Theoretical study of the $KK\bar K$ system and dynamical generation of the K(1460) resonance

TL;DR

This paper investigates the $KKar K$ system using coupled channel Faddeev equations and a potential model, revealing a quasibound state around 1420 MeV that corresponds to the K(1460) resonance.

Contribution

It provides a detailed theoretical analysis of the $KKar K$ system, demonstrating the dynamical generation of the K(1460) resonance through two different approaches.

Findings

Identified a quasibound state near 1420 MeV with I=1/2 and J^π=0^-.

The state corresponds to the experimentally observed K(1460) resonance.

Both approaches yield consistent results for the $KKar K$ system.

Abstract

The $K K\bar K$ system is investigated with a coupled channel approach based on solving the Faddeev equations considering the $KK\bar K$, $K\pi\pi$ and $K\pi\eta$ channels and using as input two-body $t$-matrices that generate dynamically the $f_0(980)$ and $a_0(980)$ resonances. In the present calculation, a quasibound state around 1420 MeV with total isospin $I=1/2$ and spin-parity $J^\pi=0^-$ is found below the three kaon threshold. This state can be identified with the K(1460) resonance listed by the Particle Data Group. We also study the $KK\bar K$ system in a single channel three-body potential model with two-body effective $KK$ and $K\bar K$ interactions, in which the $K\bar K$ interaction is adjusted to reproduce the properties of the $f_0(980)$ and $a_0(980)$ resonances as $K\bar K$ bound states, obtaining a very similar result to the one found in the Faddeev approach.