The odd-parity strange baryons $\Sigma ({\frac{1}{2}}^{-})$ below 1.8 GeV with Hamiltonian effective field theory

Abstract

We examine the spectrum of the $\Sigma ({\frac{1}{2}}^{-})$ family based on the experimental $K^{-}p$ scattering data and lattice QCD simulations within the Hamiltonian Effective Field Theory. Especially, two different scenarios are constructed in order to clarify whether there is one or two $\Sigma ({\frac{1}{2}}^{-})$ resonances with masses around 1.5$\sim$1.7 GeV. The relevant lattice QCD data support our scenario with two resonance poles at $1687-110i$ and $1714-14i$ MeV in which the bare strange triquark core plays an important role. We also show an extra clear cusp structure around 1.4 GeV in our scattering T matrices associated with the odd-parity strange baryons.

arXiv comment10 pages, 8 figures, 2 tables

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