<?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>2026-10-19T00:27:43Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/15086" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/15086</identifier><datestamp>2026-10-18T20:29:52Z</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>Measurement of jet multiplicity distributions in (Formula presented.) production in pp collisions at (Formula presented.)</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>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>Hartl, C.</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>Krätschmer, I.</dc:creator><dc:creator>Liko, D.</dc:creator><dc:creator>Mikulec, I.</dc:creator><dc:creator>Rabady, D.</dc:creator><dc:creator>Rahbaran, B.</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>Treberer-Treberspurg, W.</dc:creator><dc:creator>Waltenberger, W.</dc:creator><dc:creator>Wulz, C.-E.</dc:creator><dc:creator>Mossolov, V.</dc:creator><dc:creator>Shumeiko, N.</dc:creator><dc:creator>Suarez Gonzalez, J.</dc:creator><dc:creator>Alderweireldt, S.</dc:creator><dc:creator>Bansal, M.</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>Knutsson, A.</dc:creator><dc:creator>Luyckx, S.</dc:creator><dc:creator>Ochesanu, S.</dc:creator><dc:creator>Roland, B.</dc:creator><dc:creator>Rougny, R.</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>Van Spilbeeck, A.</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:subject>Elementary particles</dc:subject><dc:subject>A-center</dc:subject><dc:subject>Antiquarks</dc:subject><dc:subject>Center-of-mass energies</dc:subject><dc:subject>Centre-of-mass energies</dc:subject><dc:subject>Dileptons</dc:subject><dc:subject>Measurements of</dc:subject><dc:subject>Multiplicity distributions</dc:subject><dc:subject>Production cross section</dc:subject><dc:subject>Proton proton collisions</dc:subject><dc:subject>Top quarks</dc:subject><dc:subject>Quantum theory</dc:subject><dc:description>The normalised differential top quark-antiquark production cross section is measured as a function of the jet multiplicity in proton-proton collisions at a centre-of-mass energy of 7(Formula presented.) at the LHC with the CMS detector. The measurement is performed in both the dilepton and lepton+jets decay channels using data corresponding to an integrated luminosity of 5.0(Formula presented.). Using a procedure to associate jets to decay products of the top quarks, the differential cross section of the (Formula presented.) production is determined as a function of the additional jet multiplicity in the lepton+jets channel. Furthermore, the fraction of events with no additional jets is measured in the dilepton channel, as a function of the threshold on the jet transverse momentum. The measurements are compared with predictions from perturbative quantum chromodynamics and no significant deviations are observed. © 2014, The Author(s).</dc:description><dc:publisher>Springer Nature</dc:publisher><dc:date>2014</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/15086</dc:identifier><dc:identifier>https://doi.org/10.1140/epjc/s10052-014-3014-0</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/15086</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>