Showing 7 of 7 results
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.
The elliptic flow of inclusive and direct photons was measured at mid-rapidity in two centrality classes 0-20% and 20-40% in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV by ALICE. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the detector material with the $e^{+}e^{-}$ pairs reconstructed in the central tracking system. The results of the two methods were combined and the direct photon elliptic flow was extracted in the transverse momentum range $0.9 < p_{\rm T} < 6.2$ GeV/$c$. A comparison to RHIC data shows a similar magnitude of the measured direct-photon elliptic flow. Hydrodynamic and transport model calculations are systematically lower than the data, but are found to be compatible.
Ratio V2{GAMMA,INCLUSIVE,PCM}/V2{GAMMA,INCLUSIVE,COMBINED} as function of $p_\text{T}$, collision centrality 0-20%, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
Ratio V2{GAMMA,INCLUSIVE,PHOS}/V2{GAMMA,INCLUSIVE,COMBINED} as function of $p_\text{T}$, collision centrality 20-40%, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
V2{GAMMA,DECAY} as function of $p_\text{T}$, collision centrality 0-20%, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
V2{GAMMA,DECAY} as function of $p_\text{T}$, collision centrality 20-40%, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
V2{GAMMA,INCLUSIVE} as function of $p_\text{T}$, collision centrality 0-20%, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
V2{GAMMA,INCLUSIVE} as function of $p_\text{T}$, collision centrality 20-40%, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
V2{GAMMA,DIRECT} as function of $p_\text{T}$, collision centrality 0-20%, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
V2{GAMMA,DIRECT} as function of $p_\text{T}$, collision centrality 20-40%, for Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
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 measurement of azimuthal correlations of charged particles is presented for Pb-Pb collisions at $\sqrt{s_{\rm NN}}=$ 2.76 TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}=$ 5.02 TeV with the ALICE detector at the CERN Large Hadron Collider. These correlations are measured for the second, third and fourth order flow vector in the pseudorapidity region $|\eta|<0.8$ as a function of centrality and transverse momentum $p_{\rm T}$ using two observables, to search for evidence of $p_{\rm T}$-dependent flow vector fluctuations. For Pb-Pb collisions at 2.76 TeV, the measurements indicate that $p_{\rm T}$-dependent fluctuations are only present for the second order flow vector. Similar results have been found for p-Pb collisions at 5.02 TeV. These measurements are compared to hydrodynamic model calculations with event-by-event geometry fluctuations in the initial state to constrain the initial conditions and transport properties of the matter created in Pb-Pb and p-Pb collisions.
$v_2\{2\}$ with $|\eta| > 0.0$ for centrality class 0-5\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.0$ for centrality class 5-10\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.0$ for centrality class 10-20\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.0$ for centrality class 20-30\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.0$ for centrality class 30-40\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.0$ for centrality class 40-50\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.0$ for centrality class 50-60\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.0$ for centrality class 60-70\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.4$ for centrality class 0-5\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.4$ for centrality class 5-10\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.4$ for centrality class 10-20\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.4$ for centrality class 20-30\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.4$ for centrality class 30-40\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.4$ for centrality class 40-50\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.4$ for centrality class 50-60\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.4$ for centrality class 60-70\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.8$ for centrality class 0-5\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.8$ for centrality class 5-10\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.8$ for centrality class 10-20\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.8$ for centrality class 20-30\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.8$ for centrality class 30-40\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.8$ for centrality class 40-50\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.8$ for centrality class 50-60\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
$v_2\{2\}$ with $|\eta| > 0.8$ for centrality class 60-70\% in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV.
In ultrarelativistic heavy-ion collisions, the event-by-event variation of the elliptic flow $v_2$ reflects fluctuations in the shape of the initial state of the system. This allows to select events with the same centrality but different initial geometry. This selection technique, Event Shape Engineering, has been used in the analysis of charge-dependent two- and three-particle correlations in Pb-Pb collisions at $\sqrt{s_{_{\rm NN}}} =2.76$ TeV. The two-particle correlator $\langle \cos(\varphi_\alpha - \varphi_\beta) \rangle$, calculated for different combinations of charges $\alpha$ and $\beta$, is almost independent of $v_2$ (for a given centrality), while the three-particle correlator $\langle \cos(\varphi_\alpha + \varphi_\beta - 2\Psi_2) \rangle$ scales almost linearly both with the event $v_2$ and charged-particle pseudorapidity density. The charge dependence of the three-particle correlator is often interpreted as evidence for the Chiral Magnetic Effect (CME), a parity violating effect of the strong interaction. However, its measured dependence on $v_2$ points to a large non-CME contribution to the correlator. Comparing the results with Monte Carlo calculations including a magnetic field due to the spectators, the upper limit of the CME signal contribution to the three-particle correlator in the 10-50% centrality interval is found to be 26-33% at 95% confidence level.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for unbiased events in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (0-10% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (10-20% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (20-30% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (30-40% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (40-50% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (50-60% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (60-70% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (70-80% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (80-90% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$v_2\{EP\}$ with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (90-100% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for unbiased events in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (0-10% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (10-20% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (20-30% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (30-40% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (40-50% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (50-60% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (60-70% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (70-80% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (80-90% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (90-100% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for unbiased events in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (0-10% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (10-20% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (20-30% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (30-40% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (40-50% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (50-60% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (60-70% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (70-80% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (80-90% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (same charge pairs) with $|\Delta\eta| > 2.0$ as a function of centrality for shape selected events (90-100% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for unbiased events in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (0-10% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (10-20% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (20-30% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (30-40% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (40-50% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (50-60% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (60-70% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (70-80% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (80-90% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (opposite charge pairs) as a function of centrality for shape selected events (90-100% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for unbiased events in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (0-10% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (10-20% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (20-30% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (30-40% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (40-50% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (50-60% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (60-70% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (70-80% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (80-90% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} - \varphi_{\beta}) \rangle$ (same charge pairs) as a function of centrality for shape selected events (90-100% $q_2$) in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ as a function of $v_2\{EP\}$ for centrality class 0-5% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ as a function of $v_2\{EP\}$ for centrality class 5-10% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ as a function of $v_2\{EP\}$ for centrality class 10-20% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ as a function of $v_2\{EP\}$ for centrality class 20-30% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ as a function of $v_2\{EP\}$ for centrality class 30-40% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ as a function of $v_2\{EP\}$ for centrality class 40-50% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ as a function of $v_2\{EP\}$ for centrality class 50-60% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\eta$, as a function of $v_2\{EP\}$ for centrality class 0-5% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\eta$, as a function of $v_2\{EP\}$ for centrality class 5-10% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\eta$, as a function of $v_2\{EP\}$ for centrality class 10-20% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\eta$, as a function of $v_2\{EP\}$ for centrality class 20-30% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\eta$, as a function of $v_2\{EP\}$ for centrality class 30-40% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\eta$, as a function of $v_2\{EP\}$ for centrality class 40-50% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ multiplied by the charged-particle density, $dN/d\eta$, as a function of $v_2\{EP\}$ for centrality class 50-60% in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
$p_1$ parameter from a linear fit to $\langle \cos(\varphi_{\alpha} + \varphi_{\beta} - 2\Psi_{2}) \rangle$ (opposite - same) with $|\Delta\eta| > 2.0$ as a function of centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
CME fraction extracted from the slope parameter of fits to data and MC—Glauber model as a function of centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
CME fraction extracted from the slope parameter of fits to data and MC—KLN CGC model as a function of centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
CME fraction extracted from the slope parameter of fits to data and EKRT model as a function of centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.
Multi-particle cumulants and corresponding Fourier harmonics are measured for azimuthal angle distributions of charged particles in $pp$ collisions at $\sqrt{s}$ = 5.02 and 13 TeV and in $p$+Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV, and compared to the results obtained for low-multiplicity Pb+Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV. These measurements aim to assess the collective nature of particle production. The measurements of multi-particle cumulants confirm the evidence for collective phenomena in $p$+Pb and low-multiplicity Pb+Pb collisions. On the other hand, the $pp$ results for four-particle cumulants do not demonstrate collective behaviour, indicating that they may be biased by contributions from non-flow correlations. A comparison of multi-particle cumulants and derived Fourier harmonics across different collision systems is presented as a function of the charged-particle multiplicity. For a given multiplicity, the measured Fourier harmonics are largest in Pb+Pb, smaller in $p$+Pb and smallest in $pp$ collisions. The $pp$ results show no dependence on the collision energy, nor on the multiplicity.
$c_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $N_{ch}(p_T < 0.4 GeV)$ (EvSel_$N_{ch}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $N_{ch}(p_T < 0.4 GeV)$ (EvSel_$N_{ch}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $N_{ch}(p_T < 0.4 GeV)$ (EvSel_$N_{ch}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $N_{ch}(p_T < 0.4 GeV)$ (EvSel_$N_{ch}$) for PbPb collisions at $\sqrt{ s_{NN} }$=2.76 TeV.
