  In the possible scaling region for lattice chiral fermions advocated in
hep-lat/9609037, no hard spontaneous symmetry breaking occurs and doublers are
gauge-invariantly decoupled via mixing with composite three-fermion-states.
However the strong coupling expansion breaks down due to no ``static limit''
for the low-energy limit ($p\sim 0$). We further analyze relevant Green
functions of three-fermion-operators. It is shown that in the low-energy limit,
the propagators of three-fermion-states with the ``wrong'' chiralities
positively vanish due to the generalized form factors (the wave-function
renormalizations) of these composite states vanishing as $O(p^4)$. This
strongly implies that three-fermion-states with ``wrong'' chirality are
``decoupled'' in this limit.
