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{ "@context": "https://schema.org/", "@id": 108777, "@type": "ScholarlyArticle", "creator": [ { "@type": "Person", "affiliation": "CERN", "name": "CERN \u0130\u015fbirli\u011fi" } ], "datePublished": "2014-01-01", "description": "<p>The inclusive J/\u03c8 nuclear modification factor ( RAA ) in Pb\u2013Pb collisions at sNN=2.76\u00a0TeV has been measured by ALICE as a function of centrality in the e+e\u2212 decay channel at mid-rapidity ( |y|<0.8 ) and as a function of centrality, transverse momentum and rapidity in the \u03bc+\u03bc\u2212 decay channel at forward-rapidity ( 2.5<y<4 ). The J/\u03c8 yields measured in Pb\u2013Pb 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\u2013Pb cross section is 0.72\u00b10.06(stat.)\u00b10.10(syst.) at mid-rapidity and 0.58\u00b10.01(stat.)\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/\u03c8 yield originates from charm quark (re)combination in the deconfined partonic medium.</p>", "headline": "Centrality, rapidity and transverse momentum dependence of J/\u03c8 suppression in Pb\u2013Pb collisions at sNN=2.76\u00a0TeV", "identifier": 108777, "image": "https://aperta.ulakbim.gov.tr/static/img/logo/aperta_logo_with_icon.svg", "license": "http://www.opendefinition.org/licenses/cc-by", "name": "Centrality, rapidity and transverse momentum dependence of J/\u03c8 suppression in Pb\u2013Pb collisions at sNN=2.76\u00a0TeV", "url": "https://aperta.ulakbim.gov.tr/record/108777" }
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