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Mid-rapidity ($|\eta| < 1$) measurements of $c_{2}\{2\}$ as a function of multiplicity for $p$-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Mid-rapidity ($|\eta| < 1$) measurements of $c_{2}\{2\}$ as a function of multiplicity in Pb-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Comparison of $c_{2}\{2\}$ with $|\Delta \eta| > 1.4 $ for $p$-Pb and Pb-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Mid-rapidity ($|\eta| < 1$) measurements of $c_{2}\{4\}$ as a function of multiplicity for $p$-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties. The right panel shows a zoomed in version of the solid points in the left panel.
Left Panel: Mid-rapidity ($|\eta| < 1$) measurements of $c_{2}\{4\}$ as a function of multiplicity for Pb-Pb collisions. Right Panel: Comparison of $c_{2}\{4\}$ for $p$-Pb and Pb-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Left Panel: Mid-rapidity ($|\eta| < 1$) measurements of $c_{2}\{4\}$ as a function of multiplicity for Pb-Pb collisions. Right Panel: Comparison of $c_{2}\{4\}$ for $p$-Pb and Pb-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Comparison of mid-rapidity ($|\eta| < 1$) $c_{2}\{6\}$ for $p$-Pb and Pb-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Comparison of $c_{2}\{m\}$ in very high-multiplicity Pb-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Measurements of $v_{2}\{2\}$, $v_{2}\{4\}$, and $v_{2}\{6\}$ in $p$-Pb (left panel) and Pb-Pb (right panel) collisions. The measurements of $v_{2}\{2\}$ are obtained with a $|\Delta \eta| > 1.4$ gap. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Left Panel: Measurements of $[ (v_{2}\{2\}^{2}-v_{2}\{4\}^{2})/(v_{2}\{2\}^{2}+v_{2}\{4\}^{2})]^{1/2}$ in $p$-Pb and Pb-Pb collisions. The measurements of $v_{2}\{2\}$ are obtained with a $|\Delta \eta| > 1.4$ gap. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties. Right Panel: $\sigma_{v2} / \langle v_{2} \rangle$ obtained from the same $v_{2}\{2\}$ and $v_{2}\{4\}$ measurements assuming a Bessel-Gaussian distribution.
Third harmonic two-particle cumulants in $p$-Pb and Pb-Pb collisions. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.
Third harmonic flow coefficients in $p$-Pb and Pb-Pb collisions. The measurements of $v_{3}\{2\}$ are obtained with a $|\Delta \eta| > 1.4$ gap. Only statistical errors are shown as these dominate the uncertainty. See table \ref{tab:sysPb} for systematic uncertainties.