<?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>2026-10-19T01:09:14Z</responseDate><request verb="GetRecord" identifier="oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11411" metadataPrefix="oai_dc">https://ebyu-rdlopen.rawdatalibrary.net/oai/request</request><GetRecord><record><header><identifier>oai:ebyu-rdlopen.rawdatalibrary.net:ebyu/11411</identifier><datestamp>2026-10-18T21:13:14Z</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 multidifferential cross sections for dijet production in proton–proton collisions at s=13TeV</dc:title><dc:creator>Zhokin, A.</dc:creator><dc:creator>Zhizhin, I.</dc:creator><dc:creator>Zarubin, A.</dc:creator><dc:creator>Yuldashev, B.S.</dc:creator><dc:creator>Voytishin, N.</dc:creator><dc:creator>Vorobyev, A.</dc:creator><dc:creator>Uzunian, A.</dc:creator><dc:creator>Uvarov, L.</dc:creator><dc:creator>Toropin, A.</dc:creator><dc:creator>Tlisova, I.</dc:creator><dc:creator>Teryaev, O.</dc:creator><dc:creator>Terkulov, A.</dc:creator><dc:creator>Tcherniaev, E.</dc:creator><dc:creator>Sulimov, V.</dc:creator><dc:creator>Sosnov, D.</dc:creator><dc:creator>Snigirev, A.</dc:creator><dc:creator>Smirnov, V.</dc:creator><dc:creator>Slabospitskii, S.</dc:creator><dc:creator>Skovpen, Y.</dc:creator><dc:creator>Shulha, S.</dc:creator><dc:creator>Shmatov, S.</dc:creator><dc:creator>Shalaev, V.</dc:creator><dc:creator>Selivanova, D.</dc:creator><dc:creator>Savrin, V.</dc:creator><dc:creator>Savina, M.</dc:creator><dc:creator>Rusinov, V.</dc:creator><dc:creator>Radchenko, O.</dc:creator><dc:creator>Popov, V.</dc:creator><dc:creator>Polikarpov, S.</dc:creator><dc:creator>Petrushanko, S.</dc:creator><dc:creator>Perelygin, V.</dc:creator><dc:creator>Palichik, V.</dc:creator><dc:creator>Oskin, A.</dc:creator><dc:creator>Oreshkin, V.</dc:creator><dc:creator>Obraztsov, S.</dc:creator><dc:creator>Nikitenko, A.</dc:creator><dc:creator>Murzin, V.</dc:creator><dc:creator>Matveev, V.</dc:creator><dc:creator>Malakhov, A.</dc:creator><dc:creator>Makarenko, V.</dc:creator><dc:creator>Lychkovskaya, N.</dc:creator><dc:creator>Lukina, O.</dc:creator><dc:creator>Levchenko, P.</dc:creator><dc:creator>Lanev, A.</dc:creator><dc:creator>Krasnikov, N.</dc:creator><dc:creator>Kozyrev, A.</dc:creator><dc:creator>Korenkov, V.</dc:creator><dc:creator>Konstantinov, D.</dc:creator><dc:creator>Kodolova, O.</dc:creator><dc:creator>Klyukhin, V.</dc:creator><dc:subject>Bosons</dc:subject><dc:subject>Colliding beam accelerators</dc:subject><dc:subject>Detector effects</dc:subject><dc:subject>Dijet production</dc:subject><dc:subject>Distance parameter</dc:subject><dc:subject>Fixed-order</dc:subject><dc:subject>Integrated luminosity</dc:subject><dc:subject>Invariant mass</dc:subject><dc:subject>Measurements of</dc:subject><dc:subject>Production cross section</dc:subject><dc:subject>Proton proton collisions</dc:subject><dc:subject>Transverse momenta</dc:subject><dc:subject>Jets</dc:subject><dc:description>A measurement of the dijet production cross section is reported based on proton–proton collision data collected in 2016 at s=13TeV by the CMS experiment at the CERN LHC, corresponding to an integrated luminosity of up to 36.3fb-1. Jets are reconstructed with the anti-kT algorithm for distance parameters of R=0.4 and 0.8. Cross sections are measured double-differentially (2D) as a function of the largest absolute rapidity |y|max of the two jets with the highest transverse momenta pT and their invariant mass m1,2, and triple-differentially (3D) as a function of the rapidity separation y∗, the total boost yb, and either m1,2 or the average pT of the two jets. The cross sections are unfolded to correct for detector effects and are compared with fixed-order calculations derived at next-to-next-to-leading order in perturbative quantum chromodynamics. The impact of the measurements on the parton distribution functions and the strong coupling constant at the mass of the Z boson is investigated, yielding a value of αS(mZ)=0.1179±0.0019. © The Author(s) 2024.</dc:description><dc:publisher>Springer Nature</dc:publisher><dc:date>2025</dc:date><dc:type>Article</dc:type><dc:identifier>https://rdlopen.rawdatalibrary.net/r/ebyu/11411</dc:identifier><dc:identifier>https://doi.org/10.1140/epjc/s10052-024-13606-8</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/11411</dc:identifier></oai_dc:dc></metadata></record></GetRecord></OAI-PMH>