Negative parity baryons in the expansion: the quark excitation versus the meson-nucleon resonance picture
arXiv:1106.4992 · doi:10.1103/PhysRevD.84.056013
Abstract
In order to better understand the fundamental issue regarding the compatibility between the quark-shell picture and that of resonances in meson-nucleon scattering in large QCD we extend the work of Cohen and Lebed on mixed symmetric = 1 baryons to analyze excited states with = 3. We give an explicit proof on the degeneracy of mass eigenvalues of a simple Hamiltonian including operators up to order \emph{i. e.} neglecting corrections in the quark-shell picture in the large limit. We obtain three degenerate multiplets formed of states, as in the case of = 1 baryons. The compatibility between this picture and that of resonances in meson-nucleon scattering is discussed in the light of the present results.
18 pages, 4 tables. Published version. Note that Eqs. A1, A3 and A4 contain SO(3) Clebsch-Gordan coefficients, not Wigner 3j coefficients
References in corpus (3)
Cited by in corpus (5)
- Magnetic moments of the low-lying {1/2}^- octet baryon resonances
- Baryon resonances in large QCD
- baryons in large QCD revisited: The effect on Regge trajectories
- Negative parity baryons in the expansion: the three towers of states revisited
- Towers of positive parity excited baryons and their mixing in the large limit