<?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>2026-10-19T00:03:01Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14233" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14233</identifier><datestamp>2026-10-18T20:29:01Z</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>Measurement of prompt and nonprompt charmonium suppression in PbPb collisions at 5.02 TeV</dc:title><dc:creator>Sirunyan, A.M.</dc:creator><dc:creator>Tumasyan, A.</dc:creator><dc:creator>Adam, W.</dc:creator><dc:creator>Ambrogi, F.</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>Escalante Del Valle, A.</dc:creator><dc:creator>Flechl, M.</dc:creator><dc:creator>Friedl, M.</dc:creator><dc:creator>Frühwirth, R.</dc:creator><dc:creator>Ghete, V.M.</dc:creator><dc:creator>Grossmann, J.</dc:creator><dc:creator>Hrubec, J.</dc:creator><dc:creator>Jeitler, M.</dc:creator><dc:creator>König, A.</dc:creator><dc:creator>Krammer, N.</dc:creator><dc:creator>Krätschmer, I.</dc:creator><dc:creator>Liko, D.</dc:creator><dc:creator>Madlener, T.</dc:creator><dc:creator>Mikulec, I.</dc:creator><dc:creator>Pree, E.</dc:creator><dc:creator>Rad, N.</dc:creator><dc:creator>Rohringer, H.</dc:creator><dc:creator>Schieck, J.</dc:creator><dc:creator>Schöfbeck, R.</dc:creator><dc:creator>Spanring, M.</dc:creator><dc:creator>Spitzbart, D.</dc:creator><dc:creator>Waltenberger, W.</dc:creator><dc:creator>Wittmann, J.</dc:creator><dc:creator>Wulz, C.-E.</dc:creator><dc:creator>Zarucki, M.</dc:creator><dc:creator>Chekhovsky, V.</dc:creator><dc:creator>Mossolov, V.</dc:creator><dc:creator>Gonzalez, J. Suarez</dc:creator><dc:creator>De Wolf, E.A.</dc:creator><dc:creator>Di Croce, D.</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>Zeid, S. Abu</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:creator>D’hondt, J.</dc:creator><dc:creator>De Bruyn, I.</dc:creator><dc:subject>Bosons</dc:subject><dc:subject>Germanium alloys</dc:subject><dc:subject>Hadrons</dc:subject><dc:subject>Lead alloys</dc:subject><dc:subject>A-center</dc:subject><dc:subject>Center-of-mass energies</dc:subject><dc:subject>Centre-of-mass energies</dc:subject><dc:subject>Charmonium</dc:subject><dc:subject>Data sample</dc:subject><dc:subject>Integrated luminosity</dc:subject><dc:subject>Measurements of</dc:subject><dc:subject>Nuclear modification factors</dc:subject><dc:subject>Pb-Pb collisions</dc:subject><dc:subject>Transverse momenta</dc:subject><dc:subject>Binary alloys</dc:subject><dc:description>The nuclear modification factors of J / ψ and ψ(2S) mesons are measured in PbPb collisions at a centre-of-mass energy per nucleon pair of sNN=5.02TeV. The analysis is based on PbPb and p p data samples collected by CMS at the LHC in 2015, corresponding to integrated luminosities of 464μb-1 and 28pb-1, respectively. The measurements are performed in the dimuon rapidity range of | y| &lt; 2.4 as a function of centrality, rapidity, and transverse momentum (pT) from pT= 3 GeV/c in the most forward region and up to 50GeV/c. Both prompt and nonprompt (coming from b hadron decays) J / ψ mesons are observed to be increasingly suppressed with centrality, with a magnitude similar to the one observed at sNN=2.76TeV for the two J / ψ meson components. No dependence on rapidity is observed for either prompt or nonprompt J / ψ mesons. An indication of a lower prompt J / ψ meson suppression at pT&gt; 25 GeV/c is seen with respect to that observed at intermediate pT. The prompt ψ(2S) meson yield is found to be more suppressed than that of the prompt J / ψ mesons in the entire pT range. © 2018, CERN for the benefit of the CMS collaboration.</dc:description><dc:publisher>Springer Nature</dc:publisher><dc:date>2018</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/14233</dc:identifier><dc:identifier>https://doi.org/10.1140/epjc/s10052-018-5950-6</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/14233</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>