Strong decays of the newly observed narrow ΩbΩ_b structures

preprint2020arXivOpen access

Abstract

Motivated by the newly observed narrow structures Ωb(6316)−Ω_b(6316)^-, Ωb(6330)−Ω_b(6330)^-, Ωb(6340)−Ω_b(6340)^-, and Ωb(6350)−Ω_b(6350)^- in the Ξb0K−Ξ_b^0 K^- mass spectrum, we investigate the strong decays of the low-lying ΩbΩ_b states within the 3P0^3P_0 model systematically. According to their masses and decay widths, the observed Ωb(6316)−Ω_b(6316)^-, Ωb(6330)−Ω_b(6330)^-, Ωb(6340)−Ω_b(6340)^-, and Ωb(6350)−Ω_b(6350)^- resonances can be reasonably assigned as the λ−λ-mode Ωb(1P)Ω_b(1P) states with JP=1/2−,3/2−,3/2−J^P=1/2^-, 3/2^-, 3/2^-, and 5/2−5/2^-. Meanwhile, the remaining P−P-wave state with JP=1/2−J^P=1/2^- should have a rather broad width, which can hardly be observed by experiments. For the Ωb(2S)Ω_b(2S) and Ωb(1D)Ω_b(1D) states, our predictions show that these states have relatively narrow total widths and mainly decay into the ΞbKˉΞ_b \bar K, Ξb′KˉΞ_b^\prime \bar K and Ξb′∗KˉΞ_b^{\prime*} \bar K final states. These abundant theoretical predictions may be valuable for searching more excited ΩbΩ_b states in future experiments.

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