Figure 6

The nuclear modification factor $R_{AA}$ of inclusive $textrm{J}/\psi$, measured atmid-rapidity ($|y| < 0.8$) in Pb-Pb collisions ($0$-$40$% mostcentral) at $\sqrt{s_{NN}}$ = 2.76 TeV, as a function of transverse momentum $p_{T}$. The filled symbols are placed at the measured $p_{T}$ for the given interval. Since for the data point in $4.5 < p_{T} < 10$ GeV$/c$ (open symbol, $0$-$50$% most central) $\langle p_{T} \rangle$ is not available due to the limited statistics, it is plotted at the centre of the $p_{T}$ interval The uncorrelated systematic uncertainties (type II) are depicted bythe open boxes, while the correlated uncertainties (type I) are shownas the filled boxes at unity The data are compared to corresponding results by PHENIX for Au-Au collisions ($0$-$40$% most central) at $\sqrt{s_{NN}}$ = 0.2 TeV, by CMS for Pb-Pb collisions ($0$-$40$% mostcentral) at $\sqrt{s_{NN}}$ = 2.76 TeV , and to predictions by the model of Zhou et al. and Zhaoet al .