Strong decays of the hadronic molecule ${\Omega }^{\ast }(2012)$

Abstract

Strong two- and three-body decays of the new excited hyperon ${\Omega }^{\ast }(2012)$ are discussed in the hadronic molecular approach. The ${\Omega }^{\ast }(2012)$ state is considered to contain the mixed $\Xi \bar{K}$ and $\Omega \eta$ hadronic components. In our calculations we use a phenomenological hadronic Lagrangian describing the coupling of the bound states to its constituents and of the constituents to other hadrons occurring in the final state. Our results show that the decay widths of the two-body decay modes ${\Omega }^{\ast }(2012)\to \Xi \bar{K}$ lie in the few MeV region and are compatible with or dominate over the rates of the three-body modes ${\Omega }^{\ast }(2012)\to \Xi \pi \bar{K}$. The sum of two- and three-body decay widths is consistent with a width of the ${\Omega }^{\ast }(2012)$ originally measured by the Belle Collaboration. A possible scenario for the suppression of the three-body decay rate recently noticed by the Belle Collaboration is due to the dominant admixture of the $\Omega \eta$ hadronic component in the ${\Omega }^{\ast }(2012)$ state.

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Cited by in corpus (10)

• Interpretation of the ${\Omega }_c\to {\pi }^{+}\Omega (2012)\to {\pi }^{+}(\bar{K}\Xi )$ relative to ${\Omega }_c\to {\pi }^{+}\bar{K}\Xi$ from the $\Omega (2012)$ molecular perspective
• Understanding the nature of $\Omega (2012)$ in a coupled-channel approach
• Analysis of $\Omega (2012)$ as a molecule in the chiral quark model
• Further understanding the nature of $\Omega (2012)$ within a chiral quark model
• Observation of $\Omega (2012{)}^{-}\to \Xi (1530)\bar{K}$ and measurement of the effective couplings of $\Omega (2012{)}^{-}$ to $\Xi (1530)\bar{K}$ and $\Xi \bar{K}$
• Identifying triple-strangeness $\Omega$ hyperons in light of recent experimental results
• Evidence for Two Excited ${\Omega }^{-}$ Hyperons
• Structure of the ${\Omega }^{-}(2012)$ with Hamiltonian Effective Field Theory
• Observation of the $\Omega$(2012) baryon at the LHC
• Investigation on the $\Omega (2012)$ from QCD sum rules