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The Belle and Belle II collaboration; I. Adachi; N. Akopov; A. Aloisio; H. Atmacan; M. Aversano; S. Bahinipati; M. Barrett; J. Baudot; A. Baur; M. Bertemes; E. Bertholet; A. Bobrov; A. Bolz; J. Borah; A. Bozek; T. E. Browder; S. Bussino; F. Dattola; G. De Nardo; R. de Sangro; A. Di Canto; Z. Doležal; K. Dort; S. Dreyer; T. Ferber; T. Fillinger; G. Finocchiaro; R. Garg; D. Ghosh; G. Giakoustidis; O. Gogota; E. Graziani; D. Greenwald; T. Gu; S. Halder; C. Hearty; M. T. Hedges; M. Hohmann; P. Horak; K. Inami; E.-J. Jang; A. Johnson; A. B. Kaliyar; J. Kandra; K. H. Kang; F. Keil; D. Y. Kim; K. Kinoshita; P. Kodyš; A. Korobov; R. Kowalewski; Y.-J. Kwon; Y.-T. Lai; T. Lam; L. Lanceri; J. S. Lange; D. Levit; J. Li; M. Maggiora; R. Maiti; C. Marinas; C. Martellini; J. A. McKenna; I. Nakamura; Z. Natkaniec; L. Nayak; S. Ogawa; I. Peruzzi; F. Pham; M. Piccolo; L. E. Piilonen; P. L. M. Podesta-Lerma; E. Prencipe; N. Rad; M. Remnev; I. Ripp-Baudot; A. Rostomyan; D. Sahoo; A. Sangal; V. Savinov; M. E. Sevior; J.-G. Shiu; J. Skorupa; M. Sobotzik; E. Solovieva; Z. S. Stottler; M. Sumihama; F. Tenchini; Y. Uematsu; Y. Ushiroda; R. van Tonder; L. Vitale; R. Volpe; M.-Z. Wang; M. Watanabe; B. D. Yabsley; S. Yamada; Y. Zhang; Q. D. Zhou
The journal of high energy physics, 05/2024, Volume: 2024, Issue: 5Journal Article
Abstract We report results from a study of B ± → DK ± decays followed by D decaying to the CP-even final state K + K − and CP-odd final state K S 0 π 0 $$ {K}_S^0{\pi}^0 $$ , where D is an admixture of D 0 and D ¯ 0 $$ {\overline{D}}^0 $$ states. These decays are sensitive to the Cabibbo-Kobayashi-Maskawa unitarity-triangle angle ϕ 3. The results are based on a combined analysis of the final data set of 772 × 106 B B ¯ $$ B\overline{B} $$ pairs collected by the Belle experiment and a data set of 198 × 106 B B ¯ $$ B\overline{B} $$ pairs collected by the Belle II experiment, both in electron-positron collisions at the Υ(4S) resonance. We measure the CP asymmetries to be A $$ \mathcal{A} $$ CP+ = (+12.5 ± 5.8 ± 1.4)% and A $$ \mathcal{A} $$ CP− = (−16.7 ± 5.7 ± 0.6)%, and the ratios of branching fractions to be R $$ \mathcal{R} $$ CP+ = 1.164 ± 0.081 ± 0.036 and R $$ \mathcal{R} $$ CP− = 1.151 ± 0.074 ± 0.019. The first contribution to the uncertainties is statistical, and the second is systematic. The asymmetries A $$ \mathcal{A} $$ CP+ and A $$ \mathcal{A} $$ 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 ° < ϕ 3 < 16.5 ° ) or (84.5 ° < ϕ 3 < 95.5 ° ) or (163.3 ° < ϕ 3 < 171.5 ° ) and 0.321 < r B < 0.465.
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