<?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>2026-10-19T01:03:50Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/12165" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/12165</identifier><datestamp>2026-10-18T20:27:06Z</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 Higgs Boson and Observation of Z Boson through Their Decay into a Charm Quark-Antiquark Pair in Boosted Topologies in Proton-Proton Collisions at Formula Presented</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>Del Valle, A. Escalante</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>Sfar, H. Rejeb</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>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:creator>Paredes, S.</dc:creator><dc:subject>Deep neural networks</dc:subject><dc:subject>Germanium compounds</dc:subject><dc:subject>Tellurium compounds</dc:subject><dc:subject>Antiquarks</dc:subject><dc:subject>Charm quarks</dc:subject><dc:subject>Higgs boson</dc:subject><dc:subject>Integrated luminosity</dc:subject><dc:subject>Proton proton collisions</dc:subject><dc:subject>Quark antiquark pair</dc:subject><dc:subject>Standard-model Higgs bosons</dc:subject><dc:subject>The standard model</dc:subject><dc:subject>Transverse momenta</dc:subject><dc:subject>Z Bosons</dc:subject><dc:subject>article</dc:subject><dc:subject>boson</dc:subject><dc:subject>expectation</dc:subject><dc:subject>prediction</dc:subject><dc:subject>quark</dc:subject><dc:subject>Bosons</dc:subject><dc:description>A search for the standard model (SM) Higgs boson ( H ) produced with transverse momentum ( p T ) greater than 450 GeV and decaying to a charm quark-antiquark ( c c ¯ ) pair is presented. The search is performed using proton-proton collision data collected at s = 13 TeV by the CMS experiment at the LHC, corresponding to an integrated luminosity of 138 fb - 1 . Boosted H → c c ¯ decay products are reconstructed as a single large-radius jet and identified using a deep neural network charm tagging technique. The method is validated by measuring the Z → c c ¯ decay process, which is observed in association with jets at high p T for the first time with a signal strength of 1.00 - 0.14 + 0.17 ( syst ) ± 0.08 ( theo ) ± 0.06 ( stat ) , defined as the ratio of the observed process rate to the SM expectation. The observed (expected) upper limit on σ ( H ) B ( H → c c ¯ ) is set at 47 (39) times the SM prediction at 95% confidence level. © 2023 CERN, for the CMS Collaboration.</dc:description><dc:publisher>American Physical Society</dc:publisher><dc:date>2023</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/12165</dc:identifier><dc:identifier>https://doi.org/10.1103/physrevlett.131.041801</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/12165</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>