<?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>2026-10-18T23:47:37Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/13593" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/13593</identifier><datestamp>2026-10-18T20:28:25Z</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 jet mass distribution and top quark mass in hadronic decays of boosted top quarks in pp collisions at √s = 13 TeV</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>Bergauer, T.</dc:creator><dc:creator>Brandstetter, J.</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>Frühwirth, R.</dc:creator><dc:creator>Jeitler, M.</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>Rad, N.</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>Wulz, C.-E.</dc:creator><dc:creator>Zarucki, M.</dc:creator><dc:creator>Drugakov, V.</dc:creator><dc:creator>Mossolov, V.</dc:creator><dc:creator>Suarez Gonzalez, J.</dc:creator><dc:creator>Darwish, M.R.</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>Lelek, A.</dc:creator><dc:creator>Pieters, M.</dc:creator><dc:creator>Rejeb Sfar, H.</dc:creator><dc:creator>van Haevermaet, H.</dc:creator><dc:creator>van Mechelen, P.</dc:creator><dc:creator>van Putte, S.</dc:creator><dc:creator>van Remortel, N.</dc:creator><dc:creator>Blekman, F.</dc:creator><dc:creator>Bols, E.S.</dc:creator><dc:creator>Chhibra, S.S.</dc:creator><dc:creator>D'Hondt, J.</dc:creator><dc:creator>de Clercq, J.</dc:creator><dc:creator>Lontkovskyi, D.</dc:creator><dc:creator>Lowette, S.</dc:creator><dc:creator>Marchesini, I.</dc:creator><dc:creator>Moortgat, S.</dc:creator><dc:creator>Python, Q.</dc:creator><dc:creator>Skovpen, K.</dc:creator><dc:subject>CMS detectors</dc:subject><dc:subject>Hadronic decays</dc:subject><dc:subject>Hadronics</dc:subject><dc:subject>Integrated luminosity</dc:subject><dc:subject>Mass distribution</dc:subject><dc:subject>Measurements of</dc:subject><dc:subject>Quark mass</dc:subject><dc:subject>Single jet</dc:subject><dc:subject>Top quarks</dc:subject><dc:subject>Transverse momenta</dc:subject><dc:subject>article</dc:subject><dc:subject>lepton</dc:subject><dc:subject>luminance</dc:subject><dc:subject>quark</dc:subject><dc:description>A measurement is reported of the jet mass distribution in hadronic decays of boosted top quarks produced in pp collisions at √s = 13 TeV. The data were collected with the CMS detector at the LHC and correspond to an integrated luminosity of 35.9 fb−1. The measurement is performed in the lepton þ jets channel of tt events, where the lepton is an electron or muon. The products of the hadronic top quark decay t → bW → bqq¯0 are reconstructed as a single jet with transverse momentum larger than 400 GeV. The t¯t cross section as a function of the jet mass is unfolded at the particle level and used to extract a value of the top quark mass of 172.6 ± 2.5 GeV. A novel jet reconstruction technique is used for the first time at the LHC, which improves the precision by a factor of 3 relative to an earlier measurement. This highlights the potential of measurements using boosted top quarks, where the new technique will enable future precision measurements. © 2020 CERN, for the CMS Collaboration</dc:description><dc:publisher>American Physical Society</dc:publisher><dc:date>2020</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/13593</dc:identifier><dc:identifier>https://doi.org/10.1103/physrevlett.124.202001</dc:identifier><dc:identifier>0031-9007</dc:identifier><dc:language>en</dc:language><dc:relation>Physical Review Letters</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/13593</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>