<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><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>2026-04-03T19:25:37Z</responseDate><request verb="GetRecord" identifier="oai:www.recercat.cat:20.500.14342/6085" metadataPrefix="oai_dc">https://recercat.cat/oai/request</request><GetRecord><record><header><identifier>oai:recercat.cat:20.500.14342/6085</identifier><datestamp>2026-03-20T01:12:32Z</datestamp><setSpec>com_2072_482405</setSpec><setSpec>com_2072_183628</setSpec><setSpec>col_2072_482415</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" xmlns:doc="http://www.lyncode.com/xoai" 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 Bs0→ μ+μ−γ decay</dc:title>
   <dc:creator>Calvo Gomez, Miriam</dc:creator>
   <dc:creator>Golobardes Ribé, Elisabet</dc:creator>
   <dc:creator>Vilasis-Cardona, Xavier</dc:creator>
   <dc:creator>LHCb Collaboration - CERN</dc:creator>
   <dc:contributor>Universitat Ramon Llull. La Salle</dc:contributor>
   <dc:contributor>CERN</dc:contributor>
   <dc:subject>Decay processes</dc:subject>
   <dc:subject>Experimental nuclear physics</dc:subject>
   <dc:subject>Nuclear physics</dc:subject>
   <dc:subject>Particle physics</dc:subject>
   <dc:subject>Gran col·lisionador d'hadrons (França i Suïssa)</dc:subject>
   <dc:subject>530.1</dc:subject>
   <dc:subject>539</dc:subject>
   <dc:description>A search for the fully reconstructed Bs0→ μ+μ−γ decay is performed at the LHCb experiment using proton-proton collisions at s = 13 TeV corresponding to an integrated luminosity of 5.4 fb−1. No significant signal is found and upper limits on the branching fraction in intervals of the dimuon mass are set (Formula presented.) at 95% confidence level. Additionally, upper limits are set on the branching fraction in the [2mμ, 1.70] GeV/c2 dimuon mass region excluding the contribution from the intermediate ϕ(1020) meson, and in the region combining all dimuon-mass intervals.</dc:description>
   <dc:description>info:eu-repo/semantics/publishedVersion</dc:description>
   <dc:date>2020-07-11</dc:date>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:identifier>1029-8479</dc:identifier>
   <dc:identifier>https://hdl.handle.net/20.500.14342/6085</dc:identifier>
   <dc:identifier>https://doi.org/10.1007/JHEP07(2024)101</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Journal of High Energy Physics, 2024. 101</dc:relation>
   <dc:rights>© CERN</dc:rights>
   <dc:rights>Attribution 4.0 International</dc:rights>
   <dc:rights>http://creativecommons.org/licenses/by/4.0/</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>27 p.</dc:format>
   <dc:publisher>Springer</dc:publisher>
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