<?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/14202" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14202</identifier><datestamp>2026-10-18T20:28:59Z</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 new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton–proton collisions at s=13TeV</dc:title><dc:creator>Sirunyan, A.M.</dc:creator><dc:creator>Tumasyan, A.</dc:creator><dc:creator>Adam, W.</dc:creator><dc:creator>Ambrogi, F.</dc:creator><dc:creator>Asilar, E.</dc:creator><dc:creator>Bergauer, T.</dc:creator><dc:creator>Brandstetter, J.</dc:creator><dc:creator>Brondolin, E.</dc:creator><dc:creator>Dragicevic, M.</dc:creator><dc:creator>Erö, J.</dc:creator><dc:creator>Escalante Del Valle, A.</dc:creator><dc:creator>Flechl, M.</dc:creator><dc:creator>Friedl, M.</dc:creator><dc:creator>Frühwirth, R.</dc:creator><dc:creator>Ghete, V.M.</dc:creator><dc:creator>Grossmann, J.</dc:creator><dc:creator>Hrubec, J.</dc:creator><dc:creator>Jeitler, M.</dc:creator><dc:creator>König, A.</dc:creator><dc:creator>Krammer, N.</dc:creator><dc:creator>Krätschmer, I.</dc:creator><dc:creator>Liko, D.</dc:creator><dc:creator>Madlener, T.</dc:creator><dc:creator>Mikulec, I.</dc:creator><dc:creator>Pree, E.</dc:creator><dc:creator>Rad, N.</dc:creator><dc:creator>Rohringer, H.</dc:creator><dc:creator>Schieck, J.</dc:creator><dc:creator>Schöfbeck, R.</dc:creator><dc:creator>Spanring, M.</dc:creator><dc:creator>Spitzbart, D.</dc:creator><dc:creator>Taurok, A.</dc:creator><dc:creator>Waltenberger, W.</dc:creator><dc:creator>Wittmann, J.</dc:creator><dc:creator>Wulz, C.-E.</dc:creator><dc:creator>Zarucki, M.</dc:creator><dc:creator>Chekhovsky, V.</dc:creator><dc:creator>Mossolov, V.</dc:creator><dc:creator>Suarez Gonzalez, J.</dc:creator><dc:creator>De Wolf, E.A.</dc:creator><dc:creator>Di Croce, D.</dc:creator><dc:creator>Janssen, X.</dc:creator><dc:creator>Lauwers, J.</dc:creator><dc:creator>Van De Klundert, M.</dc:creator><dc:creator>Van Haevermaet, H.</dc:creator><dc:creator>Van Mechelen, P.</dc:creator><dc:creator>Van Remortel, N.</dc:creator><dc:creator>Abu Zeid, S.</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:creator>D'Hondt, J.</dc:creator><dc:subject>CMS</dc:subject><dc:subject>Compressed</dc:subject><dc:subject>Leptons</dc:subject><dc:subject>Missing energy</dc:subject><dc:subject>SUSY</dc:subject><dc:description>A search is presented for new physics in events with two low-momentum, oppositely charged leptons (electrons or muons) and missing transverse momentum in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data collected using the CMS detector at the LHC correspond to an integrated luminosity of 35.9fb−1. The observed event yields are consistent with the expectations from the standard model. The results are interpreted in terms of pair production of charginos and neutralinos (χ˜1 ± and χ˜2 0) with nearly degenerate masses, as expected in natural supersymmetry models with light higgsinos, as well as in terms of the pair production of top squarks (t˜), when the lightest neutralino and the top squark have similar masses. At 95% confidence level, wino-like χ˜1 ±/χ˜2 0 masses are excluded up to 230 GeV for a mass difference of 20 GeV relative to the lightest neutralino. In the higgsino-like model, masses are excluded up to 168 GeV for the same mass difference. For t˜ pair production, top squark masses up to 450 GeV are excluded for a mass difference of 40 GeV relative to the lightest neutralino. © 2018 The Author(s)</dc:description><dc:publisher>Elsevier B.V.</dc:publisher><dc:date>2018</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/14202</dc:identifier><dc:identifier>https://doi.org/10.1016/j.physletb.2018.05.062</dc:identifier><dc:identifier>0370-2693</dc:identifier><dc:language>en</dc:language><dc:relation>Physics Letters, Section B: Nuclear, Elementary Particle and 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/14202</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>