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J/psi nuclear modification factor (RAA) vs average Npart for 2 <pT< 5 GeV/c in Pb-Pb at 5.02 TeV

Figure Information
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
Energy
5.02 TeV
System
Pb-Pb
Figure Group
Studies of J/ψ production at forward rapidity in Pb-Pb collisions at 5.02 TeV
Figure Image
Figure image (.eps)
2019-11-02-RAAVsCent_Pt2to5.eps
Figure image (.pdf)
2019-11-02-RAAVsCent_Pt2to5.pdf
Figure Caption

p.p1 {margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px 'Helvetica Neue'}

Inclusive J/ψ nuclear modification factor as a function of average Npart for Pb–Pb collisions at \sqrt{s_{NN}}= 5.02 for 2 < pT < 5 GeV/c . The vertical error bars represent statistical uncertainties, the boxes around the points uncorrelated systematic uncertainties, while the correlated uncertainty is shown as a filled box around RAA = 1. When the corresponding results at 2.76 TeV are available, the ratio of the results at the two energies is shown in the bottom section of each figure. The RAA results at \sqrt{s_{NN}}= 5.02 TeV as well as the  ratio to the \sqrt{s_{NN}} = 2.76 TeV results are compared with transport model calculations .

Detail description

p.p1 {margin: 0.0px 0.0px 0.0px 0.0px; font: 12.0px 'Helvetica Neue'}

Inclusive J/ψ nuclear modification factor as a function of average Npart for Pb–Pb collisions at \sqrt{s_{NN}}= 5.02 for 2 < pT < 5 GeV/c . The vertical error bars represent statistical uncertainties, the boxes around the points uncorrelated systematic uncertainties, while the correlated uncertainty is shown as a filled box around RAA = 1. When the corresponding results at 2.76 TeV are available, the ratio of the results at the two energies is shown in the bottom section of each figure. The RAA results at \sqrt{s_{NN}}= 5.02 TeV as well as the  ratio to the \sqrt{s_{NN}} = 2.76 TeV results are compared with transport model calculations .