  The 't Hooft and Corrigan-Ramond limits of massless one-flavor QCD consider
the two Weyl fermions to be respectively in the fundamental representation or
the two index antisymmetric representation of the gauge group. We introduce a
limit in which one of the two Weyl fermions is in the fundamental
representation and the other in the two index antisymmetric representation of a
generic SU(N) gauge group. This theory is chiral and to avoid gauge anomalies a
more complicated chiral theory is needed. This is the generalized
Georgi-Glashow model with one vector like fermion.
  We show that there is an interesting phase in which the considered chiral
gauge theory, for any N, Higgses via a bilinear condensate: The gauge
interactions break spontaneously to ordinary massless one-flavor SU(3) QCD. The
additional elementary fermionic matter is uncharged under this SU(3) gauge
theory. It is also seen that when the number of colors reduce to three it is
exactly this hidden QCD which is revealed.
