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We thank CERN for the very successful operation of the LHC and its injectors, as well as the support staff at CERN and at our institutions worldwide without whom ATLAS could not be operated efficiently. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN, the ATLAS Tier-1 facilities at TRIUMF/SFU (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (The Netherlands), PIC (Spain), RAL (U.K.) and BNL (U.S.A.), the Tier-2 facilities worldwide and large non-WLCG resource providers. Major contributors of computing resources are listed in ref. [96]. We gratefully acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; ANID, Chile; CAS, MOST and NSFC, China; Minciencias, Colombia; MEYS CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS and CEA-DRF/IRFU, France; SRNSFG, Georgia; BMBF, HGF and MPG, Germany; GSRI, Greece; RGC and Hong Kong SAR, China; ISF and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; NWO, The Netherlands; RCN, Norway; MNiSW, Poland; FCT, Portugal; MNE/IFA, Romania; MESTD, Serbia; MSSR, Slovakia; ARIS and MVZI, Slovenia; DSI/NRF, South Africa; MICIU/AEI, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; NSTC, Taipei; TENMAK, Turkiye; STFC/UKRI, United Kingdom; DOE and NSF, United States of America. Individual groups and members have received support from BCKDF, CANARIE, CRC and DRAC, Canada; CERN-CZ, FORTE and PRIMUS, Czech Republic; COST, ERC, ERDF, Horizon 2020, ICSC-NextGenerationEU and Marie Sklodowska-Curie Actions, European Union; Investissements d'Avenir Labex, Investissements d'Avenir Idex and ANR, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF, Greece; BSF-NSF and MINERVA, Israel; NCN and NAWA, Poland; La Caixa Banking Foundation, CERCA Programme Generalitat de Catalunya and PROMETEO and GenT Programmes Generalitat Valenciana, Spain; Goran Gustafssons Stiftelse, Sweden; The Royal Society and Leverhulme Trust, United Kingdom. In addition, individual members wish to acknowledge support from Armenia: Yerevan Physics Institute (FAPERJ); CERN: European Organization for Nuclear Research (CERN PJAS); Chile: Agencia Nacional de Investigacion y Desarrollo (FONDECYT 1230812, FONDECYT 1230987, FONDECYT 1240864); China: Chinese Ministry of Science and Technology (MOST-2023YFA1605700), National Natural Science Foundation of China (NSFC-12175119, NSFC 12275265, NSFC-12075060); Czech Republic: Czech Science Foundation (GACR - 24-11373S), Ministry of Education Youth and Sports (FORTE CZ.02.01.01/00/22_008/0004632), PRIMUS Research Programme (PRIMUS/21/SCI/017); EU: H2020 European Research Council (ERC - 101002463); European Union: European Research Council (ERC - 948254, ERC 101089007), Horizon 2020 Framework Programme (MUCCA - CHIST-ERA-19-XAI-00), European Union, Future Artificial Intelligence Research (FAIR-NextGenerationEU PE00000013), Italian Center for High Performance Computing, Big Data and Quantum Computing (ICSC, NextGenerationEU); France: Agence Nationale de la Recherche (ANR-20-CE31-0013, ANR-21-CE31-0013, ANR-21-CE31-0022, ANR-22-EDIR-0002), Investissements d'Avenir Labex (ANR-11-LABX-0012); Germany: Baden-Wurttemberg Stiftung (BW Stiftung-Postdoc Eliteprogramme), Deutsche Forschungsgemeinschaft (DFG - 469666862, DFG - CR 312/5-2); Italy: Istituto Nazionale di Fisica Nucleare (ICSC, NextGenerationEU), Ministero dell'Universita e della Ricerca (PRIN -20223N7F8K - PNRR M4.C2.1.1); Japan: Japan Society for the Promotion of Science (JSPS KAKENHI JP22H01227, JSPS KAKENHI JP22H04944, JSPS KAKENHI JP22KK0227, JSPS KAKENHI JP23KK0245); The Netherlands: Netherlands Organisation for Scientific Research (NWO Veni 2020 - VI.Veni.202.179); Norway: Research Council of Norway (RCN-314472); Poland: Ministry of Science and Higher Education (IDUB AGH, POB8, D4 no 9722), Polish National Agency for Academic Exchange (PPN/PPO/2020/1/00002/U/00001), Polish National Science Centre (NCN 2021/42/E/ST2/00350, NCN OPUS nr 2022/47/B/ST2/03059, NCN UMO-2019/34/E/ST2/00393, UMO-2020/37/B/ST2/01043, UMO-2021/40/C/ST2/00187, UMO-2022/47/O/ST2/00148, UMO-2023/49/B/ST2/04085); Slovenia: Slovenian Research Agency (ARIS grant J1-3010); Spain: Generalitat Valenciana (Artemisa, FEDER, ID-IFEDER/2018/048), Ministry of Science and Innovation (MCIN & NextGenEU PCI2022135018-2, MICIN & FEDER PID2021-125273NB, RYC2019-028510-I, RYC2020-030254-I, RYC2021-031273-I, RYC2022-038164-I), PROMETEO and GenT Programmes Generalitat Valenciana (CIDEGENT/2019/027); Sweden: Swedish Research Council (Swedish Research Council 2023-04654, VR 2018-00482, VR 2022-03845, VR 2022-04683, VR 2023-03403, VR grant 2021-03651), Knut and Alice Wallenberg Foundation (KAW 2018.0157, KAW 2018.0458, KAW 2019.0447, KAW 2022.0358); Switzerland: Swiss National Science Foundation (SNSF - PCEFP2_194658); United Kingdom: Leverhulme Trust (Leverhulme Trust RPG-2020-004), Royal Society (NIF-R1-231091); United States of America: U.S. Department of Energy (ECA DE-AC02-76SF00515), Neubauer Family Foundation.

