<?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>2026-10-19T01:08:14Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14214" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/14214</identifier><datestamp>2026-10-18T20:29:00Z</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>Measurements of the p p → Z Z production cross section and the Z → 4 ℓ branching fraction, and constraints on anomalous triple gauge couplings 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>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>Rabady, D.</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>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, X.</dc:creator><dc:creator>Mossolov, V.</dc:creator><dc:creator>Gonzalez, J. Suarez</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>Zeid, S. Abu</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:creator>D’hondt, J.</dc:creator><dc:creator>De Bruyn, I.</dc:creator><dc:subject>Bosons</dc:subject><dc:subject>Forecasting</dc:subject><dc:subject>Tellurium compounds</dc:subject><dc:subject>Vanadium compounds</dc:subject><dc:subject>A-center</dc:subject><dc:subject>Branching fractions</dc:subject><dc:subject>Gauge couplings</dc:subject><dc:subject>Lepton pairs</dc:subject><dc:subject>Lepton productions</dc:subject><dc:subject>Measurements of</dc:subject><dc:subject>Model prediction</dc:subject><dc:subject>Production cross section</dc:subject><dc:subject>Proton proton collisions</dc:subject><dc:subject>Standard model</dc:subject><dc:subject>Couplings</dc:subject><dc:description>Four-lepton production in proton-proton collisions, p p → (Z / γ∗) (Z / γ∗) → 4 ℓ, where ℓ= e or μ, is studied at a center-of-mass energy of 13TeV with the CMS detector at the LHC. The data sample corresponds to an integrated luminosity of 35.9fb-1. The ZZ production cross section, σ(pp→ZZ)=17.2±0.5(stat)±0.7(syst)±0.4(theo)±0.4(lumi) pb, measured using events with two opposite-sign, same-flavor lepton pairs produced in the mass region 60&lt;mℓ+ℓ-&lt;120GeV, is consistent with standard model predictions. Differential cross sections are measured and are well described by the theoretical predictions. The Z boson branching fraction to four leptons is measured to be B(Z=4.8±0.2(stat)±0.2(syst)±0.1(theo)±0.1(lumi)×10-6 for events with a four-lepton invariant mass in the range 80&lt;m4ℓ&lt;100GeV and a dilepton mass m4GeV for all opposite-sign, same-flavor lepton pairs. The results agree with standard model predictions. The invariant mass distribution of the four-lepton system is used to set limits on anomalous ZZZ and ZZγ couplings at 95% confidence level: -0.0012&lt;f4Z&lt;0.0010, -0.0010&lt;f5Z&lt;0.0013, -0.0012&lt;f4γ&lt;0.0013, -0.0012&lt;f5γ&lt;0.0013. © 2018, CERN for the benefit of the CMS collaboration.</dc:description><dc:publisher>Springer Nature</dc:publisher><dc:date>2018</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/14214</dc:identifier><dc:identifier>https://doi.org/10.1140/epjc/s10052-018-5567-9</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/14214</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>