<?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>2026-10-18T23:16:11Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/12103" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/12103</identifier><datestamp>2026-10-18T20:27:03Z</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 Nonresonant Pair Production of Highly Energetic Higgs Bosons Decaying to Bottom Quarks</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>Pitters, F.M.</dc:creator><dc:creator>Schieck, J.</dc:creator><dc:creator>Schöfbeck, R.</dc:creator><dc:creator>Schwarz, D.</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>El Faham, H.</dc:creator><dc:creator>Lowette, S.</dc:creator><dc:creator>Moortgat, 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>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>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:creator>Pétré, L.</dc:creator><dc:subject>Bosons</dc:subject><dc:subject>Graph neural networks</dc:subject><dc:subject>Photons</dc:subject><dc:subject>Tellurium compounds</dc:subject><dc:subject>Bottom quarks</dc:subject><dc:subject>Final state</dc:subject><dc:subject>Higgs boson</dc:subject><dc:subject>Lorentz</dc:subject><dc:subject>Nonresonant</dc:subject><dc:subject>Pair production</dc:subject><dc:subject>Proton proton collisions</dc:subject><dc:subject>The standard model</dc:subject><dc:subject>Vector boson</dc:subject><dc:subject>article</dc:subject><dc:subject>boson</dc:subject><dc:subject>gluon</dc:subject><dc:subject>quark</dc:subject><dc:subject>Couplings</dc:subject><dc:description>A search for nonresonant Higgs boson ( H ) pair production via gluon and vector boson ( V ) fusion is performed in the four-bottom-quark final state, using proton-proton collision data at 13 TeV corresponding to 138 fb - 1 collected by the CMS experiment at the LHC. The analysis targets Lorentz-boosted H pairs identified using a graph neural network. It constrains the strengths relative to the standard model of the H self-coupling and the quartic V V H H couplings, κ 2 V , excluding κ 2 V = 0 for the first time, with a significance of 6.3 standard deviations when other H couplings are fixed to their standard model values. © 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/12103</dc:identifier><dc:identifier>https://doi.org/10.1103/physrevlett.131.041803</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/12103</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>