English

Can $\Omega(2012)$ be explained as a molecular state?

High Energy Physics - Phenomenology 2021-02-10 v1

Abstract

We conduct a dynamical calculation of pentaquark systems with quark contents sssuuˉsssu\bar{u} in the framework of two quark models: the chiral quark model(ChQM) and quark delocalization color screening model(QDCSM). The effective potentials between baryon and meson clusters are given, and the possible bound states are also investigated. Besides, the study of the scattering process of the open channels is also performed to look for any resonance state. The results show that the Ω(2012)\Omega(2012) is not suitable for the interpretation as a ΞKˉ\Xi^{*} \bar{K} molecular state in present quark models. Two resonance states: the ΞKˉ\Xi^{*}\bar{K}^{*} with IJP=032IJ^{P}=0\frac{3}{2}^{-} (M=23282374M=2328\sim2374 MeV, Γ=5765.5\Gamma=57\sim65.5 MeV) and IJP=132IJ^{P}=1\frac{3}{2}^{-} (M=23412386M=2341\sim2386 MeV, Γ=31.5100\Gamma=31.5\sim100 MeV) are obtained in both QDCSM and ChQM, which indicates that both of these two states are more possible to be existed and worthy of being searched by future experiments.

Keywords

Cite

@article{arxiv.2010.15398,
  title  = {Can $\Omega(2012)$ be explained as a molecular state?},
  author = {Xuejie Liu and Hongxia Huang and Jialun Ping and Dianyong Chen},
  journal= {arXiv preprint arXiv:2010.15398},
  year   = {2021}
}

Comments

9 pages, 4 figures

R2 v1 2026-06-23T19:44:11.764Z