The selectivity of the pi-decay branching ratios of the negative parit
y baryon resonances is discussed from a quark model perspective. It is
shown that the selectivity can be understood as a consequence of the
selective clustering into quark-diquark configurations with different
quantum numbers that is caused by the pseudoscalar octet chiral meson
exchange interaction between the constituent quarks. This leads to the
prediction that the resonances N(1535), Lambda(1670), Sigma(1750) wit
h mixed flavour-spin symmetry [21](FS)[21](F)[21](S) in their lowest o
rder wavefunctions should have large eta branching ratios, whereas the
N(1650) and the Lambda(1800) should not.