Measurement of single top-quark production in the s-channel in proton–proton collisions at sqrt{s} = 13 TeV with the ATLAS detector

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Heilman ,C Vernieri ,S Tokár ,W Wagner ,Aoto Tanaka ,R Wölker ,S Francescato ,H C Cheng ,L B A H Hommels ,S Díez Cornell ,H Duran Yildiz ,M Ellert ,D R Shope ,S Xella ,A Dimitrievska ,S De Castro ,H Torres ,S Yu Smirnov ,Z Hubáček ,P Jenni ,M Khandoga ,Weitao Wang ,L Serkin ,A Warburton ,P R Newman ,M Guth ,A Haas ,K Pachal ,J C Vermeulen ,Zainab Soumaimi ,P O Deviveiros ,N Kimura ,S Asai ,A Træet ,Q Shen ,K A Johns ,Z M Schillaci ,M Stolarski ,M Weirich ,R Pedro ,G Ripellino ,T Geralis ,O A Ducu ,Soufiane Zerradi ,Judith Hofer ,S Camarda ,R Hankache ,I Ochoa ,D Schaefer ,P Balek ,A Nisati ,J Schovancová ,K Mochizuki ,S H Connell ,G D Hallewell ,A Kaczmarska ,S Berlendis ,Dominik Babal ,Vladislavs Plesanovs ,Aaron Joseph Kilgallon ,J Tang ,J Pearkes ,Sanae Ezzarqtouni ,S Schlenker ,J Kroll ,D South ,Y Rozen ,Miguel Angel Principe Martin ,P Kodyš ,Polina Moskvitina ,H P Beck ,B Cole ,Y A Kurochkin ,S Stonjek ,S Tapprogge ,Marta Czurylo ,M Moreno Llácer ,M Atkinson ,M Franklin ,L Jeanty 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doi:10.1007/jhep06(2023)191

Abstract

A measurement of single top-quark production in the s-channel is performed in proton–proton collisions at a centre-of-mass energy of 13 TeV with the ATLAS detector at the CERN Large Hadron Collider. The dataset corresponds to an integrated luminosity of 139 fb−1. The analysis is performed on events with an electron or muon, missing transverse momentum and exactly two b-tagged jets in the final state. A discriminant based on matrix element calculations is used to separate single-top-quark s-channel events from the main background contributions, which are top-quark pair production and W-boson production in association with jets. The observed (expected) signal significance over the background-only hypothesis is 3.3 (3.9) standard deviations, and the measured cross-section is sigma ={8.2}_{-2.9}^{+3.5} pb, consistent with the Standard Model prediction of {sigma}^{textrm{SM}}={10.32}_{-0.36}^{+0.40} pb.

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