<?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>2026-10-19T01:56:53Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14416" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14416</identifier><datestamp>2026-10-18T20:29:12Z</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>Search for the X (5568) State Decaying into Bs0 π± in Proton-Proton Collisions at s =8 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>Suarez Gonzalez, J.</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 Haevermaet, H.</dc:creator><dc:creator>Van Mechelen, P.</dc:creator><dc:creator>Van Remortel, N.</dc:creator><dc:creator>Abu Zeid, S.</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:creator>D'Hondt, J.</dc:creator><dc:creator>De Bruyn, I.</dc:creator><dc:creator>De Clercq, J.</dc:creator><dc:subject>Mass spectrometry</dc:subject><dc:subject>Branching fractions</dc:subject><dc:subject>Decay chains</dc:subject><dc:subject>Exotic state</dc:subject><dc:subject>Integrated luminosity</dc:subject><dc:subject>Invariant mass distribution</dc:subject><dc:subject>Invariant-mass spectra</dc:subject><dc:subject>Production rates</dc:subject><dc:subject>Proton proton collisions</dc:subject><dc:subject>article</dc:subject><dc:subject>luminance</dc:subject><dc:subject>meson</dc:subject><dc:subject>High energy physics</dc:subject><dc:description>A search for resonancelike structures in the Bs0π± invariant mass spectrum is performed using proton-proton collision data collected by the CMS experiment at the LHC at s=8 TeV, corresponding to an integrated luminosity of 19.7 fb-1. The Bs0 mesons are reconstructed in the decay chain Bs0→J/ψφ, with J/ψ→μ+μ- and φ→K+K-. The Bs0π± invariant mass distribution shows no statistically significant peaks for different selection requirements on the reconstructed Bs0 and π± candidates. Upper limits are set on the relative production rates of the X(5568) and Bs0 states times the branching fraction of the decay X(5568)±→Bs0π±. In addition, upper limits are obtained as a function of the mass and the natural width of possible exotic states decaying into Bs0π±. © 2018 CERN.</dc:description><dc:publisher>American Physical Society</dc:publisher><dc:date>2018</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/14416</dc:identifier><dc:identifier>https://doi.org/10.1103/physrevlett.120.202005</dc:identifier><dc:identifier>0031-9007</dc:identifier><dc:language>en</dc:language><dc:relation>Physical Review Letters</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/14416</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>