Nayak, L.Nishida, S.Giri, A.Adachi, I.Aihara, H.Asner, D. M.Atmacan, H.Aulchenko, V.Aushev, T.Ayad, R.Babu, V.Bahinipati, S.Banerjee, S.Bauer, M.Behera, P.Belous, K.Bennett, J.Bessner, M.Bhuyan, B.Biswas, D.Bodrov, D.Borah, J.Bozek, A.Bracko, M.Branchini, P.Browder, T. E.Budano, A.Campajola, M.Cervenkov, D.Chang, M. -C.Cheon, B. G.Chilikin, K.Cho, H. E.Cho, K.Choi, S. -K.Choi, Y.Choudhury, S.Cinabro, D.Cochran, J.Das, S.Dash, N.De Nardo, G.De Pietro, G.Dhamija, R.Di Capua, F.Dingfelder, J.Dolezal, Z.Dong, T. V.Dossett, D.Dubey, S.Epifanov, D.Ferber, T.Ferlewicz, D.Fulsom, B. G.Garg, R.Gaur, V.Goldenzweig, P.Graziani, E.Gu, T.Guan, Y.Halder, S.Hara, T.Hayasaka, K.Hayashii, H.Hedges, M. T.Herrmann, D.Hou, W. -S.Hsu, C. -L.Iijima, T.Inami, K.Inguglia, G.Ipsita, N.Ishikawa, A.Itoh, R.Iwasaki, M.Jacobs, W. W.Jang, E. -J.Jia, S.Jin, Y.Joo, K. K.Kaliyar, A. B.Kawasaki, T.Kiesling, C.Kim, C. H.Kim, D. Y.Kim, K. -H.Kim, Y. -K.Kinoshita, K.Kodys, P.Konno, T.Korobov, A.Korpar, S.Kovalenko, E.Krizan, P.Krokovny, P.Kuhr, T.Kumar, M.Kumar, R.Kumara, K.Kuzmin, A.Kwon, Y. -J.Lee, S. C.Li, J.Li, L. K.Li, Y.Libby, J.Lieret, K.Lin, Y. -R.Liventsev, D.Luo, T.Ma, Y.Masuda, M.Matsuda, T.Maurya, S. K.Meier, F.Merola, M.Metzner, F.Miyabayashi, K.Mizuk, R.Mohanty, G. B.Nakamura, I.Nakao, M.Natkaniec, Z.Natochii, A.Nisar, N. K.Ogawa, S.Ono, H.Oskin, P.Pakhlov, P.Pakhlova, G.Pang, T.Pardi, S.Park, J.Park, S. -H.Passeri, A.Paul, S.Pedlar, T. K.Pestotnik, R.Piilonen, Leo E.Podobnik, T.Prencipe, E.Prim, M. T.Rostomyan, A.Rout, N.Russo, G.Sandilya, S.Sangal, A.Santelj, L.Savinov, V.Schnell, G.Schwanda, C.Schwartz, A. J.Seino, Y.Senyo, K.Sevior, M. E.Shapkin, M.Sharma, C.Shiu, J. -G.Sibidanov, A.Solovieva, E.Staric, M.Sumihama, M.Sumiyoshi, T.Takizawa, M.Tanida, K.Tenchini, F.Trabelsi, K.Uchida, M.Unno, Y.Uno, K.Uno, S.Urquijo, P.Vahsen, S. E.Varner, G.Varvell, K. E.Vinokurova, A.Wang, D.Wang, M. -Z.Watanuki, S.Won, E.Yabsley, B. D.Yan, W.Yelton, J.Yook, Y.Yuan, C. Z.Yuan, L.Yusa, Y.Zhai, Y.Zhang, Z. P.Zhilich, V.Zhukova, V.2023-12-082023-12-082023-08-282023-08-281029-8479https://hdl.handle.net/10919/117145<jats:title>A<jats:sc>bstract</jats:sc> </jats:title><jats:p>We present a search for the lepton-flavor-violating decays <jats:inline-formula><jats:alternatives><jats:tex-math>$$ {B}_s^0 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>s</mml:mi> <mml:mn>0</mml:mn> </mml:msubsup> </mml:math></jats:alternatives></jats:inline-formula> → <jats:italic>ℓ</jats:italic><jats:sup>∓</jats:sup><jats:italic>τ</jats:italic><jats:sup><jats:italic>±</jats:italic></jats:sup>, where <jats:italic>ℓ</jats:italic> = <jats:italic>e, μ</jats:italic>, using the full data sample of 121 fb<jats:sup><jats:italic>−</jats:italic>1</jats:sup> collected at the Υ(5<jats:italic>S</jats:italic>) resonance with the Belle detector at the KEKB asymmetric-energy <jats:italic>e</jats:italic><jats:sup>+</jats:sup><jats:italic>e</jats:italic><jats:sup><jats:italic>−</jats:italic></jats:sup> collider. We use <jats:inline-formula><jats:alternatives><jats:tex-math>$$ {B}_s^0{\overline{B}}_s^0 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>s</mml:mi> <mml:mn>0</mml:mn> </mml:msubsup> <mml:msubsup> <mml:mover> <mml:mi>B</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>s</mml:mi> <mml:mn>0</mml:mn> </mml:msubsup> </mml:math></jats:alternatives></jats:inline-formula> events