<?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>2026-10-19T01:02:07Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11897" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11897</identifier><datestamp>2026-10-18T21:13:18Z</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>A search for decays of the Higgs boson to invisible particles in events with a top-antitop quark pair or a vector boson in proton-proton collisions at √s=13TeV</dc:title><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>Escalante Del Valle, A.</dc:creator><dc:creator>Hussain, P.S.</dc:creator><dc:creator>Jeitler, M.</dc:creator><dc:creator>Krammer, N.</dc:creator><dc:creator>Lechner, L.</dc:creator><dc:creator>Liko, D.</dc:creator><dc:creator>Mikulec, I.</dc:creator><dc:creator>Paulitsch, P.</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>Kello, T.</dc:creator><dc:creator>Rejeb Sfar, H.</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>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>Morton, A.</dc:creator><dc:creator>Müller, D.</dc:creator><dc:creator>Sahasransu, A.R.</dc:creator><dc:creator>Tavernier, S.</dc:creator><dc:creator>Van Doninck, W.</dc:creator><dc:creator>Van Putte, S.</dc:creator><dc:creator>Vannerom, D.</dc:creator><dc:creator>Clerbaux, B.</dc:creator><dc:creator>Dansana, S.</dc:creator><dc:creator>De Lentdecker, G.</dc:creator><dc:creator>Favart, L.</dc:creator><dc:creator>Hohov, D.</dc:creator><dc:creator>Jaramillo, J.</dc:creator><dc:creator>Lee, K.</dc:creator><dc:creator>Mahdavikhorrami, M.</dc:creator><dc:creator>Makarenko, I.</dc:creator><dc:creator>Malara, A.</dc:creator><dc:subject>Germanium alloys</dc:subject><dc:subject>Germanium compounds</dc:subject><dc:subject>Tellurium compounds</dc:subject><dc:subject>Branching fractions</dc:subject><dc:subject>Confidence levels</dc:subject><dc:subject>Final state</dc:subject><dc:subject>Hadronics</dc:subject><dc:subject>Higgs boson</dc:subject><dc:subject>Integrated luminosity</dc:subject><dc:subject>Limit sets</dc:subject><dc:subject>Proton proton collisions</dc:subject><dc:subject>Upper limits</dc:subject><dc:subject>Vector boson</dc:subject><dc:subject>Bosons</dc:subject><dc:description>A search for decays to invisible particles of Higgs bosons produced in association with a top-antitop quark pair or a vector boson, which both decay to a fully hadronic final state, has been performed using proton-proton collision data collected at s=13TeV by the CMS experiment at the LHC, corresponding to an integrated luminosity of 138 fb-1 . The 95% confidence level upper limit set on the branching fraction of the 125 GeV Higgs boson to invisible particles, B(H → inv) , is 0.54 (0.39 expected), assuming standard model production cross sections. The results of this analysis are combined with previous B(H → inv) searches carried out at s=7 , 8, and 13 TeV in complementary production modes. The combined upper limit at 95% confidence level on B(H → inv) is 0.15 (0.08 expected). © 2023, CERN for the benefit of the CMS Collaboration.</dc:description><dc:publisher>Springer Nature</dc:publisher><dc:date>2023</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/11897</dc:identifier><dc:identifier>https://doi.org/10.1140/epjc/s10052-023-11952-7</dc:identifier><dc:identifier>1434-6044</dc:identifier><dc:language>en</dc:language><dc:relation>European Physical Journal C</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/11897</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>