The spin-orbit (LS) force of the hyperon-nucleon interaction is studie
d in the chiral SU(3) quark model. The symmetric LS terms from the one
gluon exchange (OGE) and the scalar nonet exchange (OSE) are taken in
to account. It is shown that two different treatments (the LS coupling
from either OGE or OSE being artificially enhanced in order to reprod
uce the P-3(J) phase shifts of the nucleon-nucleon scattering) lead to
very similar LS couplings in the Sigma N(I = 3/2) channel but give qu
ite different results in the Lambda N - Sigma N(I = 1/2) coupled-chann
el system. A prominent resonance occurs in the P-1(1) state of the Lam
bda N channel mainly due to the stronger LS(-) couplings in the Lambda
N - Sigma N(I = 1/2) coupled-channel system in the OGE enhanced case.
Comparatively the Lambda N P-1(1) phase shift curve exhibits a rather
smooth behaviour in the OSE enhanced case. Comparing our theoretical
results with the experimental data available, and considering the requ
irement of the baryon spectrum, one can deduce that a stronger color-i
ndependent LS coupling is preferred in the chiral quark model. (C) 199
8 Elsevier Science B.V.