in which one <jats:inline-formula><jats:alternatives><jats:tex-math>$$ {B}_s^0 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>s</mml:mi> <mml:mn>0</mml:mn> </mml:msubsup> </mml:math></jats:alternatives></jats:inline-formula> meson is reconstructed in a semileptonic decay mode and the other in the signal mode. We find no evidence for <jats:inline-formula><jats:alternatives><jats:tex-math>$$ {B}_s^0 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>s</mml:mi> <mml:mn>0</mml:mn> </mml:msubsup> </mml:math></jats:alternatives></jats:inline-formula><jats:italic>→ ℓ</jats:italic><jats:sup>∓</jats:sup><jats:italic>τ</jats:italic><jats:sup><jats:italic>±</jats:italic></jats:sup> decays and set upper limits on their branching fractions at 90% confidence level as <jats:inline-formula><jats:alternatives><jats:tex-math>$$ \mathcal{B} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>B</mml:mi> </mml:math></jats:alternatives></jats:inline-formula>(<jats:inline-formula><jats:alternatives><jats:tex-math>$$ {B}_s^0 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>s</mml:mi> <mml:mn>0</mml:mn> </mml:msubsup> </mml:math></jats:alternatives></jats:inline-formula><jats:italic>→ e</jats:italic><jats:sup>∓</jats:sup><jats:italic>τ</jats:italic><jats:sup><jats:italic>±</jats:italic></jats:sup>) <jats:italic><</jats:italic> 14 <jats:italic>×</jats:italic> 10<jats:sup><jats:italic>−</jats:italic>4</jats:sup> and <jats:inline-formula><jats:alternatives><jats:tex-math>$$ \mathcal{B} $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>B</mml:mi> </mml:math></jats:alternatives></jats:inline-formula>(<jats:inline-formula><jats:alternatives><jats:tex-math>$$ {B}_s^0 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>s</mml:mi> <mml:mn>0</mml:mn> </mml:msubsup> </mml:math></jats:alternatives></jats:inline-formula><jats:italic>→ μ</jats:italic><jats:sup>∓</jats:sup><jats:italic>τ</jats:italic><jats:sup><jats:italic>±</jats:italic></jats:sup>) <jats:italic><</jats:italic> 7<jats:italic>.</jats:italic>3 <jats:italic>×</jats:italic> 10<jats:sup><jats:italic>−</jats:italic>4</jats:sup>. Our result represents the first upper limit on the <jats:inline-formula><jats:alternatives><jats:tex-math>$$ {B}_s^0 $$</jats:tex-math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>B</mml:mi> <mml:mi>s</mml:mi> <mml:mn>0</mml:mn> </mml:msubsup> </mml:math></jats:alternatives></jats:inline-formula><jats:italic>→ e</jats:italic><jats:sup>∓</jats:sup><jats:italic>τ</jats:italic><jats:sup><jats:italic>±</jats:italic></jats:sup> decay rate.</jats:p>13 page(s)enIn CopyrightScience & TechnologyPhysical SciencesPhysics, Particles & FieldsPhysicsB Physicse(+)-e(-) ExperimentsFlavour PhysicsIDENTIFICATION5106 Nuclear and Plasma Physics5107 Particle and High Energy Physics4902 Mathematical Physics49 Mathematical Sciences51 Physical SciencesSearch for B<sub>s</sub><SUP>0</SUP> → <i>l</i><SUP>∓</SUP>τ<SUP>±</SUP> with the semi-leptonic tagging method at BelleArticleJournal of High Energy Physicshttps://doi.org/10.1007/JHEP08(2023)17820238Piilonen, Leo [0000-0001-6836-0748]1029-8479