We discuss the group theory relevant to the ground-state baryons in la
rge N-c QCD. For very large representation, the group generators becom
e classical variables. We find the form of the classical generators fo
r the completely symmetric N index representation of SU(m) as N --> in
finity and derive an integral formula for the matrix elements of an ar
bitrary polynomial in the group generators between low-spin baryon sta
tes in the large N limit.