<?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>2026-10-18T23:15:12Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11271" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11271</identifier><datestamp>2026-10-18T20:26:20Z</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 the polarizations of prompt and non-prompt J/Ψ and Ψ(2S) mesons produced in pp collisions at √s = 13TeV</dc:title><dc:creator>Hayrapetyan, A.</dc:creator><dc:creator>Tumasyan, A.</dc:creator><dc:creator>Adam, W.</dc:creator><dc:creator>Andrejkovic, J.W.</dc:creator><dc:creator>Bergauer, T.</dc:creator><dc:creator>Chatterjee, S.</dc:creator><dc:creator>Damanakis, K.</dc:creator><dc:creator>Dragicevic, M.</dc:creator><dc:creator>Hussain, P.S.</dc:creator><dc:creator>Jeitler, M.</dc:creator><dc:creator>Krammer, N.</dc:creator><dc:creator>Li, A.</dc:creator><dc:creator>Liko, D.</dc:creator><dc:creator>Mikulec, I.</dc:creator><dc:creator>Schieck, J.</dc:creator><dc:creator>Schöfbeck, R.</dc:creator><dc:creator>Schwarz, D.</dc:creator><dc:creator>Sonawane, M.</dc:creator><dc:creator>Templ, S.</dc:creator><dc:creator>Waltenberger, W.</dc:creator><dc:creator>Wulz, C.-E.</dc:creator><dc:creator>Darwish, M.R.</dc:creator><dc:creator>Janssen, T.</dc:creator><dc:creator>Van Laer, T.</dc:creator><dc:creator>Van Mechelen, P.</dc:creator><dc:creator>Breugelmans, N.</dc:creator><dc:creator>D’Hondt, J.</dc:creator><dc:creator>Dansana, S.</dc:creator><dc:creator>De Moor, A.</dc:creator><dc:creator>Delcourt, M.</dc:creator><dc:creator>Heyen, F.</dc:creator><dc:creator>Lowette, S.</dc:creator><dc:creator>Makarenko, I.</dc:creator><dc:creator>Müller, D.</dc:creator><dc:creator>Tavernier, S.</dc:creator><dc:creator>Tytgat, M.</dc:creator><dc:creator>Van Onsem, G.P.</dc:creator><dc:creator>Van Putte, S.</dc:creator><dc:creator>Vannerom, D.</dc:creator><dc:creator>Bilin, B.</dc:creator><dc:creator>Clerbaux, B.</dc:creator><dc:creator>Das, A.K.</dc:creator><dc:creator>De Lentdecker, G.</dc:creator><dc:creator>Evard, H.</dc:creator><dc:creator>Favart, L.</dc:creator><dc:creator>Gianneios, P.</dc:creator><dc:creator>Jaramillo, J.</dc:creator><dc:creator>Khalilzadeh, A.</dc:creator><dc:creator>Khan, F.A.</dc:creator><dc:creator>Lee, K.</dc:creator><dc:subject>CMS</dc:subject><dc:subject>Quarkonium polarization</dc:subject><dc:subject>Quarkonium production</dc:subject><dc:description>The polarizations of prompt and non-prompt [Formula presented] and ψ(2S) mesons are measured in proton-proton collisions at s=13 TeV, using data samples collected by the CMS experiment in 2017 and 2018, corresponding to a total integrated luminosity of 103.3fb−1. Based on the analysis of the dimuon decay angular distributions in the helicity frame, the polar anisotropy, λϑ, is measured as a function of the transverse momentum, pT, of the charmonium states, in the 25–120 and 20–100 GeV ranges for the [Formula presented] and ψ(2S), respectively. The non-prompt polarizations agree with predictions based on the hypothesis that, for pT≳25GeV, the non-prompt [Formula presented] and ψ(2S) are predominantly produced in two-body B meson decays. The prompt results clearly exclude strong transverse polarizations, even for pT exceeding 30 times the [Formula presented] mass, where λϑ tends to an asymptotic value around 0.3. Taken together with previous measurements, by CMS and LHCb at s=7 TeV, the prompt polarizations show a significant variation with pT, at low pT. © 2024 CERN for the benefit of the CMS Collaboration</dc:description><dc:publisher>Elsevier B.V.</dc:publisher><dc:date>2024</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/11271</dc:identifier><dc:identifier>https://doi.org/10.1016/j.physletb.2024.139044</dc:identifier><dc:identifier>0370-2693</dc:identifier><dc:language>en</dc:language><dc:relation>Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics</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/11271</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>