Wang, D.Yelton, J.Adachi, I.Ahn, J. K.Aihara, H.Asner, D. M.Atmacan, H.Ayad, R.Babu, V.Banerjee, SwBauer, M.Behera, P.Belous, K.Bennett, J.Bessner, M.Bilka, T.Biswas, D.Bodrov, D.Borah, J.Bozek, A.Bracko, M.Branchini, P.Browder, T. E.Budano, A.Campajola, M.Cervenkov, D.Chang, M. -C.Chen, A.Cheon, B. G.Cho, H. E.Cho, K.Cho, S. -J.Choi, S. -K.Choi, Y.Choudhury, S.Cinabro, D.Das, S.De Nardo, G.De Pietro, G.Dhamija, R.Di Capua, F.Dole, Z.Dong, T. V.Dossett, D.Epifanov, D.Ferber, T.Ferlewicz, D.Fulsom, B. G.Garg, R.Gaur, V.Giri, A.Goldenzweig, P.Graziani, E.Gu, T.Gudkova, K.Hadjivasiliou, C.Han, X.Hayasaka, K.Hayashii, H.Hedges, M. T.Hsu, C. -L.Inami, K.Ipsita, N.Ishikawa, A.Itoh, R.Iwasaki, M.Jacobs, W. W.Jang, E. -J.Jia, S.Jin, Y.Kaliyar, A. B.Kang, K. H.Kawasaki, T.Kiesling, C.Kim, C. H.Kim, D. Y.Kim, K. -H.Kim, Y. -K.Kinoshita, K.Kodys, P.Korobov, A.Korpar, S.Kovalenko, E.Krizan, P.Krokovny, P.Kumar, M.Kumar, R.Kumara, K.Kwon, Y. -J.Lam, T.Lange, J. S.Lee, S. C.Levit, D.Lewis, P.Li, L. K.Li, Y.Li, Y. B.Li Gioi, L.Libby, J.Lieret, K.Lin, Y. -R.Liventsev, D.Matsuda, T.Matvienko, D.Meier, F.Merola, M.Metzner, F.Miyabayashi, K.Mizuk, R.Mohanty, G. B.Mussa, R.Nakamura, I.Nakano, T.Nakao, M.Natkaniec, Z.Natochii, A.Nayak, L.Nayak, M.Nisar, N. K.Nishida, S.Ogawa, S.Ono, H.Oskin, P.Pakhlova, G.Pardi, S.Park, H.Park, J.Patra, S.Paul, S.Pedlar, T. K.Pestotnik, R.Piilonen, L. E.Podobnik, T.Prencipe, E.Prim, M. T.Rout, N.Russo, G.Sandilya, S.Sangal, A.Santelj, L.Savinov, V.Schnell, G.Schueler, J.Schwanda, C.Seino, Y.Senyo, K.Sevior, M. E.Shan, W.Shapkin, M.Sharma, C.Shen, C. P.Shiu, J. -G.Sokolov, A.Solovieva, E.Staric, M.Sumihama, M.Sumiyoshi, T.Sutcliffe, W.Takizawa, M.Tamponi, U.Tanida, K.Tenchini, F.Uchida, M.Uno, S.van Tonder, R.Varner, G.Varvell, K. E.Vinokurova, A.Wang, M. -Z.Wang, X. L.Watanabe, M.Watanuki, S.Werbycka, O.Won, E.Xu, X.Yabsley, B. D.Yan, W.Yang, S. B.Yin, J. H.Yuan, C. Z.Yuan, L.Zhang, Z. P.Zhilich, V.Zhukova, V.2024-01-222024-01-222023-02-212470-0010https://hdl.handle.net/10919/117454Using the entire data sample of 980 fb-1 collected at or near the ϒ(4S) resonance with the Belle detector operating at the KEKB asymmetric-energy e+e- collider, we report the measurement of the mass, width, and the branching ratios of the Λc(2625)+ charmed baryon. The mass difference between Λc(2625)+ and Λc+ is measured to be M(Λc(2625)+)-M(Λc+)=341.518±0.006±0.049 MeV/c2. The upper limit on the width is measured to be Γ(Λc(2625)+)<0.52 MeV/c2 at 90% confidence level. Based on a full Dalitz plot fit, branching ratios with respect to the mode Λc(2625)+→Λc+π+π- are measured to be B(Λc(2625)+→ςc0π+)B(Λc(2625)+→Λc+π+π-)=(5.19±0.23±0.40)% and B(Λc(2625)+→ςc++π-)B(Λc(2625)+→Λc+π+π-)=(5.13±0.26±0.32)%, where the first and second uncertainties are statistical and systematic, respectively. These measurements can be used to further constrain the parameters of the underlying theoretical models.10 page(s)application/pdfenIn CopyrightMeasurement of the mass and width of the Lambda(c) (2625)(+) charmed baryon and the branching ratios of Lambda(c) (2625)(+)-> Sigma(0)(c)pi(+) and Lambda(c) (2625)(+) -> Sigma(++)(c)pi(-)Article - RefereedPhysical Review Dhttps://doi.org/10.1103/PhysRevD.107.0320081073Piilonen, Leo [0000-0001-6836-0748]2470-0029