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L.Fallon, C.Ferbel, T.Galanti, M.Garcia-Bellido, A.Hindrichs, O.Khukhunaishvili, A.Ranken, E.Taus, R.Chiarito, B.Chou, J. P.Gandrakota, A.Gershtein, Y.Halkiadakis, E.Hart, A.Heindl, M.Hughes, E.Kaplan, S.Karacheban, O.Laflotte, I.Lath, A.Montalvo, R.Nash, K.Osherson, M.Salur, S.Schnetzer, S.Somalwar, S.Stone, R.Thayil, S. A.Thomas, S.Acharya, H.Delannoy, A. G.Spanier, S.Bouhali, O.Dalchenko, M.Delgado, A.Eusebi, R.Gilmore, J.Huang, T.Kamon, T.Luo, S.Malhotra, S.Mueller, R.Overton, D.Perniè, L.Rathjens, D.Safonov, A.Akchurin, N.Damgov, J.Hegde, V.Kunori, S.Lamichhane, K.Mengke, T.Muthumuni, S.Peltola, T.Undleeb, S.Volobouev, I.Whitbeck, A.Appelt, E.Greene, S.Gurrola, A.Janjam, R.Johns, W.Maguire, C.Melo, A.Ni, H.Padeken, K.Romeo, F.Sheldon, P.Tuo, S.Velkovska, J.Arenton, M. W.Cox, B.Cummings, G.Hakala, J.Hirosky, R.Joyce, M.Ledovskoy, A.Li, A.Neu, C.Tannenwald, B.Wolfe, E.Xia, F.Karchin, P. E.Poudyal, N.Thapa, P.Black, K.Bose, T.Buchanan, J.Caillol, C.Dasu, S.De Bruyn, I.Everaerts, P.Galloni, C.He, H.Herndon, M.Hervé, A.Hussain, U.Lanaro, A.Loeliger, A.Loveless, R.Madhusudanan Sreekala, J.Mallampalli, A.Pinna, D.Savin, A.Shang, V.Smith, W. H.Teague, D.Trembath-reichert, S.Vetens, W.2022-05-012022-05-012021-08-10Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics, v. 819.0370-2693http://hdl.handle.net/11449/233313A search is performed for the rare decay W±→π±γ in proton-proton collisions at s=13TeV. Data corresponding to an integrated luminosity of 137fb−1 were collected during 2016 to 2018 with the CMS detector. This analysis exploits a novel search strategy based on W boson production in top quark pair events. An inclusive search for the W±→π±γ decay is not optimal at the LHC because of the high trigger thresholds. Instead, a trigger selection is exploited in which the W boson originating from one of the top quarks is used to tag the event in a leptonic decay. The W boson emerging from the other top quark is used to search for the W±→π±γ signature. Such decays are characterized by an isolated track pointing to a large energy deposit, and by an isolated photon of large transverse momentum. The presence of b quark jets reduces the background from the hadronization of light-flavor quarks and gluons. The W±→π±γ decay is not observed. An upper exclusion limit is set to this branching fraction, corresponding to 1.50×10−5 at 95% confidence level, whereas the expected upper exclusion limit is 0.85−0.29+0.52×10−5.engCMSEWKStandard modelArtigo10.1016/j.physletb.2021.1364092-s2.0-85111246735