<?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>2026-10-19T04:50:37Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/15902" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/15902</identifier><datestamp>2026-10-18T20:30:45Z</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>Observation of Z decays to four leptons with the CMS detector at the LHC</dc:title><dc:creator>Chatrchyan, S.</dc:creator><dc:creator>Khachatryan, V.</dc:creator><dc:creator>Sirunyan, A.M.</dc:creator><dc:creator>Tumasyan, A.</dc:creator><dc:creator>Adam, W.</dc:creator><dc:creator>Aguilo, E.</dc:creator><dc:creator>Bergauer, T.</dc:creator><dc:creator>Dragicevic, M.</dc:creator><dc:creator>Erö, J.</dc:creator><dc:creator>Fabjan, C.</dc:creator><dc:creator>Friedl, M.</dc:creator><dc:creator>Frühwirth, R.</dc:creator><dc:creator>Ghete, V.M.</dc:creator><dc:creator>Hammer, J.</dc:creator><dc:creator>Hörmann, N.</dc:creator><dc:creator>Hrubec, J.</dc:creator><dc:creator>Jeitler, M.</dc:creator><dc:creator>Kiesenhofer, W.</dc:creator><dc:creator>Knünz, V.</dc:creator><dc:creator>Krammer, M.</dc:creator><dc:creator>Liko, D.</dc:creator><dc:creator>Mikulec, I.</dc:creator><dc:creator>Pernicka, M.</dc:creator><dc:creator>Rahbaran, B.</dc:creator><dc:creator>Rohringer, C.</dc:creator><dc:creator>Rohringer, H.</dc:creator><dc:creator>Schöfbeck, R.</dc:creator><dc:creator>Strauss, J.</dc:creator><dc:creator>Taurok, A.</dc:creator><dc:creator>Wagner, P.</dc:creator><dc:creator>Waltenberger, W.</dc:creator><dc:creator>Walzel, G.</dc:creator><dc:creator>Widl, E.</dc:creator><dc:creator>Wulz, C.-E.</dc:creator><dc:creator>Mossolov, V.</dc:creator><dc:creator>Shumeiko, N.</dc:creator><dc:creator>Gonzalez, J. Suarez</dc:creator><dc:creator>Bansal, S.</dc:creator><dc:creator>Cornelis, T.</dc:creator><dc:creator>De Wolf, E.A.</dc:creator><dc:creator>Janssen, X.</dc:creator><dc:creator>Luyckx, S.</dc:creator><dc:creator>Mucibello, L.</dc:creator><dc:creator>Ochesanu, S.</dc:creator><dc:creator>Roland, B.</dc:creator><dc:creator>Rougny, R.</dc:creator><dc:creator>Selvaggi, M.</dc:creator><dc:creator>Staykova, Z.</dc:creator><dc:creator>Van Haevermaet, H.</dc:creator><dc:creator>Van Mechelen, P.</dc:creator><dc:subject>Hadron-Hadron Scattering</dc:subject><dc:description>The first observation of the Z boson decaying to four leptons in proton-proton collisions is presented. The analyzed data set corresponds to an integrated luminosity of 5.02 fb-1 at s=7 TeV collected by the CMS detector at the Large Hadron Collider. A pronounced resonance peak, with a statistical significance of 9.7 σ, is observed in the distribution of the invariant mass of four leptons (electrons and/or muons) with mass and width consistent with expectations for Z boson decays. The branching fraction and cross section reported here are defined by phase space restrictions on the leptons, namely, 80 &lt; m 4ℓ &lt; 100 GeV, where m 4ℓ is the invariant mass of the four leptons, and m ℓℓ &gt; 4 GeV for all pairs of leptons, where m ℓℓ is the two-lepton invariant mass. The measured branching fraction is B({Z → 4ℓ)=({4.2-0.8+0.9 (stat.)±0.2(syst.))×times 10-6 and agrees with the standard model prediction of 4.45 × 10-6. The measured cross section times branching fraction is σ (pp → Z)B(Z →4ℓ)=112-20+23(stat.)-5+7 (syst.)-2+3 (lumi.) fb, also consistent with the standard model prediction of 120 fb. The four-lepton mass peak arising from Z → 4ℓ decays provides a calibration channel for the Higgs boson search in the H → ZZ → 4ℓ decay mode.[Figure not available: see fulltext.] © 2012 CERN for the benefit of the CMS collaboration.</dc:description><dc:publisher>Springer Verlag</dc:publisher><dc:date>2012</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/15902</dc:identifier><dc:identifier>https://doi.org/10.1007/jhep12(2012)034</dc:identifier><dc:identifier>1126-6708</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/15902</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>