The constituent quark model can explain the strong selectivity of the
N eta decay branching ratios of the nucleon resonances if the fine str
ucture interaction between the constituent quarks is described in term
s of Goldstone boson exchange. This chiral quark model predicts that t
he resonances N(1535), N(1710), Lambda(1670), Sigma(1750), which have
mixed flavor and spin symmetry [21](FS)[21](F)[21](s) wavefunctions in
lowest order, should have large N eta branching ratios, while N eta d
ecay of the other resonances that have different flavor-spin symmetry
should be strongly suppressed in agreement with the experimental branc
hing ratios.