Centrality, rapidity and transverse momentum dependence of J/ψ suppression in Pb–Pb collisions at sNN=2.76 TeV

B. Abelev (Lawrence Livermore National Laboratory, Livermore, CA, United States) ; J. Adam (Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic) ; D. Adamová (Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic) ; M.M. Aggarwal (Physics Department, Panjab University, Chandigarh, India) ; G. Aglieri Rinella (European Organization for Nuclear Research (CERN), Geneva, Switzerland) ; et al. - Show all 948 authors

The inclusive J/ψ nuclear modification factor ( RAA ) in Pb–Pb collisions at sNN=2.76 TeV has been measured by ALICE as a function of centrality in the e+e− decay channel at mid-rapidity ( |y|<0.8 ) and as a function of centrality, transverse momentum and rapidity in the μ+μ− decay channel at forward-rapidity ( 2.5<y<4 ). The J/ψ yields measured in Pb–Pb are suppressed compared to those in pp collisions scaled by the number of binary collisions. The RAA integrated over a centrality range corresponding to 90% of the inelastic Pb–Pb cross section is 0.72±0.06(stat.)±0.10(syst.) at mid-rapidity and 0.58±0.01(stat.)±0.09(syst.) at forward-rapidity. At low transverse momentum, significantly larger values of RAA are measured at forward-rapidity compared to measurements at lower energy. These features suggest that a contribution to the J/ψ yield originates from charm quark (re)combination in the deconfined partonic medium.

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  "control_number": "3202", 
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      "title": "Centrality, rapidity and transverse momentum dependence of J/\u00cf\u0088 suppression in Pb\u00e2\u0080\u0093Pb collisions at sNN=2.76\u00c2 TeV"
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      "source": "Elsevier", 
      "value": "The inclusive J/\u00cf\u0088 nuclear modification factor ( RAA ) in Pb\u00e2\u0080\u0093Pb collisions at sNN=2.76\u00c2 TeV has been measured by ALICE as a function of centrality in the e+e\u00e2\u0088\u0092 decay channel at mid-rapidity ( |y|&lt;0.8 ) and as a function of centrality, transverse momentum and rapidity in the \u00ce\u00bc+\u00ce\u00bc\u00e2\u0088\u0092 decay channel at forward-rapidity ( 2.5&lt;y&lt;4 ). The J/\u00cf\u0088 yields measured in Pb\u00e2\u0080\u0093Pb are suppressed compared to those in pp collisions scaled by the number of binary collisions. The RAA integrated over a centrality range corresponding to 90% of the inelastic Pb\u00e2\u0080\u0093Pb cross section is 0.72\u00c2\u00b10.06(stat.)\u00c2\u00b10.10(syst.) at mid-rapidity and 0.58\u00c2\u00b10.01(stat.)\u00c2\u00b10.09(syst.) at forward-rapidity. At low transverse momentum, significantly larger values of RAA are measured at forward-rapidity compared to measurements at lower energy. These features suggest that a contribution to the J/\u00cf\u0088 yield originates from charm quark (re)combination in the deconfined partonic medium."
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Published on:
27 May 2014
Publisher:
Elsevier
Published in:
Physics Letters B (2014)

Pages 314-327
DOI:
https://doi.org/10.1016/j.physletb.2014.05.064
Copyrights:
The Authors
Licence:
CC-BY-3.0

Fulltext files: