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  • Adachi, I; Aloisio, A; Asner, D. M; Aushev, V; Bahinipati, S; Bambade, P; Beaubien, A; Bennett, J. V; Bertacchi, V; Bianchi, F; Biswas, D; Budano, A; Campajola, M; Cao, L; Casarosa, G; Cheema, P; Chirapatpimol, K; De La Cruz-Burelo, E; De Nardo, G; De Nuccio, M; de Sangro, R; Destefanis, M; Dhamija, R; Di Capua, F; Dingfelder, J; Dubey, S; Ecker, P; Feichtinger, P; Garcia-Hernandez, M; Gaudino, G; Gaur, V; Gaz, A; Ghosh, D; Ghumaryan, H; Giakoustidis, G; Gradl, W; Grammatico, T; Gruberová, Z; Gu, T; Guan, Y; Han, Y; Hara, T; Higuchi, T; Hohmann, M; Ishikawa, A; Itoh, R; Iwasaki, M; Jang, E. -J; Jia, S; Kawasaki, T; Kiesling, C; Kim, C. -H; Kohani, S; Korpar, S; Kraetzschmar, T. M. G; Križan, P; Kumar, M; Lanceri, L; Diberder, F. R. Le; Liu, Z. Q; Ma, Y; Maggiora, M; Manfredi, R; Manoni, E; Mantovano, M; Marcantonio, D; Marinas, C; Martini, A; Martinov, T; Massaccesi, L; McKenna, J. A; Mehta, R; Merola, M; Molina-Gonzalez, N; Onishchuk, Y; Otani, F; Pardi, S; Pestotnik, R; Angioni, G. Pinna; Podobnik, T; Rauls, N; Roehrken, M; Savinov, V; Shimasaki, T; Shiu, J. -G; Singh, J. B; Sobie, R. J; Tittel, O; Urquijo, P; Varvell, K. E; Vismaya, V. S; Wach, B; Wallner, S; Warburton, A; Wessel, C; Xu, X. P; Yelton, J; Yoshihara, K; Zhang, B; Zhou, Q. D

    01/2024
    Journal Article

    We present an analysis of the process $e^{+}e^{-}\to\pi^{+}\pi^{-}\Upsilon(nS)$ (where $n$ = 1, 2, or 3) reconstructed in $19.6\rm$ $\rm fb^{-1}$ of Belle II data during a special run of the SuperKEKB collider at four energy points near the peak of the $\Upsilon(10753)$ resonance. By analyzing the mass distribution of the $\pi^+\pi^-\Upsilon(nS)$ system and the Born cross sections of the $e^{+}e^{-}\to\pi^{+}\pi^{-}\Upsilon(nS)$ process, we report the first observation of $\Upsilon(10753)$ decays to the $\pi^{+}\pi^{-}\Upsilon(1S)$ and $\pi^{+}\pi^{-}\Upsilon(2S)$ final states, and find no evidence for decays to $\pi^{+}\pi^{-}\Upsilon(3S)$. Possible intermediate states in the $\pi^+\pi^-\Upsilon(1S,2S)$ transitions are also investigated, and no evidence for decays proceeding via the $\pi^\mp Z_b^\pm$ or $f_0(980)\Upsilon(nS)$ intermediate states is found. We measure Born cross sections for the $e^{+}e^{-}\to\pi^{+}\pi^{-}\Upsilon(nS)$ process that, combined with results from Belle, improve the precision of measurements of the $\Upsilon(10753)$ mass and width by nearly a factor of two to $(10756.3\pm2.7\pm0.6)$ MeV/$c^2$ and $(29.7\pm8.5\pm1.1)$ MeV, respectively. The relative ratios of the Born cross sections at the $\Upsilon(10753)$ resonance peak are also reported for the first time.