$c_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{2, | \Delta \eta > 2 \}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_2\{2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_2\{2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_2\{2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{2, | \Delta \eta > 2 \}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{4\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_2\{6\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{6\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_2\{6\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{6\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_2\{8\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{8\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_2\{8\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_2\{8\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$v_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$v_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{2, | \Delta \eta > 2 \}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$v_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$v_2\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{2, | \Delta \eta > 2 \}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{6\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{8\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{4\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{6\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{8\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{4\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{6\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{8\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{4\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{6\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{8\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{4\}/v_2\{2, | \Delta \eta > 2 \}$ ratio for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{6\}/v_2\{4\}$ ratio for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{8\}/v_2\{6\}$ ratio for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{4\}/v_2\{2, | \Delta \eta > 2 \}$ ratio for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{6\}/v_2\{4\}$ ratio for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{8\}/v_2\{6\}$ ratio for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{4\}/v_2\{2, | \Delta \eta > 2 \}$ ratio for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{6\}/v_2\{4\}$ ratio for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{8\}/v_2\{6\}$ ratio for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_2\{4\}/v_2\{2, | \Delta \eta > 2 \}$ ratio for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{6\}/v_2\{4\}$ ratio for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_2\{8\}/v_2\{6\}$ ratio for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_3\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_3\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_3\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_3\{2, | \Delta \eta > 2 \}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_3\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_3\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_3\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_3\{2, | \Delta \eta > 2 \}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_4\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_4\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_4\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_4\{2, | \Delta \eta > 2 \}$ cumulants for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$c_4\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$c_4\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$c_4\{2, | \Delta \eta > 2\}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$c_4\{2, | \Delta \eta > 2 \}$ cumulants for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_3\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$v_3\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_3\{2, | \Delta \eta > 2 \}$ harmonics for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_3\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_3\{2, | \Delta \eta > 2 \}$ harmonics for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_4\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$v_4\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$v_4\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_4\{2, | \Delta \eta > 2 \}$ harmonics for reference particles with 0.3 $< p_T <$ 3.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$v_4\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 5.02 TeV.
$v_4\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pp collisions at $\sqrt{s}$= 13 TeV.
$v_4\{2, | \Delta \eta > 2\}$ harmonics for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for pPb collisions at $\sqrt{ s_{NN} }$= 5.02 TeV.
$v_4\{2, | \Delta \eta > 2 \}$ harmonics for reference particles with 0.5 $< p_T <$ 5.0 GeV selected according to $M_{ref}$ (EvSel_$M_{ref}$) for PbPb collisions at $\sqrt{ s_{NN} }$= 2.76 TeV.
$ v_2\{4\} $ harmonics for reference particles with 0.2 $ < p_{T} < $ 3.0 GeV as a function of $ < N_{ch}(|\eta|<1) > $ for p+Pb collisions at $ \sqrt{ s_{NN} } $= 5.02 TeV.
$ v_2\{4\} $ harmonics for reference particles with 0.2 $ < p_{T}< $ 3.0 GeV as a function of $ < N_{ch}(|\eta|<1) > $ for Pb+Pb collisions at $ \sqrt{ s_{NN} } $= 2.76 TeV.
ATLAS measurements of the azimuthal anisotropy in lead-lead collisions at $\sqrt{s_{NN}}=2.76$ TeV are shown using a dataset of approximately 7 $\mu$b$^{-1}$ collected at the LHC in 2010. The measurements are performed for charged particles with transverse momenta $0.5<p_T<20$ GeV and in the pseudorapidity range $|\eta|<2.5$. The anisotropy is characterized by the Fourier coefficients, $v_n$, of the charged-particle azimuthal angle distribution for n = 2-4. The Fourier coefficients are evaluated using multi-particle cumulants calculated with the generating function method. Results on the transverse momentum, pseudorapidity and centrality dependence of the $v_n$ coefficients are presented. The elliptic flow, $v_2$, is obtained from the two-, four-, six- and eight-particle cumulants while higher-order coefficients, $v_3$ and $v_4$, are determined with two- and four-particle cumulants. Flow harmonics $v_n$ measured with four-particle cumulants are significantly reduced compared to the measurement involving two-particle cumulants. A comparison to $v_n$ measurements obtained using different analysis methods and previously reported by the LHC experiments is also shown. Results of measurements of flow fluctuations evaluated with multi-particle cumulants are shown as a function of transverse momentum and the collision centrality. Models of the initial spatial geometry and its fluctuations fail to describe the flow fluctuations measurements.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 0-2%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 2-5%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 10-15%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 20-25%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 30-35%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 40-45%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 45-50%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 50-55%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 55-60%.
The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 60-80%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 0-2%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 2-5%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 10-15%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 20-25%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 30-35%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 40-45%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 45-50%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 50-55%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 55-60%.
The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 60-80%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 2-5%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 10-15%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 20-25%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 30-35%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 40-45%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 45-50%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 50-55%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 55-60%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 60-80%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 2-5%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 10-15%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 20-25%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 30-35%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 40-45%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 45-50%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 50-55%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 55-60%.
