The Charm and Bottom Hyperons in a Chiral Quark Model

Abstract

The spectrum of the C=1 hyperons is well described by the constituent quark model, if the fine structure interaction between the light and strange quarks is mediated by the $SU(3{)}_F$ octet of light pseudoscalar mesons, which are the Goldstone bosons of the hidden approximate chiral symmetry of QCD. With the addition of a phenomenological flavor exchange interaction of the same form between the light and the charm quarks to describe the ${\Sigma }_c-{\Sigma }_c^{\ast }$ and ${\Xi }_c^s-{\Xi }_c^{\ast }$ splittings, the splittings between the C=1 states fall within 10-30 MeV of the empirical values. Predictions are presented for the lowest negative parity excited states and the magnetic moments as well. Corresponding predictions for the B=-1 hyperon states are also given.

Numerical values in Table 3 for negative parity charm cascade state energies & misprint in Table 1 corrected

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