First Measurements of Absolute Branching Fractions of the Ξ_{c}^{0} Baryon at Belle.

Y B Li,C P Shen, C Z Yuan,I Adachi,H Aihara,S Al Said,D M Asner,T Aushev, R Ayad,I Badhrees, Y Ban,V Bansal, C Beleño, M Berger,V Bhardwaj,B Bhuyan, T Bilka,J Biswal, A Bondar, A Bozek, M Bračko, L Cao,D Červenkov,A Chen,B G Cheon,K Chilikin,K Cho,S-K Choi,Y Choi,D Cinabro,S Cunliffe,S Di Carlo,Z Doležal, T V Dong, Z Drásal, S Eidelman,J E Fast,B G Fulsom,R Garg, V Gaur,N Gabyshev,A Garmash,A Giri, P Goldenzweig,D Greenwald,B Grube, K Hayasaka, H Hayashii,C-L Hsu,T Iijima,K Inami, G Inguglia,A Ishikawa,R Itoh,M Iwasaki, Y Iwasaki,W W Jacobs,S Jia,Y Jin,D Joffe,K K Joo, G Karyan, T Kawasaki,H Kichimi,D Y Kim, H J Kim,J B Kim,K T Kim, S H Kim,K Kinoshita, P Kodyš,S Korpar, D Kotchetkov,P Križan,R Kroeger,P Krokovny,T Kumita,A Kuzmin,Y-J Kwon,J Y Lee,S C Lee,L K Li,L Li Gioi,J Libby,D Liventsev, M Lubej,J MacNaughton, M Masuda,T Matsuda,M Merola,K Miyabayashi,H Miyata,R Mizuk,G B Mohanty, R Mussa, E Nakano,M Nakao,K J Nath,M Nayak,M Niiyama,S Nishida,H Ono, Y Onuki,P Pakhlov,G Pakhlova,B Pal,S Pardi,S-H Park,S Paul, T K Pedlar, R Pestotnik, L E Piilonen,V Popov, E Prencipe,G Russo, Y Sakai,M Salehi,S Sandilya, L Santelj,T Sanuki, V Savinov,O Schneider, G Schnell,J Schueler, C Schwanda,A J Schwartz, Y Seino,K Senyo,M E Sevior,T-A Shibata,J-G Shiu, B Shwartz,E Solovieva, M Starič, M Sumihama, T Sumiyoshi, W Sutcliffe,M Takizawa,K Tanida,Y Tao, F Tenchini,K Trabelsi,M Uchida,T Uglov, Y Unno,S Uno, P Urquijo,R Van Tonder, G Varner,B Wang,C H Wang,M-Z Wang,P Wang,X L Wang,E Won,S B Yang,H Ye, J Yelton, J H Yin,Y Yusa, Z P Zhang,V Zhilich,V Zhukova,

PHYSICAL REVIEW LETTERS(2019)

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摘要
We present the first measurements of absolute branching fractions of Ξ_{c}^{0} decays into Ξ^{-}π^{+}, ΛK^{-}π^{+}, and pK^{-}K^{-}π^{+} final states. The measurements are made using a dataset comprising (772±11)×10^{6} BB[over ¯] pairs collected at the ϒ(4S) resonance with the Belle detector at the KEKB e^{+}e^{-} collider. We first measure the absolute branching fraction for B^{-}→Λ[over ¯]_{c}^{-}Ξ_{c}^{0} using a missing-mass technique; the result is B(B^{-}→Λ[over ¯]_{c}^{-}Ξ_{c}^{0})=(9.51±2.10±0.88)×10^{-4}. We subsequently measure the product branching fractions B(B^{-}→Λ[over ¯]_{c}^{-}Ξ_{c}^{0})B(Ξ_{c}^{0}→Ξ^{-}π^{+}), B(B^{-}→Λ[over ¯]_{c}^{-}Ξ_{c}^{0})B(Ξ_{c}^{0}→ΛK^{-}π^{+}), and B(B^{-}→Λ[over ¯]_{c}^{-}Ξ_{c}^{0})B(Ξ_{c}^{0}→pK^{-}K^{-}π^{+}) with improved precision. Dividing these product branching fractions by the result for B^{-}→Λ[over ¯]_{c}^{-}Ξ_{c}^{0} yields the following branching fractions: B(Ξ_{c}^{0}→Ξ^{-}π^{+})=(1.80±0.50±0.14)%, B(Ξ_{c}^{0}→ΛK^{-}π^{+})=(1.17±0.37±0.09)%, and B(Ξ_{c}^{0}→pK^{-}K^{-}π^{+})=(0.58±0.23±0.05)%. For the above branching fractions, the first uncertainties are statistical and the second are systematic. Our result for B(Ξ_{c}^{0}→Ξ^{-}π^{+}) can be combined with Ξ_{c}^{0} branching fractions measured relative to Ξ_{c}^{0}→Ξ^{-}π^{+} to yield other absolute Ξ_{c}^{0} branching fractions.
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