Abudinen, F.Aggarwal, L.Ahmed, H.Aihara, H.Akopov, N.Al Said, S.Aloisio, A.Ky, N. AnhAsner, D. M.Atmacan, H.Aushev, V.Ayad, R.Babu, V.Bacher, S.Baehr, S.Bahinipati, S.Bambade, P.Banerjee, SwBansal, S.Baudot, J.Becker, J.Behera, P. K.Belous, K.Bennett, J.Bernlochner, F. U.Bertemes, M.Bertholet, E.Bessner, M.Bettarini, S.Bianchi, F.Bilka, T.Biswas, D.Bobrov, A.Bodrov, D.Bonvicini, G.Borah, J.Bozek, A.BraCko, M.Branchini, P.Briere, R. A.Browder, T. E.Budano, A.Bussino, S.Campajola, M.Cao, L.Casarosa, G.Cecchi, C.Cervenkov, D.Cheema, P.Chekelian, V.Chen, A.Cheon, B. G.Chilikin, K.Chirapatpimol, K.Cho, H. -E.Cho, S. -J.Choi, S. -K.Choi, Y.Choudhury, S.Cinabro, D.Corona, L.Cunliffe, S.Czank, T.Das, S.Dattola, F.De La Cruz-Burelo, E.de Marino, G.Maurya, S. K.De Nardo, G.De Nuccio, M.De Pietro, G.de Sangro, R.Destefanis, M.Dey, S.De Yta-Hernandez, A.Dhamija, R.Di Canto, A.Dolezal, Z.Dominguez Jimenez, I.Dong, T.Dorigo, M.Dossett, D.Dubey, S.Dujany, G.Eliachevitch, M.Epifanov, D.Feichtinger, P.Ferlewicz, D.Fillinger, T.Fiore, S.Fodor, A.Forti, F.Fulsom, B. G.Gabrielli, A.Ganiev, E.Garcia-Hernandez, M.Gaur, V.Gaz, A.Giordano, R.Giri, A.Glazov, A.Godang, R.Goldenzweig, P.Golob, B.Gradl, W.Graziani, E.Greenwald, D.Gu, T.Guan, Y.Gudkova, K.Guilliams, J.Hadjivasiliou, C.Halder, S.Hara, T.Hartbrich, O.Hayasaka, K.Hayashii, H.Hazra, S.Heredia de la Cruz, I.Hershenhorn, A.Higuchi, T.Hill, E. C.Hou, W. -S.Hsu, C. -L.Iijima, T.Inami, K.Ishikawa, A.Iwasaki, M.Jacobs, W. W.Jang, E. -J.Jin, Y.Junkerkalefeld, H.Kaliyar, A. B.Kang, K. H.Karl, R.Karyan, G.Kato, Y.Ketter, C.Kiesling, C.Kim, C. -H.Kim, D. Y.Kim, K. -H.Kim, Y. -K.Kinoshita, K.Kodys, P.Koga, T.Kohani, S.Korpar, S.Kovalenko, E.Kraetzschmar, T. M. G.Krizan, P.Krokovny, P.Kuhr, T.Kumar, J.Kumar, M.Kumar, R.Kumara, K.Kuzmin, A.Kwon, Y. -J.Lacaprara, S.Lai, Y. -T.La Licata, C.Lanceri, L.Lange, J. S.Leboucher, R.Lee, S. C.Leitl, P.Li, J.Li, S. X.Li Gioi, L.Libby, J.Lieret, K.Liptak, Z.Liu, Q. Y.Liventsev, D.Longo, S.Lueck, T.Lyu, C.Maggiora, M.Maiti, R.Maity, S.Manfredi, R.Manoni, E.Marcello, S.Martini, A.Massaccesi, L.Masuda, M.Matsuoka, K.Matvienko, D.McKenna, J. A.Meier, F.Merola, M.Metzner, F.Milesi, M.Miller, C.Miyabayashi, K.Mizuk, R.Mohanty, G. B.Molina-Gonzalez, N.Moser, H. -G.Mueller, F.Murphy, C.Mussa, R.Nakamura, K. R.Nakano, T.Nakao, M.Naruki, M.Narwal, D.Natochii, A.Nayak, L.Nayak, M.Nazaryan, G.Nisar, N. K.Nishida, S.Nishimura, K.Onishchuk, Y.Ono, H.Oskin, P.Pakhlova, G.Paladino, A.Panta, A.Paoloni, E.Parham, K.Park, S. -H.Passeri, A.Pathak, A.Patra, S.Pestotnik, R.Piilonen, L. E.Podobnik, T.Pokharel, S.Polat, L.Praz, C.Prell, S.Prencipe, E.Prim, M. T.Purwar, H.Rabusov, A.Rados, P.Raiz, S.Reiter, S.Remnev, M.Ripp-Baudot, I.Rizzo, G.Rizzuto, L. B.Robertson, S. H.Rohrken, M.Roney, J. M.Rostomyan, A.Rout, N.Sahoo, D.Sanders, D. A.Sandilya, S.Santelj, L.Sato, Y.Savinov, V.Scavino, B.Schnell, G.Schueler, J.Schwartz, A. J.Seino, Y.Selce, A.Senyo, K.Sevior, M. E.Shapkin, M.Sharma, C.Shillington, T.Shwartz, B.Sibidanov, A.Simon, F.Singh, J. B.Soffer, A.Solovieva, E.Spataro, S.Spruck, B.Stefkova, S.Stottler, Z. S.Stroili, R.Sumisawa, K.Sutcliffe, W.Suzuki, S. Y.Tabata, M.Takizawa, M.Tanida, K.Tenchini, F.Tiwary, R.Tonelli, D.Torassa, E.Trabelsi, K.Uchida, M.Ueda, I.Uglov, T.Uno, K.Uno, S.Ushiroda, Y.Vahsen, S. E.van Tonder, R.Varvell, K. E.Vinokurova, A.Vitale, L.Wakeling, H. M.Wang, E.Wang, M. -Z.Wang, X. L.Warburton, A.Watanuki, S.Werbycka, O.Wessel, C.Won, E.Yabsley, B. D.Yan, W.Ye, H.Yoshihara, K.Yusa, Y.Zani, L.Zhai, Y.Zhang, Y.Zhilich, V.Zhou, Q. D.Zhou, X. Y.Zhukova, V.2024-01-222024-01-222022-02-091029-8479https://hdl.handle.net/10919/117468We present a measurement of the Cabibbo-Kobayashi-Maskawa unitarity triangle angle ϕ3 (also known as γ) using a model-independent Dalitz plot analysis of B+ → D (KS0h+h−)h+, where D is either a D0 or D¯ 0 meson and h is either a π or K. This is the first measurement that simultaneously uses Belle and Belle II data, combining samples corresponding to integrated luminosities of 711 fb−1 and 128 fb−1, respectively. All data were accumulated from energy-asymmetric e+e− collisions at a centre-of-mass energy corresponding to the mass of the Υ(4S) resonance. We measure ϕ3 = (78.4 ± 11.4 ± 0.5 ± 1.0)°, where the first uncertainty is statistical, the second is the experimental systematic uncertainty and the third is from the uncertainties on external measurements of the D-decay strong-phase parameters. [Figure not available: see fulltext.]34 page(s)application/pdfenIn CopyrightB PhysicsCKM Angle Gammae(-)-e(-) ExperimentsArticle - Refereedhttps://doi.org/10.1007/JHEP02(2022)06320222Piilonen, Leo [0000-0001-6836-0748]1029-8479