Tang, S. S.Li, Y. B.Shen, C. P.Adachi, I.Aihara, H.Asner, D. M.Atmacan, H.Aushev, T.Ayad, R.Babu, V.Behera, P.Belous, K.Bessner., M.Bhardwaj., V.Bhuyan., B.Bilka, T.Bodrov, D.Bonvicini, G.Borah, J.Bozek, A.Bracko, M.Branchini, P.Budano, A.Cervenkov, D.Chang, M. -C.Chang, P.Chekelian, V.Cheon, B. G.Chilikin, K.Cho, H. E.Cho, K.Cho, S. -J.Choi, S. -K.Choi, Y.Choudhury, S.Cinabro, D.Das, S.De Pietro, G.Dhamija, R.Di Capua, F.Dingfelder, J.Dolezal, Z.V. Dong, T.Ferlewicz, D.Fulsom, B. G.Garg, R.Gaur, V.Gabyshev, N.Garmash, A.Giri, A.Goldenzweig, P.Graziani, E.Gu, T.Gudkova, K.Hadjivasiliou, C.Hayashii, H.Hedges, M. T.Herrmann, D.Hou, W. -S.Inami, K.Ipsita, N.Ishikawa, A.Itoh, R.Iwasaki, M.Jacobs, W. W.Jia, S.Jin, Y.Joo, K. K.Kang, K. H.Karyan, G.Kiesling, C.Kim, C. H.Kim, D. Y.Kim, K. -H.Kinoshita, K.Kodys, P.Korobov, A.Korpar, S.Kovalenko, E.Krizan, P.Krokovny, P.Kumar, M.Kumara, K.Kwon, Y. -J.Lam, T.Lange, J. S.Lee, S. C.Li, J.Li, L. K.Li, Y.Li Gioi, L.Libby, J.Lieret, K.Liventsev, D.Masuda, M.Matvienko, D.Maurya, S. K.Meier, F.Merola, M.Miyabayashi, K.Mizuk, R.Nakao, M.Natkaniec, Z.Natochii, A.Nayak, L.Nayak, M.Nisar, N. K.Nishida, S.Ogawa, S.Ono, H.Onuki, Y.Pakhlova, G.Pardi, S.Park, S. -H.Passeri, A.Patra, S.Paul, S.Pedlar, T. K.Pestotnik, R.Piilonen, Leo E.Podobnik, T.Prencipe, E.Prim, M. T.Rout, N.Russo, G.Sakai, Y.Sandilya, S.Sangal, A.Santelj, L.Savinov, V.Schnell, G.Schueler, J.Seino, Y.Senyo, K.Sevior, M. E.Shapkin, M.Sharma, C.Shiu, J. -G.Sokolov, A.Solovieva, E.Staric, M.Stottler, Z. S.Sumihama, M.Sumiyoshi, T.Takizawa, M.Tanida, K.Tenchini, F.Trabelsi, K.Uchida, M.Uglov, T.Unno, Y.Uno, K.Uno, S.Urquijo, P.Usov, Y.van Tonder, R.Varner, G.Vinokurova, A.Vossen, A.Waheed, E.Wang, E.Wang, M. -Z.Watanabe, M.Won, E.Xu, X.Yabsley, B. D.Yan, W.Yang, S. B.Yin, J. H.Yuan, C. Z.Yusa, Y.Zhai, Y.Zhang, Z. P.Zhilich, V.Zhukova, V.2024-01-222024-01-222023-02-152470-0010https://hdl.handle.net/10919/117450Based on a data sample of 983 fb-1 collected with the Belle detector at the KEKB asymmetric-energy e+e- collider, we present the study of the heavy-flavor-conserving decay Ξc0→Λc+π- with Λc+ reconstructed via its pK-π+ decay mode. The branching fraction ratio B(Ξc0→Λc+π-)/B(Ξc0→Ξ-π+) is measured to be 0.38±0.04±0.04. Combining with the world average value of B(Ξc0→Ξ-π+), the branching fraction B(Ξc0→Λc+π-) is deduced to be (0.54±0.05±0.05±0.12)%. Here, the uncertainties above are statistical, systematic, and from B(Ξc0→Ξ-π+), respectively.6 page(s)application/pdfenIn CopyrightArticle - Refereedhttps://doi.org/10.1103/PhysRevD.107.0320051073Piilonen, Leo [0000-0001-6836-0748]2470-0029