Hayrapetyan, Aram A.Tumasyan, A. R.Adam, WolfgangAndrejkovic, J. W.Bergauer, ThomasChatterjee, SumanJeitler, Manfred A.2025-02-102025-02-1020240370-2693https://doi.org/10.1016/j.physletb.2024.139044The 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, λ<inf>ϑ</inf>, is measured as a function of the transverse momentum, p<inf>T</inf>, 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 p<inf>T</inf>≳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 p<inf>T</inf> exceeding 30 times the [Formula presented] mass, where λ<inf>ϑ</inf> 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 p<inf>T</inf>, at low p<inf>T</inf>. © 2025 Elsevier B.V., All rights reserved.eninfo:eu-repo/semantics/openAccessCMSQuarkonium PolarizationQuarkonium ProductionArticle10.1016/j.physletb.2024.1390442-s2.0-85205550955