In the possible scaling region for an SU(2) lattice chiral fermion advocate
d in Nucl. Phys. B486, 282 (1997), no hard spontaneous symmetry breaking oc
curs and doublers are gauge-invariantly decoupled via mixing with composite
three-fermion states that are formed by local multifermion interactions. H
owever, the strong coupling expansion breaks down due to the no "static lim
it" for the low-energy limit (pa similar to 0). In both neutral and charged
channels, we further analyze the relevant truncated Green functions of thr
ee-fermion operators by strong coupling expansion and analytical continuati
on of these Green functions in momentum space. It is shown that in the low-
energy limit these relevant truncated Green functions of three-fermion stat
es with the "wrong" chiralities positively vanish due to the generalized fo
rm factors (the wave-function renormalizations) of these composite three-fe
rmion states vanishing as O[(pa)(4)] for pa similar to 0. This strongly imp
lies that the composite three-fermion states with the "wrong'' chirality ar
e "decoupled" in this limit and the low-energy spectrum is chiral; as a con
sequence, chiral gauge symmetries can be exactly preserved.