Year: 2017
Type: article
Abstract: The pole structure of the $\mathrm{\ensuremath{\Lambda}}(1405)$ is examined by fitting the couplings of an underlying Hamiltonian effective field theory to cross sections of ${K}^{\ensuremath{-}}p$ scattering in the infinite-volume limit. Finite-volume spectra are then obtained from the theory, and compared to lattice QCD results for the mass of the $\mathrm{\ensuremath{\Lambda}}(1405)$. Momentum-dependent, nonseparable potentials motivated by the well-known Weinberg-Tomozawa terms are used, with SU(3) flavor symmetry broken in the couplings and masses. In addition, we examine the effect on the behavior of the spectra from the inclusion of a bare triquarklike isospin-zero basis state. It is found that the cross sections are consistent with the experimental data with two complex poles for the $\mathrm{\ensuremath{\Lambda}}(1405)$, regardless of whether a bare-baryon basis state is introduced or not. However, it is apparent that the bare baryon is important for describing the results of lattice QCD at high pion masses.
Language: Latvian
Subfield: Nuclear and High Energy Physics
Field: Physics and Astronomy
Domain: Physical Sciences
Open Access status: green
OpenAlex ID: W2476112623