<?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>2026-10-18T23:15:09Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11751" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11751</identifier><datestamp>2026-10-18T20:26:45Z</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 decay of the Higgs boson to a pair of light pseudoscalar bosons in the final state with four bottom quarks 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>Lowette, S.</dc:creator><dc:creator>Makarenko, I.</dc:creator><dc:creator>Müller, D.</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>Evard, H.</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>Khan, F.A.</dc:creator><dc:creator>Lee, K.</dc:creator><dc:creator>Mahdavikhorrami, M.</dc:creator><dc:creator>Malara, A.</dc:creator><dc:subject>Beyond Standard Model</dc:subject><dc:subject>Hadron-Hadron Scattering</dc:subject><dc:subject>Supersymmetry</dc:subject><dc:description>A search is presented for the decay of the 125 GeV Higgs boson (H) to a pair of new light pseudoscalar bosons (a), followed by the prompt decay of each a boson to a bottom quark-antiquark pair, H→aa→bb¯bb¯. The analysis is performed using a data sample of proton-proton collisions collected with the CMS detector at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb−1. To reduce the background from standard model processes, the search requires the Higgs boson to be produced in association with a leptonically decaying W or Z boson. The analysis probes the production of new light bosons in a 15 &lt; ma &lt; 60 GeV mass range. Assuming the standard model predictions for the Higgs boson production cross sections for pp → WH and ZH, model independent upper limits at 95% confidence level are derived for the branching fraction BH→aa→bb¯bb¯. The combined WH and ZH observed upper limit on the branching fraction ranges from 1.10 for ma = 20 GeV to 0.36 for ma = 60 GeV, complementing other measurements in the μμττ, ττττ and bbℓℓ (ℓ = μ, τ) channels. © The Author(s) 2024.</dc:description><dc:publisher>Springer Science and Business Media Deutschland GmbH</dc:publisher><dc:date>2024</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/11751</dc:identifier><dc:identifier>https://doi.org/10.1007/jhep06(2024)097</dc:identifier><dc:identifier>1029-8479</dc:identifier><dc:language>en</dc:language><dc:relation>Journal of 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/11751</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>