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CasaisCaspary, R.Casse, G.Cattaneo, M.Cavallero, G.Cavallini, V.Celani, SaraCerasoli, J.Cervenkov, D.Chadwick, A. J.Chahrour, I. C.Chapman, M. G.Charles, M.Charpentier, Ph.Barajas, C. A. ChavezChefdeville, M.Chen, C.Chen, S.Chernov, A.Chernyshenko, S.Chobanova, V.Cholak, SerhiiChrzaszcz, M.Chubykin, A.Chulikov, V.Ciambrone, P.Cicala, M. F.Vidal, X. CidCiezarek, G.Cifra, P.Ciullo, G.Clarke, P. E. L.Clemencic, M.Cliff, H. V.Closier, J.Cobbledick, J. L.Coco, V.Cogan, J.Cogneras, E.Cojocariu, L.Collins, P.Colombo, T.Comerma-Montells, A.Congedo, L.Contu, A.Cooke, N.Corredoira, I.Corti, G.Meldrum, J. J. CotteeCouturier, B.Craik, D. C.Cruz Torres, M.Currie, R.Da Silva, C. L.Dadabaev, S.Dai, L.Dai, X.Dall'Occo, E.Dalseno, J.D'Ambrosio, C.Daniel, J.Danilina, A.d'Argent, P.Davies, J. E.Davis, A.Francisco, O. De Aguiarde Boer, J.De Bruyn, K.De Capua, S.De Cian, MichelDe Freitas Carneiro Da Graca, U.De Lucia, E.De Miranda, J. 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R. J.Williams, R.Wilson, F. F.Wislicki, W.Witek, M.Witola, L.Wong, C. P.Wormser, G.Wotton, S. A.Wu, H.Wu, J.Wu, Y.Wyllie, K.Xian, S.Xiang, Z.Xie, Y.Xu, A.Xu, J.Xu, L.Xu, M.Xu, Z.Yang, D.Yang, S.Yang, X.Yang, Y.Yang, Z.Yeroshenko, V.Yeung, H.Yin, H.Yu, C. Y.Yu, J.Yuan, X.Zaffaroni, EttoreZavertyaev, M.Zdybal, M.Zeng, M.Zhang, C.Zhang, D.Zhang, J.Zhang, L.Zhang, S.Zhang, Y.Zhao, Y.Zharkova, A.Zhelezov, A.Zheng, Y.Zhou, T.Zhou, X.Zhou, Y.Zhovkovska, V.Zhu, L. Z.Zhu, X.Zhu, Z.Zhukov, V.Zhuo, J.Zou, Q.Zucchelli, S.Zuliani, D.Zunica, G.2024-04-032024-04-032024-04-032024-02-2910.1140/epjc/s10052-023-12376-zhttps://infoscience.epfl.ch/handle/20.500.14299/206947WOS:001185559300001A model-independent study of CP violation in B-0 -> DK (*0) decays is presented using data corresponding to an integrated luminosity of 9 fb(-1) collected by the LHCb experiment at centre-of-mass energies of v s = 7, 8 and 13TeV. The CKM angle. is determined by examining the distributions of signal decays in phase-space bins of the self-conjugate D. K(S)(0)h(+) h(-) decays, where h = p, K. Observables related to CP violation are measured and the angle. is determined to be. = (49+22 -19).. Measurements of the amplitude ratio and strong-phase difference between the favoured and suppressed B-0 decays are also presented.Physical Sciencestext::journal::journal article::research article