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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; Bondar, A; Branchini, P; Campajola, M; Cecchi, C; Cerasoli, J; Chang, M. -C; Cheon, B. G; Chilikin, K; Cho, H. -E; Dey, S; Doležal, Z; Jiménez, I. Domínguez; Fodor, A; Garcia-Hernandez, M; Garg, R; Gaudino, G; Gaz, A; Ghosh, D; Ghumaryan, H; Giakoustidis, G; Giri, A; Gradl, W; Guan, Y; Hara, T; Hedges, M. T; de la Cruz, I. Heredia; Higuchi, T; Ito, S; Jin, Y; Junkerkalefeld, H; Ketter, C; Kim, D. Y; Koga, T; Kuzmin, A; Kwon, Y. -J; Lai, Y. -T; Lewis, P. M; Li, C; Libby, J; Longo, S; Lyu, C; Maharana, S. P; Maiti, R; Martellini, C; Metzner, F; Miller, C; Mirra, M; Molina-Gonzalez, N; Mondal, S; Moneta, S; Mrvar, M; Mussa, R; Otani, F; Paladino, A; Peruzzi, I; Praz, C; Prell, S; Prencipe, E; Purwar, H; Reiter, S; Remnev, M; Rizzo, G; Roehrken, M; Sangal, A; Scavino, B; Senyo, K; Sevior, M. E; Sfienti, C; Sharma, C; Skorupa, J; Sokolov, A; Stottler, Z. S; Stroili, R; Sutcliffe, W; Svidras, H; Tanida, K; Tiwary, R; Tonelli, D; Torassa, E; Uematsu, Y; Urquijo, P; Varvell, K. E; Veronesi, M; Wach, B; Wang, E; Warburton, A; Yamada, S; Yang, S. B; Zhilich, V

    arXiv (Cornell University), 10/2023
    Journal Article

    Phys.Rev.D 108 (2023) 9, 092013 We determine the CKM matrix-element magnitude $|V_{cb}|$ using $\overline{B}^0\to D^{*+}\ell^-\bar\nu_\ell$ decays reconstructed in $189 \, \mathrm{fb}^{-1}$ of collision data collected by the Belle II experiment, located at the SuperKEKB $e^+e^-$ collider. Partial decay rates are reported as functions of the recoil parameter $w$ and three decay angles separately for electron and muon final states. We obtain $|V_{cb}|$ using the Boyd-Grinstein-Lebed and Caprini-Lellouch-Neubert parametrizations, and find $|V_{cb}|_\mathrm{BGL}=(40.57\pm 0.31 \pm 0.95\pm 0.58)\times 10^{-3}$ and $|V_{cb}|_\mathrm{CLN}=(40.13 \pm 0.27 \pm 0.93\pm 0.58 )\times 10^{-3}$ with the uncertainties denoting statistical components, systematic components, and components from the lattice QCD input, respectively. The branching fraction is measured to be ${\cal B}(\overline{B}^0\to D^{*+}\ell^-\bar\nu_\ell)=(4.922 \pm 0.023 \pm 0.220)\%$. The ratio of branching fractions for electron and muon final states is found to be $0.998 \pm 0.009 \pm 0.020$. In addition, we determine the forward-backward angular asymmetry and the $D^{*+}$ longitudinal polarization fractions. All results are compatible with lepton-flavor universality in the Standard Model.