S_3 and the L=1 Baryons in the Quark Model and the Chiral Quark Model

Details S_3 and the L=1 Baryons in the Quark Model and the Chiral Quark Model S_3 and the L=1 Baryons in the Quark Model and the Chiral Quark Model

1998-10-16

arxiv.org/abs/hep-ph/9810392v1

Phys.Rev.D59:094010,1999

Physics

High Energy Physics

High Energy Physics - Phenomenology

24 pages, requires pictex

Scientific paper

10.1103/PhysRevD.59.094010

The S_3 symmetry corresponding to permuting the positions of the quarks within a baryon allows us to study the 70-plet of L=1 baryons without an explicit choice for the spatial part of the quark wave functions: given a set of operators with definite transformation properties under the spin-flavor group SU(3) x SU(2) and under this S_3, the masses of the baryons can be expressed in terms of a small number of unknown parameters which are fit to the observed L=1 baryon mass spectrum. This approach is applied to study both the quark model and chiral constituent quark model. The latter theory leads to a set of mass perturbations which more satisfactorily fits the observed L=1 baryon mass spectrum (though we can say nothing, within our approach, about the physical reasonableness of the parameters in the fit). Predictions for the mixing angles and the unobserved baryon masses are given for both models as well as a discussion of specific baryons.

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