<?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>2026-10-18T23:16:35Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/15191" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/15191</identifier><datestamp>2026-10-18T20:29:58Z</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 the production cross section ratio σ(χb2(1P))/σ(χb1(1P)) in pp collisions at s=8TeV</dc:title><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 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>Van Spilbeeck, A.</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:subject>Bottomonium</dc:subject><dc:subject>CMS</dc:subject><dc:subject>P-wave states</dc:subject><dc:subject>Quarkonium production</dc:subject><dc:description>A measurement of the production cross section ratio σ(χb2(1P))/σ(χb1(1P)) is presented. The χb1(1P) and χb2(1P) bottomonium states, promptly produced in pp collisions at s=8TeV, are detected by the CMS experiment at the CERN LHC through their radiative decays χb1,2(1P)→ϒ(1S)+γ. The emitted photons are measured through their conversion to e+e- pairs, whose reconstruction allows the two states to be resolved. The ϒ(1S) is measured through its decay to two muons. An event sample corresponding to an integrated luminosity of 20.7fb-1 is used to measure the cross section ratio in a phase-space region defined by the photon pseudorapidity, |ηγ|&lt;1.0; the ϒ(1S) rapidity, |yϒ|&lt;1.5; and the ϒ(1S) transverse momentum, 7&lt;pTϒ&lt;40GeV. The cross section ratio shows no significant dependence on the ϒ(1S) transverse momentum, with a measured average value of 0.85±0.07(stat+syst)±0.08(BF), where the first uncertainty is the combination of the experimental statistical and systematic uncertainties and the second is from the uncertainty in the ratio of the χb branching fractions. © 2015 CERN for the benefit of the CMS Collaboration.</dc:description><dc:publisher>Elsevier B.V.</dc:publisher><dc:date>2015</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/15191</dc:identifier><dc:identifier>https://doi.org/10.1016/j.physletb.2015.02.048</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/15191</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>