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Search for dark mesons decaying to top and bottom quarks in proton-proton collisions at √s=13 TeV with the ATLAS detector

Publicated to:Journal Of High Energy Physics. 2024 (9): 5- - 2024-09-02 2024(9), DOI: 10.1007/JHEP09(2024)005

Authors: Aad, G; Aakvaag, E; Abbott, B; Abdelhameed, S; Abeling, K; Abicht, N J; Abidi, S H; Aboelela, M; Aboulhorma, A; Abramowicz, H; Abreu, H; Abulaiti, Y; Acharya, B S; Ackermann, A; Bourdarios, C Adam; Adamczyk, L; Addepalli, S V; Addison, M J; Adelman, J; Adiguzel, A; Adye, T; Affolder, A A; Afik, Y; Agaras, M N; Agarwala, J; Aggarwal, A; Agheorghiesei, C; Ahmadov, F; Ahmed, W S; Ahuja, S; Ai, X; Aielli, G; Aikot, A; Tamlihat, M Ait; Aitbenchikh, B; Akbiyik, M; Akimov, A V; Akiyama, D; Akolkar, N N; Aktas, S; Al Khoury, K; Alberghi, G L; Albert, J; Albicocco, P; Albouy, G L; Alderweireldt, S; Alegria, Z L; Aleksa, M; Aleksandrov, I N; Alexa, C; Alexopoulos, T; Alfonsi, F; Algren, M; Alhroob, M; Ali, B; Ali, H M J; Ali, S; Alibocus, S W; Aliev, M; Alimonti, G; Alkakhi, W; Allaire, C; Allbrooke, B M M; Allen, J F; Allendes Flores, C A; Allport, P P; Aloisio, A; Alonso, F; Alpigiani, C; Alsolami, Z M K; Alvarez Estevez, M; Fernandez, A Alvarez; Cardoso, M Alves; Alviggi, M G; Aly, M; Amaral Coutinho, Y; Ambler, A; Amelung, C; Amerl, M; Ames, C G; Amidei, D; Amini, B; Amirie, K J; Amor Dos Santos, S P; Amos, K R; Amperiadou, D; An, S; Ananiev, V; Anastopoulos, C; Andeen, T; Anders, J K; Anderson, A C; Andrean, S Y; Andreazza, A; Angelidakis, S; Angerami, A; Anisenkov, A V; Annovi, A; Antel, C; Antipov, E; Antonelli, M; Anulli, F; Aoki, M; Aoki, T; Aparo, M A; Bella, L Aperio; Appelt, C; Apyan, A; Val, S J Arbiol; Arcangeletti, C; Arce, A T H; Arguin, J-F; Argyropoulos, S; Arling, J -H; Arnaez, O; Arnold, H; Artoni, G; Asada, H; Asai, K; Asai, S; Asbah, N A; Pickering, R A Ashby; Assamagan, K; Astalos, R; Astrand, K S V; Atashi, S; Atkin, R J; Atkinson, M; Atmani, H; Atmasiddha, P A; Augsten, K; Auricchio, S; Auriol, A D; Austrup, V A; Avolio, G; Axiotis, K; Azuelos, G; Babal, D; Bachacou, H; Bachas, K; Bachiu, A; Backman, F; Badea, A; Baer, T M; Bagnaia, P; Bahmani, M; Bahner, D; Bai, K; Baines, J T; Baines, L; Baker, O K; Bakos, E; Gupta, D Bakshi; Balabram Filho, L E; Balakrishnan, V; Balasubramanian, R; Baldin, E M; Balek, P; Ballabene, E; Balli, F; Baltes, L M; Balunas, W K; Balz, J; Bamwidhi, I; Banas, E; Bandieramonte, M; Bandyopadhyay, A; Bansal, S; Barak, L; Barakat, M; Barberio, E L; Barberis, D; Barbero, M; Barel, M Z; Barillari, T; Barisits, M-S; Barklow, T; Baron, P; Moreno, D A Baron; Baroncelli, A; Barr, A J; Barr, J D; Barreiro, F; da Costa, J Barreiro