<?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>2026-10-19T00:27:23Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11246" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11246</identifier><datestamp>2026-10-18T21:13:13Z</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 pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton–proton collisions at √s=13TeV</dc:title><dc:creator>Druzhkin, D.</dc:creator><dc:creator>Borshch, V.</dc:creator><dc:creator>Babaev, A.</dc:creator><dc:creator>Uzunian, A.</dc:creator><dc:creator>Slabospitskii, S.</dc:creator><dc:creator>Konstantinov, D.</dc:creator><dc:creator>Kachanov, V.</dc:creator><dc:creator>Skovpen, Y.</dc:creator><dc:creator>Radchenko, O.</dc:creator><dc:creator>Kozyrev, A.</dc:creator><dc:creator>Dimova, T.</dc:creator><dc:creator>Blinov, V.</dc:creator><dc:creator>Vorotnikov, G.</dc:creator><dc:creator>Volkov, P.</dc:creator><dc:creator>Savrin, V.</dc:creator><dc:creator>Petrushanko, S.</dc:creator><dc:creator>Perfilov, M.</dc:creator><dc:creator>Obraztsov, S.</dc:creator><dc:creator>Kodolova, O.</dc:creator><dc:creator>Klyukhin, V.</dc:creator><dc:creator>Dudko, L.</dc:creator><dc:creator>Dubinin, M.</dc:creator><dc:creator>Bunichev, V.</dc:creator><dc:creator>Boos, E.</dc:creator><dc:creator>Terkulov, A.</dc:creator><dc:creator>Kirakosyan, M.</dc:creator><dc:creator>Azarkin, M.</dc:creator><dc:creator>Andreev, V.</dc:creator><dc:creator>Polikarpov, S.</dc:creator><dc:creator>Danilov, M.</dc:creator><dc:creator>Chistov, R.</dc:creator><dc:creator>Zhokin, A.</dc:creator><dc:creator>Popov, V.</dc:creator><dc:creator>Nikitenko, A.</dc:creator><dc:creator>Lychkovskaya, N.</dc:creator><dc:creator>Gavrilov, V.</dc:creator><dc:creator>Ivanov, K.</dc:creator><dc:creator>Aushev, T.</dc:creator><dc:creator>Toropin, A.</dc:creator><dc:creator>Tlisova, I.</dc:creator><dc:creator>Krasnikov, N.</dc:creator><dc:creator>Kirsanov, M.</dc:creator><dc:creator>Kirpichnikov, D.</dc:creator><dc:creator>Karneyeu, A.</dc:creator><dc:creator>Golubev, N.</dc:creator><dc:creator>Gninenko, S.</dc:creator><dc:creator>Dermenev, A.</dc:creator><dc:creator>Andreev, Yu.</dc:creator><dc:creator>Vorobyev, A.</dc:creator><dc:creator>Uvarov, L.</dc:creator><dc:subject>Astrophysics</dc:subject><dc:subject>Charged particles</dc:subject><dc:subject>Fighter aircraft</dc:subject><dc:subject>Germanium compounds</dc:subject><dc:subject>Particle detectors</dc:subject><dc:subject>Antiquarks</dc:subject><dc:subject>CMS detectors</dc:subject><dc:subject>Final state</dc:subject><dc:subject>Heavy particles</dc:subject><dc:subject>Pair production</dc:subject><dc:subject>Proton proton collisions</dc:subject><dc:subject>Spin 1/2</dc:subject><dc:subject>Top quarks</dc:subject><dc:subject>Transverse momenta</dc:subject><dc:subject>Upper limits</dc:subject><dc:subject>Tellurium compounds</dc:subject><dc:description>A search is presented for the pair production of new heavy resonances, each decaying into a top quark (t) or antiquark and a gluon (g). The analysis uses data recorded with the CMS detector from proton–proton collisions at a center-of-mass energy of 13TeV at the LHC, corresponding to an integrated luminosity of 138fb-1. Events with one muon or electron, multiple jets, and missing transverse momentum are selected. After using a deep neural network to enrich the data sample with signal-like events, distributions in the scalar sum of the transverse momenta of all reconstructed objects are analyzed in the search for a signal. No significant deviations from the standard model prediction are found. Upper limits at 95% confidence level are set on the product of cross section and branching fraction squared for the pair production of excited top quarks in the t∗→tg decay channel. The upper limits range from 120 to 0.8fb for a t∗with spin-1/2 and from 15 to 1.0fb for a t∗with spin-3/2. These correspond to mass exclusion limits up to 1050 and 1700GeV for spin-1/2 and spin-3/2 t∗particles, respectively. These are the most stringent limits to date on the existence of t∗→tg resonances. © CERN for the benefit of the CMS Collaboration 2025.</dc:description><dc:publisher>Springer Nature</dc:publisher><dc:date>2025</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/11246</dc:identifier><dc:identifier>https://doi.org/10.1140/epjc/s10052-024-13729-y</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/11246</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>