The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 60-80%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 2-5%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 10-15%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 20-25%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 30-35%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 40-45%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 45-50%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 50-55%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 55-60%.
The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 60-80%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 40-50%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 10-20%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 20-30%.
The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 30-40%.
The triangular flow harmonic measured with the two-particle cumulats as a function of transverse momentum in centrality bin 0-25%.
The triangular flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 0-25%.
The triangular flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 0-25%.
The triangular flow harmonic measured with the two-particle cumulats as a function of transverse momentum in centrality bin 25-60%.
The triangular flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 25-60%.
The triangular flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 25-60%.
The quadrangular flow harmonic measured with the two-particle cumulats as a function of transverse momentum in centrality bin 0-25%.
The quadrangular flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 0-25%.
The quadrangular flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 0-25%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 0-2%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 2-5%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 5-10%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 10-15%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 15-20%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 20-25%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 25-30%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 30-35%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 35-40%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 40-45%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 45-50%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 50-55%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 55-60%.
The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 60-80%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 0-2%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 2-5%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 5-10%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 10-15%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 15-20%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 20-25%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 25-30%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 30-35%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 35-40%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 40-45%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 45-50%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 50-55%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 55-60%.
The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 60-80%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 2-5%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 5-10%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 10-15%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 15-20%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 20-25%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 25-30%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 30-35%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 35-40%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 40-45%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 45-50%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 50-55%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 55-60%.
The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 60-80%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 2-5%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 5-10%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 10-15%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 15-20%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 20-25%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 25-30%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 30-35%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 35-40%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 40-45%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 45-50%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 50-55%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 55-60%.
The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 60-80%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 2-5%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 5-10%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 10-15%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 15-20%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 20-25%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 25-30%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 30-35%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 35-40%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 40-45%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 45-50%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 50-55%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 55-60%.
The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 60-80%.
The triangular flow harmonic measured with the two-particle cumulats as a function of pseudorapidity in centrality bin 0-60%.
The triangular flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 0-60%.
The triangular flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 0-60%.
The quadrangular flow harmonic measured with the two-particle cumulats as a function of pseudorapidity in centrality bin 0-25%.
The quadrangular flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 0-25%.
The quadrangular flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 0-25%.
The second flow harmonic measured with the two-particle cumulats as a function of <Npart>.
The second flow harmonic measured with the four-particle cumulats as a function of <Npart>.
The second flow harmonic measured with the six-particle cumulats as a function of <Npart>.
The second flow harmonic measured with the eight-particle cumulats as a function of <Npart>.
The ratio of second flow harmonics measured with the six- and four-particle cumulants as a function of <Npart>.
The ratio of second flow harmonics measured with the eight- and four-particle cumulants as a function of <Npart>.
The second flow harmonic measured with the Event Plane method as a function of <Npart>.
The triangular flow harmonic measured with the Event Plane method as a function of <Npart>.
The triangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.
The triangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.
The quadrangular flow harmonic measured with the Event Plane method as a function of <Npart>.
The quadrangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.
The quadrangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 2-5%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 10-15%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 20-25%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 30-35%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 40-45%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 45-50%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 50-55%.
The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 55-60%.
The second flow harmonic fluctuations, F(v2), as a function of <Npart>.
The triangular flow harmonic fluctuations, F(v3), as a function of <Npart>.
The triangular flow harmonic fluctuations, F(v4), as a function of <Npart>.
The second flow harmonic measured with the two-particle cumulats as a function of <Npart>.
The second flow harmonic measured with the four-particle cumulats as a function of <Npart>.
The second flow harmonic measured with the six-particle cumulats as a function of <Npart>.
The second flow harmonic measured with the eight-particle cumulats as a function of <Npart>.
The ratio of second flow harmonics measured with the six- and four-particle cumulants as a function of <Npart>.
The ratio of second flow harmonics measured with the eight- and four-particle cumulants as a function of <Npart>.
The triangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.
The quadrangular flow harmonic measured with the Event Plane method as a function of <Npart>.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 2-5%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 10-15%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 20-25%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 30-35%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 40-45%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 45-50%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 50-55%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 55-60%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 2-5%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 5-10%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 10-15%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 15-20%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 20-25%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 25-30%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 30-35%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 35-40%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 40-45%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 45-50%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 50-55%.
The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 55-60%.
The second flow harmonic fluctuations, F(v2), as a function of <Npart>.
The triangular flow harmonic fluctuations, F(v3), as a function of <Npart>.
The triangular flow harmonic fluctuations, F(v4), as a function of <Npart>.
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