Excited baryons in large QCD
arXiv:hep-ph/0505118 · doi:10.1016/j.physletb.2005.09.076
Abstract
The masses of the positive parity and non-strange baryons are calculated in large QCD by considering the most dominant operators in an expansion. The approach is based on the introduction of an excited core, obtained after the last particle (an excited quark) has been removed. Configuration mixing is neglected, for simplicity. Although being a sub-leading order, we find that the spin-spin interaction plays a dominant role in describing the data. The role of operators is also pointed out. We show how the contribution of the linear term in , of the spin-spin and spin-orbit terms vary with the excitation energy.
arXiv comment11 pages, 3 figures, LaTeX, uses espcrc1.sty (included), correspond with the published version
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