A search for heavy Higgs bosons decaying into vector bosons in same-sign two-lepton final states in pp collisions at sqrt{s} = 13 TeV with the ATLAS detector

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Rafideen Bin Norisam ,P T Koenig ,V Vorobel ,M K Ayoub ,T Dias Do Vale ,Y Fu ,H Ma ,Marija Glišić ,N Rompotis ,S Kuday ,S Barsov ,P Yin ,M J White ,M Lokajı́ček ,E Guilloton ,M Tomoto ,Emily Filmer ,M Gignac ,O E Vickey Boeriu ,Risa Ushioda ,T Guillemin ,H Abreu ,S C Lee ,A M Wharton ,B Vormwald ,Linghua Guo ,E Lytken ,B Liberti ,W Ding ,Andrea Di Luca ,R Wang ,Q Shen ,D Kar ,X Yue ,C Grud ,À Zoccoli ,Věra Latoňová ,T Seiss ,J Roemer ,A Sanchez Pineda ,J Llorente Merino ,Laurynas Mince ,G Callea ,Z Doležal ,Gustavs Kehris ,S Asai ,B A Schumm ,M S Lutz ,A C Romero Hernandez ,H Zhu ,A Dimitrievska ,T Harenberg ,William Dale Heidorn ,M Moreno Llácer ,Giorgia Proto ,Esra Mohammed Shrif ,S Simion ,R Iguchi ,F Bartels ,Yanwen Hong ,B Zhou ,J Assahsah ,G Gagliardi ,Y Shimogama ,Z Yan ,G Alimonti ,Gregory James Ottino ,V Pleskot ,C M Hawkes ,E Lobodzinska ,V Solovyev ,Ricardo Barrué ,F Derue ,Lukas Ehrke ,J Jamieson ,H Lyons ,K W Janas ,P J Falke ,B Malaescu ,Z Marshall ,M Morii ,V D’amico ,R Müller ,S L Wu ,D P C Sankey ,S.‐C Hsu ,M Renda ,R Schwienhorst ,S Ali ,A Farbin ,H Wahlberg ,P Schacht ,T Bisanz ,S Kabana ,A Peyaud ,A Sanchez ,A Formica ,Iakov Aizenberg ,J W Cowley ,A Farilla ,C Troncon ,E M Baldin ,M Aoki ,Evan Michael Carlson ,R Narayan ,R Hankache ,F Crescioli ,M J Costa ,L Keszeghova ,X Ai ,B Hiti ,S Palestini ,E Kneringer ,G Navarro ,C M Robles Gajardo ,M Franklin ,D Scheirich ,D Boye ,L Carminati ,P Jenni ,Olivera Vujinovic ,R J Hawkings ,M J Kareem ,M Beretta ,P Gutiérrez ,Jad Mathieu Sardain ,J Kroll ,Viktor Ananiev ,J R Pater ,Maria Teresa Camerlingo ,V Gautam ,G Iacobucci ,Kai Chung Tam ,J Schovancová ,M Kiehn ,R Sikora ,G Jäkel ,K Černý ,S Hou ,S Morgenstern ,Ruth Pöttgen ,G N Hamity ,D Boscherini ,P Kluit ,M Demichev ,V Cavaliere ,A Khanov ,K Kawagoe ,K Peters ,K Axiotis ,C Kato,L Zwalinski

doi:10.1007/jhep07(2023)200

Abstract

A search for heavy Higgs bosons produced in association with a vector boson and decaying into a pair of vector bosons is performed in final states with two leptons (electrons or muons) of the same electric charge, missing transverse momentum and jets. A data sample of proton–proton collisions at a centre-of-mass energy of 13 TeV recorded with the ATLAS detector at the Large Hadron Collider between 2015 and 2018 is used. The data correspond to a total integrated luminosity of 139 fb−1. The observed data are in agreement with Standard Model background expectations. The results are interpreted using higher-dimensional operators in an effective field theory. Upper limits on the production cross-section are calculated at 95% confidence level as a function of the heavy Higgs boson’s mass and coupling strengths to vector bosons. Limits are set in the Higgs boson mass range from 300 to 1500 GeV, and depend on the assumed couplings. The highest excluded mass for a heavy Higgs boson with the coupling combinations explored is 900 GeV. Limits on coupling strengths are also provided.

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