<?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>2026-10-19T01:18:11Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11745" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11745</identifier><datestamp>2026-10-18T20:26:44Z</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>Test of lepton flavor universality in B ± → K ± μ + μ − and B ± → K ± e + e − decays in proton-proton collisions at s = 13 TeV</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 Mechelen, P.</dc:creator><dc:creator>Bols, E.S.</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>Faham, H. El</dc:creator><dc:creator>Lowette, S.</dc:creator><dc:creator>Makarenko, I.</dc:creator><dc:creator>Müller, D.</dc:creator><dc:creator>Sahasransu, A.R.</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>Clerbaux, B.</dc:creator><dc:creator>Das, A.K.</dc:creator><dc:creator>De Lentdecker, G.</dc:creator><dc:creator>Favart, L.</dc:creator><dc:creator>Gianneios, P.</dc:creator><dc:creator>Hohov, D.</dc:creator><dc:creator>Jaramillo, J.</dc:creator><dc:creator>Khalilzadeh, A.</dc:creator><dc:creator>Lee, K.</dc:creator><dc:creator>Mahdavikhorrami, M.</dc:creator><dc:creator>Malara, A.</dc:creator><dc:subject>B meson</dc:subject><dc:subject>B physics</dc:subject><dc:subject>b to sll transitions</dc:subject><dc:subject>CMS</dc:subject><dc:subject>lepton flavor universality</dc:subject><dc:description>A test of lepton flavor universality in B ± → K ± μ + μ − and B ± → K ± e + e − decays, as well as a measurement of differential and integrated branching fractions of a nonresonant B ± → K ± μ + μ − decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at s = 13 TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions B ( B ± → K ± μ + μ − ) to B ( B ± → K ± e + e − ) is determined from the measured double ratio R ( K ) of these decays to the respective branching fractions of the B ± → J / ψ K ± with J / ψ → μ + μ − and e + e − decays, which allow for significant cancellation of systematic uncertainties. The ratio R ( K ) is measured in the range 1.1 &lt; q 2 &lt; 6.0 GeV 2 , where q is the invariant mass of the lepton pair, and is found to be R ( K ) = 0.78 − 0.23 + 0.47 , in agreement with the standard model expectation R ( K ) ≈ 1 . This measurement is limited by the statistical precision of the electron channel. The integrated branching fraction in the same q 2 range, B ( B ± → K ± μ + μ − ) = ( 12.42 ± 0.68 ) × 10 − 8 , is consistent with the present world-average value and has a comparable precision. © 2024 CERN, for the benefit of the CMS Collaboration.</dc:description><dc:publisher>Institute of Physics</dc:publisher><dc:date>2024</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/11745</dc:identifier><dc:identifier>https://doi.org/10.1088/1361-6633/ad4e65</dc:identifier><dc:identifier>0034-4885</dc:identifier><dc:language>en</dc:language><dc:relation>Reports on Progress in 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/11745</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>