and excited states within a HQSS model
arXiv:1911.06089 · doi:10.1140/epjc/s10052-019-7568-8
Abstract
We study odd parity and resonances using a unitarized coupled-channel framework based on a HQSS-extended Weinberg-Tomozawa baryon-meson interaction, while paying a special attention to the renormalization procedure. We predict a large molecular component for the with a dominant light-degree-of-freedom spin configuration. We discuss the differences between the and states, and conclude that they cannot be SU(3) siblings, whereas we predict the existence of other states, two of them related to the two-pole structure of the . It is of particular interest a pair of and poles, which form a HQSS doublet and that we tentatively assign to the and , respectively. Within this picture, the would be part of a SU(3) sextet, containing either the or the , and that would be completed by the . Moreover, we identify a sextet with the state and the recently discovered . Assuming the equal spacing rule and to complete this multiplet, we predict the existence of a odd parity state, with a mass of 6360 MeV and that should be seen in the channel.
13 pages, 5 figures, 4 tables
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