_5\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_6\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_5\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_6\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_5\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_6\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_5\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_6\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_5\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 1.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
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 $p_\text{T}$.
ratio of $v_3\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
ratio of $v_4\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
ratio of $v_2\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
ratio of $v_3\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
ratio of $v_4\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
ratio of $v_2\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
ratio of $v_3\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
ratio of $v_4\{2,|\Delta\eta| > 1.\}$ at $\sqrt{s_{\rm NN}} = 5.02$ and 2.76 TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_2\{2,|\Delta\eta| > 2.\}_{\text{ratio to 20-30}\%}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_3\{2,|\Delta\eta| > 2.\}^{4/3}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_3\{2,|\Delta\eta| > 2.\}^{4/3}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_3\{2,|\Delta\eta| > 2.\}^{4/3}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_3\{2,|\Delta\eta| > 2.\}^{4/3}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_3\{2,|\Delta\eta| > 2.\}^{4/3}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_3\{2,|\Delta\eta| > 2.\}^{4/3}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_3\{2,|\Delta\eta| > 2.\}^{4/3}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_3\{2,|\Delta\eta| > 2.\}^{4/3}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{4/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{4/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{4/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{4/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{4/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{4/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{4/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_4\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{4/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{3/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{3/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{3/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-20$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{3/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-30$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{3/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-40$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{3/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-50$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{3/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-60$\%$ as a function of $p_\text{T}$.
$v_3\{2,|\Delta\eta| > 2.\}/v_2\{2,|\Delta\eta| > 2.\}^{3/2}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 60-70$\%$ as a function of $p_\text{T}$.
$v_2\{2\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$v_2\{6\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$v_2\{8\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$v_2\{2\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$v_2\{6\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$v_2\{8\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$c_2\{2\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$c_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$c_2\{6\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$c_2\{8\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$c_2\{2\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$c_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$c_2\{6\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$c_2\{8\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$v_2\{6\}/v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$v_2\{6\}/v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$v_2\{8\}/v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$v_2\{8\}/v_2\{4\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV as a function of centrality.
$v_2\{8\}/v_2\{6\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$(v_2\{4\}-v_2\{6\})/11$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$v_2\{6\}-v_2\{8\}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
$\gamma_{1}^{exp}$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
Elliptic Power parameter $k_2$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
Elliptic Power parameter $\alpha$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
Elliptic Power parameter $\varepsilon_0$ for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of centrality.
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 5-10$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 25-30$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 45-50$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 0-5$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 10-15$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 15-20$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 20-25$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 30-35$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 35-40$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 40-45$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 50-55$\%$
Elliptic Power distribution P(v2), rescaled by <v2>, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and centrality 55-60$\%$
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