Abstract

The inclusive J/ψ production in Pb–Pb collisions at the center-of-mass energy per nucleon pair sqrt{s_{mathrm{NN}}} = 5.02 TeV, measured with the ALICE detector at the CERN LHC, is reported. The J/ψ meson is reconstructed via the dimuon decay channel at forward rapidity (2.5 < y < 4) down to zero transverse momentum. The suppression of the J/ψ yield in Pb–Pb collisions with respect to binary-scaled pp collisions is quantified by the nuclear modification factor (RAA). The RAA at sqrt{s_{mathrm{NN}}} = 5.02 TeV is presented and compared with previous measurements at sqrt{s_{mathrm{NN}}} = 2.76 TeV as a function of the centrality of the collision, and of the J/ψ transverse momentum and rapidity. The inclusive J/ψ RAA shows a suppression increasing toward higher transverse momentum, with a steeper dependence for central collisions. The modification of the J/ψ average transverse momentum and average squared transverse momentum is also studied. Comparisons with the results of models based on a transport equation and on statistical hadronization are carried out.

Highlights

  • 5.02 TeV function is of presented and the centrality compared with of the collision, and of the J/ψ transverse momentum and rapidity

  • The inclusive J/ψ RAA shows a suppression increasing toward higher transverse momentum, with a steeper dependence for central collisions

  • It is worth noting that the regeneration contribution should favour low transverse momentum J/ψ, as the bulk of charm quarks are produced at small momenta [21, 22]

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Summary

Apparatus and data sample

The ALICE detector and its performance are extensively described in refs. [39] and [40], respectively. The V0 [42], composed of two arrays of 32 scintillator tiles each, and located on both sides of the IP, covers 2.8 < η < 5.1 (V0A) and −3.7 < η < −1.7 (V0C), and is used as a trigger detector, for the centrality determination and to remove beam-induced background. The current analysis exploits the data samples of Pb–Pb collisions at √sNN = 5.02 TeV collected during 2015 This corresponds to an integrated luminosity LPinbtPb ≈ 225 μb−1

Data analysis
Nuclear modification factor
Centrality dependence of RAA
Conclusions
Full Text
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