Cubic Casimir operator of SU(3) and confinement in the nonrelativistic quark model
arXiv:hep-ph/0101007 · doi:10.1016/S0370-2693(01)00008-9
Abstract
Only two-body [] confining potentials have been considered, thus far, in the quark model without gluons, which by construction can only depend on the quadratic Casimir operator of the colour SU(3) group. A three-quark potential that depends on the cubic Casimir operator is added to the quark model. This results in improved properties of colour non-singlet states, which can now be arranged to have (arbitrarily) higher energy than the singlet, and the "colour dissolution/anticonfinement" problem of the model is avoided.
10 pages, 2 tables, RevTex, to appear in Phys. Lett. B
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