New look at the baryon multiplet in the expansion
arXiv:hep-ph/0610099 · doi:10.1016/j.nuclphysa.2008.07.006
Abstract
So far, the masses of excited states of mixed orbital symmetry and in particular those of nonstrange baryons derived in the expansion were based on the separation of a system of quarks into a symmetric core and an excited quark. Here we avoid this separation and show that an advantage of this new approach is to substantially reduce the number of linearly independent operators entering the mass formula. A novelty is that the isospin-isospin term becomes as dominant in as the spin-spin term in resonances.
12 pages, 7 tables, to be published in Nuclear Physics A
References in corpus (5)
Cited by in corpus (9)
- Baryon resonances in large QCD
- SU(6) baryon multiplet in the expansion
- Pion Electroproduction Amplitude Relations in the 1/N_c Expansion
- Group Theoretical Analysis of the Wave Function of the Nonstrange Baryons in the Expansion
- Excited baryon resonances in large QCD
- SU(3) flavor symmetry breaking in large excited hyperons
- Excited Baryons in Large Nc QCD: Matching the 1/Nc expansion to quark models using the permutation group S_N
- Permutation group S_N and hadron spectroscopy
- The baryon multiplet in the expansion revisited