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J/psi nuclear modification factor (RAA) vs average Npart for 8 <pT< 12 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_Pt8to12.eps
Figure image (.pdf)
2019-11-02-RAAVsCent_Pt8to12.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 8 < pT < 12 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. The RAA 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 8 < pT < 12 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. The RAA results are compared with transport model calculations .