  I show that in the large-N limit the ground state baryons with helicity h
fall into an ((N-2h)/4,(N+2h)/4) irreducible representation of SU(2)XSU(2).
This representation determines the absolute normalization of the ground state
baryon axial vector couplings at large-N. Results map precisely to
(spin-flavor) SU(4) results. For instance, I find g_A =(N+2)/3. As a
consequence of this multiplet structure, chiral symmetry forbids pion
transitions between the ground state baryons and other baryon towers in the
large-N limit.
