<?xml version="1.0" encoding="UTF-8"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-10-19T04:51:57Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14727" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14727</identifier><datestamp>2026-10-18T20:29:32Z</datestamp><setSpec>openaire</setSpec><setSpec>driver</setSpec><setSpec>com_ebyu_10000</setSpec><setSpec>col_ebyu_10001</setSpec></header><metadata><oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:title>Suppression and azimuthal anisotropy of prompt and nonprompt J / ψ production in PbPb collisions at √sNN=2.76TeV</dc:title><dc:creator>Khachatryan, V.</dc:creator><dc:creator>Sirunyan, A.M.</dc:creator><dc:creator>Tumasyan, A.</dc:creator><dc:creator>Adam, W.</dc:creator><dc:creator>Asilar, E.</dc:creator><dc:creator>Bergauer, T.</dc:creator><dc:creator>Brandstetter, J.</dc:creator><dc:creator>Brondolin, E.</dc:creator><dc:creator>Dragicevic, M.</dc:creator><dc:creator>Erö, J.</dc:creator><dc:creator>Flechl, M.</dc:creator><dc:creator>Friedl, M.</dc:creator><dc:creator>Frühwirth, R.</dc:creator><dc:creator>Ghete, X.M.</dc:creator><dc:creator>Hartl, C.</dc:creator><dc:creator>Hörmann, N.</dc:creator><dc:creator>Hrubec, J.</dc:creator><dc:creator>Jeitler, M.</dc:creator><dc:creator>König, A.</dc:creator><dc:creator>Krätschmer, I.</dc:creator><dc:creator>Liko, D.</dc:creator><dc:creator>Matsushita, T.</dc:creator><dc:creator>Mikulec, I.</dc:creator><dc:creator>Rabady, D.</dc:creator><dc:creator>Rad, N.</dc:creator><dc:creator>Rahbaran, B.</dc:creator><dc:creator>Rohringer, H.</dc:creator><dc:creator>Schieck, J.</dc:creator><dc:creator>Strauss, J.</dc:creator><dc:creator>Waltenberger, W.</dc:creator><dc:creator>Wulz, C.-E.</dc:creator><dc:creator>Dvornikov, O.</dc:creator><dc:creator>Makarenko, V.</dc:creator><dc:creator>Zykunov, V.</dc:creator><dc:creator>Mossolov, V.</dc:creator><dc:creator>Shumeiko, N.</dc:creator><dc:creator>Gonzalez, J. Suarez</dc:creator><dc:creator>Alderweireldt, S.</dc:creator><dc:creator>De Wolf, E.A.</dc:creator><dc:creator>Janssen, X.</dc:creator><dc:creator>Lauwers, J.</dc:creator><dc:creator>Van De Klundert, M.</dc:creator><dc:creator>Van Haevermaet, H.</dc:creator><dc:creator>Van Mechelen, P.</dc:creator><dc:creator>Van Remortel, N.</dc:creator><dc:creator>Van Spilbeeck, A.</dc:creator><dc:creator>Abu Zeid, S.</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:creator>D’hondt, J.</dc:creator><dc:creator>Daci, N.</dc:creator><dc:subject>Anisotropy</dc:subject><dc:subject>Binary alloys</dc:subject><dc:subject>Hadrons</dc:subject><dc:subject>Kinematics</dc:subject><dc:subject>Anisotropy coefficients</dc:subject><dc:subject>Azimuthal anisotropy</dc:subject><dc:subject>Charm+</dc:subject><dc:subject>Kinematic range</dc:subject><dc:subject>Nuclear modification factors</dc:subject><dc:subject>Pb-Pb collisions</dc:subject><dc:subject>Strong dependences</dc:subject><dc:subject>Transverse momenta</dc:subject><dc:subject>Germanium alloys</dc:subject><dc:description>The nuclear modification factor RAA and the azimuthal anisotropy coefficient v2 of prompt and nonprompt (i.e. those from decays of b hadrons) J / ψ mesons, measured from PbPb and pp collisions at sNN=2.76TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta pT&gt; 6.5 GeV/c and rapidity | y| &lt; 2.4 , extending down to pT= 3 GeV/c in the 1.6 &lt; | y| &lt; 2.4 range. The v2 of prompt J / ψ is found to be nonzero, but with no strong dependence on centrality, rapidity, or pT over the full kinematic range studied. The measured v2 of nonprompt J / ψ is consistent with zero. The RAA of prompt J / ψ exhibits a suppression that increases from peripheral to central collisions but does not vary strongly as a function of either y or pT in the fiducial range. The nonprompt J / ψRAA shows a suppression which becomes stronger as rapidity or pT increases. The v2 and RAA of open and hidden charm, and of open charm and beauty, are compared. © 2017, CERN for the benefit of the CMS collaboration.</dc:description><dc:publisher>Springer Nature</dc:publisher><dc:date>2017</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/14727</dc:identifier><dc:identifier>https://doi.org/10.1140/epjc/s10052-017-4781-1</dc:identifier><dc:identifier>1434-6044</dc:identifier><dc:language>en</dc:language><dc:relation>European Physical Journal C</dc:relation><dc:rights>info:eu-repo/semantics/openAccess</dc:rights><dc:type>info:eu-repo/semantics/article</dc:type><dc:identifier>https://ebyu-rdlopen.rawdatalibrary.net/tr/items/ebyu/14727</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>