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  • Belle, The; Collaborations, Belle II; Ayad, R; Bae, H; Bambade, P; Becherer, F; Becker, J; Behera, P. K; Belous, K; Bertholet, E; Bessner, M; Bettarini, S; Bilka, T; Borah, J; Bračko, M; Briere, R. A; Chang, P; Choudhury, S; Cremaldi, L. M; Czank, T; De La Cruz-Burelo, E; De Nardo, G; De Nuccio, M; de Sangro, R; Destefanis, M; Dong, T. V; Dorigo, M; Dreyer, S; Dujany, G; Eliachevitch, M; Finck, C; Frey, A; Fulsom, B. G; Ganiev, E; Gellrich, A; Ghevondyan, G; Giordano, R; Graziani, E; Hou, W. -S; Hsu, C. -L; Iijima, T; Jacobs, W. W; Jia, S; Kang, K. H; Karyan, G; Kindo, H; Korobov, A; Kovalenko, E; Kumar, R; Lacaprara, S; Li, Y; Liu, Q. Y; Ma, Y; Maggiora, M; Manfredi, R; Manoni, E; Mantovano, M; Marinas, C; Martini, A; Martinov, T; Massaccesi, L; Matsuda, T; Maurya, S. K; McKenna, J. A; Mehta, R; Merola, M; Milesi, M; Miyabayashi, K; Nishida, S; Oskin, P; Praz, C; Prell, S; Prencipe, E; Purwar, H; Reif, M; Ripp-Baudot, I; Rizzo, G; Roehrken, M; Sangal, A; Scavino, B; Senyo, K; Shan, W; Sharma, C; Shillington, T; Sobie, R. J; Sobotzik, M; Sokolov, A; Spruck, B; Svidras, H; Takahashi, M; Tonelli, D; Tsaklidis, I; Ueda, I; Varner, G. S; Varvell, K. E; Vitale, L; Wang, D; Warburton, A; Yin, J. H; Zhilich, V

    arXiv (Cornell University), 08/2023
    Journal Article

    We report results from a study of $B^\pm \rightarrow DK^\pm$ decays followed by $D$ decaying to $CP$~eigenstates, where $D$ indicates a $D^0$ or $\bar{D}^{0}$ meson. These decays are sensitive to the Cabibbo-Kobayashi-Maskawa unitarity-triangle angle $\phi_{3}$. The results are based on a combined analysis of the final data set of $772 \times 10^6~B\bar{B}$ pairs collected by the Belle experiment and a data set of $198 \times 10^6~B\bar{B}$ pairs collected by the Belle~II experiment, both in electron-positron collisions at the $\Upsilon(4S)$ resonance. We measure the $CP$ asymmetries to be $\mathcal{ A}_{CP +} =~(+12.5 \pm 5.8 \pm 1.4)\% $ and $\mathcal{ A}_{CP -} =~(-16.7 \pm 5.7 \pm 0.6)\%$, and the ratios of branching fractions to be $\mathcal{ R}_{CP+}=~1.164 \pm 0.081 \pm 0.036 $ and $\mathcal{ R}_{CP-} =~1.151 \pm 0.074 \pm 0.019$. The first contribution to the uncertainties is statistical, and the second is systematic. The asymmetries $\mathcal{A}_{CP +}$ and $\mathcal{A}_{CP -}$ have similar magnitudes and opposite signs; their difference corresponds to 3.5~standard deviations. From these values we calculate 68.3\% confidence intervals of ($8.5^{\circ}<\phi_{3}<16.5^{\circ}$) or ($84.5^{\circ}<\phi_{3}<95.5^{\circ}$) or ($163.3^{\circ}<\phi_{3}<171.5^{\circ}$) and $0.321<r_{B}<0.465$.