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Excited Ω hyperon in charmful Ωb weak decays

Kai-Lei Wang1,2,*, Juan Wang1,3,†, Yu-Kuo Hsiao3,‡, and Xian-Hui Zhong2,4,§

  • 1Department of Physics, Changzhi University, Changzhi, Shanxi 046011, China
  • 2Synergetic Innovation Center for Quantum Effects and Applications (SICQEA), Hunan Normal University, Changsha 410081, China
  • 3School of Physics and Information Engineering, Shanxi Normal University, Taiyuan 030031, China
  • 4Department of Physics, Hunan Normal University, and Key Laboratory of Low-Dimensional Quantum Structures and Quantum Control of Ministry of Education, Changsha 410081, China

  • *Contact author: wangkaileicz@foxmail.com
  • †Contact author: wjuanmm@163.com
  • ‡Contact author: yukuohsiao@gmail.com
  • §Contact author: zhongxh@hunnu.edu.cn

Phys. Rev. D 111, 114028 – Published 24 June, 2025

DOI: https://doi.org/10.1103/4g99-psnm

Abstract

We investigate the sextet b-baryon decay processes Ωb→J/ψΩ(*), where Ω* represents the 1P-, 1D- and 2S-wave excited Ω hyperons in the spectroscopy. Using the constituent quark model, we obtain B(Ωb→J/ψΩ)=8.8×10−4, which agrees with the previous studies to the order of magnitude. By identifying Ω(2012) as Ω(12P3/2−), B(Ωb→J/ψΩ(2012))=1.1×10−3 can be similarly significant. Additionally, Ω(12D5/2+) and Ω(14D3/2+,14D5/2+) states exhibit production rates of 0.5, and (0.6, 0.8), respectively, relative to their ground-state counterpart. Notably, our findings suggest that B(Ωb→J/ψΩ(22S1/2+,24S3/2+)) are as large as (4.5,20)×10−4, making them accessible to experiments at LHCb.

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