The $\Lambda (1405)$ resonance as a genuine three-quark or molecular state

Abstract

The mechanism for the formation of the $\Lambda (1405)$ resonance is studied in a chiral quark model that includes quark-meson as well as contact (four point) interactions. The negative-parity $S$-wave scattering amplitudes for strangeness $-1$ and $1$ are calculated within a unified coupled-channel framework that includes the $KN$, $\bar{K}N$, $\pi \Sigma$, $\eta \Lambda$, $K\Xi$, $\pi \Lambda$, and $\eta \Sigma$ channels and possible genuine three-quark bare singlet and octet states corresponding to ${\frac{1}{2}}^{-}$ resonances. We show that in order to reproduce the scattering amplitudes in the $S_{01}$ partial wave it is important to include the pertinent three-quark octet states as well as the singlet state, while the inclusion of the contact term is not mandatory. The Laurent-Pietarinen expansion is used to determine the $S$-matrix poles. Following their evolution as a function of increasing interaction strength, the mass of the singlet state is strongly reduced due to the attractive self-energy in the $\pi \Sigma$ and $\bar{K}N$ channels; when it drops below the $KN$ threshold, the state acquires a dominant $\bar{K}N$ component which can be identified with a molecular state. The attraction between the kaon and the nucleon is generated through the $\bar{K}N{\Lambda }^{\ast }$ interaction rather than by meson-nucleon forces.

Comments: 13 pages, 9 figures. Updated results and discussion of dynamical generation of resonances