  The variety of the phase transitions in Induced QCD are studied. Depending
upon the parameters in the scalar field potential, there could be infinite
number of fixed points, with different critical behavior. The integral equation
for the density of the eigenvalues of the scalar field are generalized to the
weak coupling phases, with the gap at the origin. We find a wide class of the
massive solutions of these integral equations in the strong coupling phases,
and derive an explicit eigenvalue equation for the scalar branch of the mass
spectrum.
