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The mass spectrum and magnetic moments of \Xi and \Omega baryon resonancesare investigated in the bound state approach of the Skyrme model. The empiricalhyperon spectrum shows that several hyperon resonances share a pattern of(approximately) equal mass spacings between the states of same spin but ofopposite parity. It is found that this pattern can be explained mostly by theenergy difference between the P-wave and S-wave kaons bound to the soliton.Although one cannot exclude the possibility that these states can be describedas pion-hyperon resonances, the present approach predicts that \Xi(1620) and\Xi(1690) have J^P = 12^-, while \Xi(1950) has J^P = 12^+. The differences withthe quark model predictions for the \Xi and \Omega baryon spectrum are pointedout. Several relations for the masses and magnetic moments of those resonancesare also obtained.Comment: 17 pages, REVTeX, to be published in Phys. Rev.

physical review. d. particles, fields, gravitation, and cosmology/physical review. d, particles, fields, gravitation, and cosmology

<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Ξ</mml:mi></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Ω</mml:mi></mml:math>baryons in the Skyrme model

ΞandΩbaryons in the Skyrme model