Abstract
Using the local hidden gauge approach, we study the possibility of the existence of bottomed strange molecular states with isospin 0. We find three bound states with spin-parity $0^+$, $1^+$ and $2^+$ generated by the $\bar{K}^*B^*$ and $\omega B_s^*$ interaction, among which the state with spin 2 can be identified as $B_{s2}^*(5840)$. In addition, we also study the $\bar{K}^*B$ and $\omega B_s$ interaction and find a bound state which can be associated to $B_{s1}(5830)$. Besides, the $\bar{K}B^*$ and $\eta B_s^*$ and $\bar{K}B$ and $\eta B_s$ systems are studied, and two bound states are predicted. We expect that further experiments can confirm our predictions.
Highlights
We find three bound states with spin parity 0þ, 1þ, and 2þ generated by the K ÃBÃ and ωBÃs interaction, among which the state with spin 2 can be identified as BÃs2ð5840Þ
The local hidden gauge symmetry was introduced in Refs. [1,2,3,4] which regards vector mesons as the gauge bosons and pseudoscalar mesons as the Goldstone bosons
As mentioned in the previous subsection, the Bs1ð5830Þ cannot be explained as the K ÃBÃ bound state with spin 1, since in the Particle Data Group (PDG) the mass of Bs1ð5830Þ is smaller than that of BÃs2ð5840Þ, which is contrary to our results
Summary
The local hidden gauge symmetry was introduced in Refs. [1,2,3,4] which regards vector mesons as the gauge bosons and pseudoscalar mesons as the Goldstone bosons. [6] with a mass and width around 1800 and 80 MeV, respectively. This state, h1ð1800Þ, is dynamically generated from the KÃK Ã interaction, and it was investigated in the process J=ψ → ηKÃ0K Ã0 in Ref. BÃs2ð5840Þ was observed by both the CDF and D0 collaborations in the BþK− channel [16,17,18]. The LHCb Collaboration first measured the mass and width of BÃs2ð5840Þ in the BÃþK− channel.
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