Centrality dependence of J/$ψ$ and $ψ$(2S) production and nuclear modification in p-Pb collisions at $\sqrt{s_{\rm NN}} =$ 8.16 TeV

Description
Figures from paper submitted to Journal of High Energy Physics
Abstract:

The inclusive production of the J/$\psi$ and $\psi$(2S) charmonium states is studied as a function of centrality in p-Pb collisions at a centre-of-mass energy per nucleon pair $\sqrt{s_{\rm NN}} = 8.16$ TeV at the LHC. The measurement is performed in the dimuon decay channel with the ALICE apparatus in the centre-of-mass rapidity intervals $-4.46 <~ y_{\rm cms} <~ -2.96$ (Pb-going direction) and $2.03 <~ y_{\rm cms} <~ 3.53$ (p-going direction), down to zero transverse momentum ($p_{\rm T}$). The J/$\psi$ and $\psi$(2S) production cross sections are evaluated as a function of the collision centrality, estimated through the energy deposited in the zero degree calorimeter located in the Pb-going direction. The $p_{\rm T}$-differential J/$\psi$ production cross section is measured at backward and forward rapidity for several centrality classes, together with the corresponding average $\langle p_{\rm T} \rangle$ and $\langle p^{2}_{\rm T} \rangle$ values. The nuclear effects affecting the production of both charmonium states are studied using the nuclear modification factor. In the p-going direction, a suppression of the production of both charmonium states is observed, which seems to increase from peripheral to central collisions. In the Pb-going direction, however, the centrality dependence is different for the two states: the nuclear modification factor of the J/$\psi$ increases from below unity in peripheral collisions to above unity in central collisions, while for the $\psi$(2S) it stays below or consistent with unity for all centralities with no significant centrality dependence. The results are compared with measurements in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV and no significant dependence on the energy of the collision is observed. Finally, the results are compared with theoretical models implementing various nuclear matter effects.

JHEP 02 (2021) 002
e-Print: arXiv:2008.04806 | PDF | inSPIRE

Energy
8 TeV
System
p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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Figure image (.pdf)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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Figure image (.pdf)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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Figure image (.pdf)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
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8 TeV
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p-Pb
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PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
Energy
8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
Energy
8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
Energy
8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
System
p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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8 TeV
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p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
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Figure image (.pdf)
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8 TeV
System
p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
Figure image (.eps)
Figure image (.pdf)
Energy
8 TeV
System
p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
Figure image (.eps)
Figure image (.pdf)
Energy
8 TeV
System
p-Pb
Scope: PWG
PWG-DQ (Dileptons and Quarkonia)
Figure image (.eps)
Figure image (.pdf)