<?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>2026-10-18T23:16:39Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/12930" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/12930</identifier><datestamp>2026-10-18T20:27:47Z</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 supersymmetry in final states with two or three soft leptons and missing transverse momentum in proton-proton collisions at √s = 13 TeV</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>Dragicevic, M.</dc:creator><dc:creator>Escalante Del Valle, A.</dc:creator><dc:creator>Frühwirth, R.</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>Spanring, M.</dc:creator><dc:creator>Templ, S.</dc:creator><dc:creator>Waltenberger, W.</dc:creator><dc:creator>Wulz, C.-E.</dc:creator><dc:creator>Chekhovsky, V.</dc:creator><dc:creator>Litomin, A.</dc:creator><dc:creator>Makarenko, V.</dc:creator><dc:creator>Darwish, M.R.</dc:creator><dc:creator>De Wolf, E.A.</dc:creator><dc:creator>Janssen, T.</dc:creator><dc:creator>Kello, T.</dc:creator><dc:creator>Lelek, A.</dc:creator><dc:creator>Rejeb Sfar, H.</dc:creator><dc:creator>Van Mechelen, P.</dc:creator><dc:creator>Van Putte, S.</dc:creator><dc:creator>Van Remortel, N.</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:creator>Bols, E.S.</dc:creator><dc:creator>D’Hondt, J.</dc:creator><dc:creator>De Clercq, J.</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>Van Mulders, P.</dc:creator><dc:creator>Beghin, D.</dc:creator><dc:creator>Bilin, B.</dc:creator><dc:creator>Clerbaux, B.</dc:creator><dc:subject>Hadron-Hadron Scattering</dc:subject><dc:subject>Supersymmetry</dc:subject><dc:description>A search for supersymmetry in events with two or three low-momentum leptons and missing transverse momentum is performed. The search uses proton-proton collisions at s = 13 TeV collected in the three-year period 2016–2018 by the CMS experiment at the LHC and corresponding to an integrated luminosity of up to 137 fb−1. The data are found to be in agreement with expectations from standard model processes. The results are interpreted in terms of electroweakino and top squark pair production with a small mass difference between the produced supersymmetric particles and the lightest neutralino. For the electroweakino interpretation, two simplified models are used, a wino-bino model and a higgsino model. Exclusion limits at 95% confidence level are set on χ~20/χ~1± masses up to 275 GeV for a mass difference of 10 GeV in the wino-bino case, and up to 205(150) GeV for a mass difference of 7.5 (3) GeV in the higgsino case. The results for the higgsino are further interpreted using a phenomenological minimal supersymmetric standard model, excluding the higgsino mass parameter μ up to 180 GeV with the bino mass parameter M1 at 800 GeV. In the top squark interpretation, exclusion limits are set at top squark masses up to 540 GeV for four-body top squark decays and up to 480 GeV for chargino-mediated decays with a mass difference of 30 GeV. [Figure not available: see fulltext.]. © 2022, The Author(s).</dc:description><dc:publisher>Springer Science and Business Media Deutschland GmbH</dc:publisher><dc:date>2022</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/12930</dc:identifier><dc:identifier>https://doi.org/10.1007/jhep04(2022)091</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/12930</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>