Showing 2 of 2 results
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$\%$
The second and the third order anisotropic flow, $V_{2}$ and $V_3$, are mostly determined by the corresponding initial spatial anisotropy coefficients, $\varepsilon_{2}$ and $\varepsilon_{3}$, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, $V_n$ ($n > 3$), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow $V_n$ for $n=4$, $5$, $6$ with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range $|\eta| < 0.8$ and the transverse momentum range $0.2 < p_{\rm T} < 5.0$ GeV/$c$ as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the initial conditions, including initial spatial geometry and its fluctuations, as well as the ratio of the shear viscosity to entropy density of the produced system.
Study of relationship between linear and non-linear modes in higher order anisotropic flow in Pb–Pb collisions at 2.76 TeV.
Study of relationship between linear and non-linear modes in higher order anisotropic flow in Pb–Pb collisions at 2.76 TeV.
Study of relationship between linear and non-linear modes in higher order anisotropic flow in Pb–Pb collisions at 2.76 TeV.
Study of relationship between linear and non-linear modes in higher order anisotropic flow in Pb–Pb collisions at 2.76 TeV.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
Centrality dependence of rho_mn in Pb–Pb collisions at 2.76 TeV.
Centrality dependence of rho_mn in Pb–Pb collisions at 2.76 TeV.
Centrality dependence of rho_mn in Pb–Pb collisions at 2.76 TeV.
Centrality dependence of rho_mn in Pb–Pb collisions at 2.76 TeV.
Centrality dependence of chi in Pb–Pb collisions at 2.76 TeV.
Centrality dependence of chi in Pb–Pb collisions at 2.76 TeV.
Centrality dependence of chi in Pb–Pb collisions at 2.76 TeV.
Centrality dependence of chi in Pb–Pb collisions at 2.76 TeV.
When you search on a word, e.g. 'collisions', we will automatically search across everything we store about a record. But, sometimes you may wish to be more specific. Here we show you how.
Guidance and examples on the query string syntax can be found in the Elasticsearch documentation.
About HEPData Submitting to HEPData HEPData File Formats HEPData Coordinators HEPData Terms of Use HEPData Cookie Policy
Status
Email
Forum
Twitter
GitHub
Copyright ~1975-Present, HEPData | Powered by Invenio, funded by STFC, hosted and originally developed at CERN, supported and further developed at IPPP Durham.