Guimaraes; Barron, U; Barros Teixeira, M G; Barsov, S; Bartels, F; Bartoldus, R; Barton, A E; Bartos, P; Basan, A; Baselga, M; Bassalat, A; Basso, M J; Bataju, S; Bate, R; Bates, R L; Batlamous, S; Batool, B; Battaglia, M; Battulga, D; Bauce, M; Bauer, M; Bauer, P; Bazzano Hurrell, L T; Beacham, J B; Beau, T; Beaucamp, J Y; Beauchemin, P H; Bechtle, P; Beck, H P; Becker, K; Beddall, A J; Bednyakov, V A; Bee, C P; Beemster, L J; Beermann, T A; Begalli, M; Begel, M; Behera, A; Behr, J K; Beirer, J F; Beisiegel, F; Belfkir, M; Bella, G; Bellagamba, L; Bellerive, A; Bellos, P; Beloborodov, K; 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Di Donato, C; Di Girolamo, A; Di Gregorio, G; Di Luca, A; Di Micco, B; Di Nardo, R; Di Petrillo, K F; Diamantopoulou, M; Dias, F A; Do Vale, T Dias; Diaz, M A; Capriles, F G Diaz; Didenko, A R; Didenko, M; Diehl, E B; Cornell, S Diez; Pardos, C Diez; Dimitriadi, C; Dimitrievska, A; Dingfelder, J; Dingley, T; Dinu, I-M; Dittmeier, S J; Dittus, F; Divisek, M; Dixit, B; Djama, F; Djobava, T; Doglioni, C; Dohnalova, A; Dolejsi, J; Dolezal, Z; Domijan, K; Dona, K M; Donadelli, M; Dong, B; Donini, J; D'Onofrio, A; D'Onofrio, M; Dopke, J; Doria, A; Dos Santos Fernandes, N; Dougan, P; Dova, M T; Doyle, A T; Draguet, M A; Dreyer, E; Drivas-koulouris, I; Drnevich, M; Drozdova, M; Du, D; du Pree, T A; Dubinin, F; Dubovsky, M; Duchovni, E; Duckeck, G; Ducu, O A; Duda, D; Dudarev, A; Duden, E R; D'uffizi, M; Duflot, L; Duhrssen, M; Duminica, I; Dumitriu, A E; Dunford, M; Dungs, S; Dunne, K; Duperrin, A; Yildiz, H Duran; Duren, M; Durglishvili, A; Dwyer, B L; Dyckes, G I; Dyndal, M; Dziedzic, B S; Earnshaw, Z O; 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Affiliations

Abstract

A search for dark mesons originating from strongly-coupled, SU(2) dark flavor symmetry conserving models and decaying gaugephobically to pure Standard Model final states containing top and bottom quarks is presented. The search targets fully hadronic final states and final states with exactly one electron or muon and multiple jets. The analyzed data sample corresponds to an integrated luminosity of 140 fb(-1) of proton-proton collisions collected at root s = 13TeV with the ATLAS detector at the Large Hadron Collider. No significant excess over the Standard Model background expectation is observed and the results are used to set the first direct constraints on this type of model. The two-dimensional signal space of dark pion masses m(pi D) and dark rho-meson masses m(rho D) is scanned. For m(pi D) /m(rho D) = 0.45, dark pions with masses m(pi D) < 940 GeV are excluded at the 95% CL, while for m(pi D) /m(rho D) = 0.25 masses m(pi D) < 740 GeV are excluded.

Keywords