Journal of High Energy Physics (Jan 2023)

Evidence for the singly Cabibbo-suppressed decay Ω c 0 → Ξ − π + $$ {\Omega}_c^0\to {\Xi}^{-}{\pi}^{+} $$ and search for Ω c 0 → Ξ − K + $$ {\Omega}_c^0\to {\Xi}^{-}{K}^{+} $$ and Ω − K + decays at Belle

  • The Belle collaboration,
  • X. Han,
  • S. Jia,
  • L. Yuan,
  • C. P. Shen,
  • I. Adachi,
  • J. K. Ahn,
  • H. Aihara,
  • D. M. Asner,
  • T. Aushev,
  • R. Ayad,
  • V. Babu,
  • S. Bahinipati,
  • Sw. Banerjee,
  • P. Behera,
  • K. Belous,
  • J. Bennett,
  • M. Bessner,
  • V. Bhardwaj,
  • T. Bilka,
  • D. Biswas,
  • D. Bodrov,
  • J. Borah,
  • M. Bračko,
  • P. Branchini,
  • T. E. Browder,
  • A. Budano,
  • M. Campajola,
  • D. Červenkov,
  • M.-C. Chang,
  • P. Chang,
  • A. Chen,
  • B. G. Cheon,
  • K. Chilikin,
  • H. E. Cho,
  • K. Cho,
  • S.-K. Choi,
  • Y. Choi,
  • S. Choudhury,
  • D. Cinabro,
  • G. De Nardo,
  • G. De Pietro,
  • R. Dhamija,
  • F. Di Capua,
  • Z. Doležal,
  • T. V. Dong,
  • D. Epifanov,
  • T. Ferber,
  • D. Ferlewicz,
  • B. G. Fulsom,
  • V. Gaur,
  • A. Giri,
  • P. Goldenzweig,
  • E. Graziani,
  • T. Gu,
  • C. Hadjivasiliou,
  • T. Hara,
  • K. Hayasaka,
  • H. Hayashii,
  • W.-S. Hou,
  • C.-L. Hsu,
  • T. Iijima,
  • K. Inami,
  • N. Ipsita,
  • A. Ishikawa,
  • R. Itoh,
  • M. Iwasaki,
  • W. W. Jacobs,
  • E.-J. Jang,
  • Q. P. Ji,
  • Y. Jin,
  • A. B. Kaliyar,
  • C. Kiesling,
  • C. H. Kim,
  • D. Y. Kim,
  • Y.-K. Kim,
  • K. Kinoshita,
  • P. Kodyš,
  • T. Konno,
  • A. Korobov,
  • S. Korpar,
  • E. Kovalenko,
  • P. Križan,
  • P. Krokovny,
  • T. Kuhr,
  • M. Kumar,
  • R. Kumar,
  • K. Kumara,
  • Y.-J. Kwon,
  • T. Lam,
  • M. Laurenza,
  • S. C. Lee,
  • C. H. Li,
  • J. Li,
  • L. K. Li,
  • S. X. Li,
  • Y. Li,
  • Y. B. Li,
  • L. Li Gioi,
  • J. Libby,
  • K. Lieret,
  • M. Masuda,
  • S. K. Maurya,
  • M. Merola,
  • K. Miyabayashi,
  • R. Mizuk,
  • G. B. Mohanty,
  • R. Mussa,
  • I. Nakamura,
  • M. Nakao,
  • H. Nakazawa,
  • Z. Natkaniec,
  • A. Natochii,
  • N. K. Nisar,
  • S. Nishida,
  • S. Ogawa,
  • H. Ono,
  • Y. Onuki,
  • G. Pakhlova,
  • H. Park,
  • J. Park,
  • S. Patra,
  • S. Paul,
  • T. K. Pedlar,
  • R. Pestotnik,
  • L. E. Piilonen,
  • E. Prencipe,
  • M. T. Prim,
  • N. Rout,
  • G. Russo,
  • S. Sandilya,
  • L. Santelj,
  • V. Savinov,
  • G. Schnell,
  • J. Schueler,
  • C. Schwanda,
  • Y. Seino,
  • K. Senyo,
  • M. E. Sevior,
  • W. Shan,
  • M. Shapkin,
  • C. Sharma,
  • J.-G. Shiu,
  • B. Shwartz,
  • E. Solovieva,
  • M. Starič,
  • M. Sumihama,
  • T. Sumiyoshi,
  • M. Takizawa,
  • K. Tanida,
  • F. Tenchini,
  • K. Trabelsi,
  • M. Uchida,
  • T. Uglov,
  • Y. Unno,
  • K. Uno,
  • S. Uno,
  • P. Urquijo,
  • S. E. Vahsen,
  • R. van Tonder,
  • G. Varner,
  • A. Vinokurova,
  • X. L. Wang,
  • E. Won,
  • B. D. Yabsley,
  • W. Yan,
  • S. B. Yang,
  • J. Yelton,
  • J. H. Yin,
  • C. Z. Yuan,
  • Z. P. Zhang,
  • V. Zhilich,
  • V. Zhukova

DOI
https://doi.org/10.1007/JHEP01(2023)055
Journal volume & issue
Vol. 2023, no. 1
pp. 1 – 14

Abstract

Read online

Abstract Using a data sample of 980 fb −1 collected with the Belle detector at the KEKB asymmetric-energy e + e − collider, we study for the first time the singly Cabibbo-suppressed decays Ω c 0 → Ξ − π + $$ {\Omega}_c^0\to {\Xi}^{-}{\pi}^{+} $$ and Ω − K + and the doubly Cabibbo-suppressed decay Ω c 0 → Ξ − K + $$ {\Omega}_c^0\to {\Xi}^{-}{K}^{+} $$ . Evidence for an Ω c 0 $$ {\Omega}_c^0 $$ signal in the Ω c 0 $$ {\Omega}_c^0 $$ → Ξ − π + mode is reported with a significance of 4.5σ including systematic uncertainties. The ratio of branching fractions to the normalization mode Ω c 0 $$ {\Omega}_c^0 $$ → Ω − π + is measured to be B Ω c 0 → Ξ − π + / B Ω c 0 → Ω − π + = 0.253 ± 0.052 stat . ± 0.030 syst . . $$ \mathcal{B}\left({\Omega}_c^0\to {\Xi}^{-}{\pi}^{+}\right)/\mathcal{B}\left({\Omega}_c^0\to {\Omega}^{-}{\pi}^{+}\right)=0.253\pm 0.052\left(\textrm{stat}.\right)\pm 0.030\left(\textrm{syst}.\right). $$ No significant signals of Ω c 0 → Ξ − K + $$ {\Omega}_c^0\to {\Xi}^{-}{K}^{+} $$ and Ω − K + modes are found. The upper limits at 90% confidence level on ratios of branching fractions are determined to be B Ω c 0 → Ξ − K + / B Ω c 0 → Ω − π + < 0.070 $$ \mathcal{B}\left({\Omega}_c^0\to {\Xi}^{-}{K}^{+}\right)/\mathcal{B}\left({\Omega}_c^0\to {\Omega}^{-}{\pi}^{+}\right)<0.070 $$ and B Ω c 0 → Ω − K + / B Ω c 0 → Ω − π + < 0.29 . $$ \mathcal{B}\left({\Omega}_c^0\to {\Omega}^{-}{K}^{+}\right)/\mathcal{B}\left({\Omega}_c^0\to {\Omega}^{-}{\pi}^{+}\right)<0.29. $$

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