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\(f_J(2220)\) and hadronic
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  • 作者:Y. K. Hsiao (1) (2)
    C. Q. Geng (1) (2) (3)

    1. Physics Division
    ; National Center for Theoretical Sciences ; Hsinchu ; 300 ; Taiwan
    2. Department of Physics
    ; National Tsing Hua University ; Hsinchu ; 300 ; Taiwan
    3. College of Mathematics and Physics
    ; Chongqing University of Posts and Telecommunications ; Chongqing ; 400065 ; China
  • 刊名:The European Physical Journal C - Particles and Fields
  • 出版年:2015
  • 出版时间:March 2015
  • 年:2015
  • 卷:75
  • 期:3
  • 全文大小:298 KB
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  • 刊物类别:Physics and Astronomy
  • 刊物主题:Physics
    Elementary Particles and Quantum Field Theory
    Nuclear Physics, Heavy Ions and Hadrons
    Physics beyond the Standard Model
    Measurement Science and Instrumentation
    Astronomy, Astrophysics and Cosmology
  • 出版者:Springer Berlin / Heidelberg
  • ISSN:1434-6052
文摘
We study the hadronic \(\bar{B}^0_s\) decays based on the existence of the resonant state \(f_J(2220)\) . In particular, we are able to explain the unexpected large experimental result of \(\mathcal{B}(\bar{B}^0_s\rightarrow J/\psi p\bar{p}) =(3.0^{+1.2}_{-1.1}\pm 0.52\pm 0.03)\times 10^{-6}\) measured recently by the LHCb collaboration due to the resonant contribution in \(\bar{B}^0_s\rightarrow J/\psi f_J(2220)\) with \(f_J(2220) \rightarrow p\bar{p}\) , while it is estimated to be at most of order \(10^{-9}\) in terms of the OZI rule without the resonance. In addition, we find that \(\mathcal{B}(\bar{B}^0_s\rightarrow D^{*0}(f_J\rightarrow ) p\bar{p})=(4.70\pm 2.89)\times 10^{-7}\) , \(\mathcal{B}(\bar{B}^0_s\rightarrow J/\psi (f_J\rightarrow )\pi \pi )=(15.6\pm 15.2)\times 10^{-6}\) , and \(\mathcal{B}(\bar{B}^0_s\rightarrow D^{*0}(f_J\rightarrow )\pi \pi )=(24.5\pm 24.4)\times 10^{-7}\) , while \(\mathcal{B}(\bar{B}^0_s\rightarrow J/\psi (f_J\rightarrow )K\bar{K}) and \(\mathcal{B}(\bar{B}^0_s\rightarrow D^{*0}(f_J\rightarrow )K\bar{K}) . Moreover, we predict that the decay branching ratios of \(\bar{B}^0_s\rightarrow (J/\psi ,D^{*0})\Lambda \bar{\Lambda }\) are \((2.68\pm 1.23)\times 10^{-7}\) and \((2.25\pm 0.80)\times 10^{-6}\) . Some of the predicted \(\bar{B}^0_s\) decays are accessible to the experiments at the LHCb.

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