<?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>2026-10-19T01:04:02Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/13294" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/13294</identifier><datestamp>2026-10-18T20:28:07Z</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 CKM matrix elements in single top quark t-channel production in proton-proton collisions at s=13 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>Bergauer, T.</dc:creator><dc:creator>Dragicevic, M.</dc:creator><dc:creator>Erö, J.</dc:creator><dc:creator>Del Valle, A. Escalante</dc:creator><dc:creator>Flechl, M.</dc:creator><dc:creator>Frühwirth, R.</dc:creator><dc:creator>Jeitler, M.</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>Rad, N.</dc:creator><dc:creator>Schieck, J.</dc:creator><dc:creator>Schöfbeck, R.</dc:creator><dc:creator>Spanring, M.</dc:creator><dc:creator>Waltenberger, W.</dc:creator><dc:creator>Wulz, C.-E.</dc:creator><dc:creator>Zarucki, M.</dc:creator><dc:creator>Drugakov, V.</dc:creator><dc:creator>Mossolov, V.</dc:creator><dc:creator>Gonzalez, J. Suarez</dc:creator><dc:creator>Darwish, M.R.</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>Kello, T.</dc:creator><dc:creator>Lelek, A.</dc:creator><dc:creator>Pieters, M.</dc:creator><dc:creator>Sfar, H. Rejeb</dc:creator><dc:creator>Van Haevermaet, H.</dc:creator><dc:creator>Van Mechelen, P.</dc:creator><dc:creator>Van Putte, S.</dc:creator><dc:creator>Van Remortel, N.</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:creator>Bols, E.S.</dc:creator><dc:creator>Chhibra, S.S.</dc:creator><dc:creator>D’Hondt, J.</dc:creator><dc:creator>De Clercq, J.</dc:creator><dc:creator>Lontkovskyi, D.</dc:creator><dc:creator>Lowette, S.</dc:creator><dc:creator>Marchesini, I.</dc:creator><dc:creator>Moortgat, S.</dc:creator><dc:creator>Python, Q.</dc:creator><dc:creator>Tavernier, S.</dc:creator><dc:creator>Van Doninck, W.</dc:creator><dc:subject>CKM matrix</dc:subject><dc:subject>CMS</dc:subject><dc:subject>Physics</dc:subject><dc:subject>Top quark</dc:subject><dc:description>The first direct, model-independent measurement is presented of the modulus of the Cabibbo–Kobayashi–Maskawa (CKM) matrix elements |η|Vtb, |η|Vtd, and |η|Vts, in final states enriched in single top quark t-channel events. The analysis uses proton-proton collision data from the LHC, collected during 2016 by the CMS experiment, at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 35.9 fb−1. Processes directly sensitive to these matrix elements are considered at both the production and decay vertices of the top quark. In the standard model hypothesis of CKM unitarity, a lower limit of |η|Vtb&gt;0.970 is measured at the 95% confidence level. Several theories beyond the standard model are considered, and by releasing all constraints among the involved parameters, the values |η|Vtb=0.988±0.024, and |η|Vtd                         2+|η|Vts                         2=0.06±0.06, where the uncertainties include both statistical and systematic components, are measured. © 2020 The Author</dc:description><dc:publisher>Elsevier B.V.</dc:publisher><dc:date>2020</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/13294</dc:identifier><dc:identifier>https://doi.org/10.1016/j.physletb.2020.135609</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/13294</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>