  The mixed model of the large $ N $ induced QCD, with $ N_f \ll N $ flavors of
heavy fermions in fundamental representation, is solved in the local limit. The
$ Z_N$ symmetry is broken spontaneously in the large $ N $ limit, evading the
Elitzur "no-go" theorem. As a result of this symmetry breaking, there is the
Bose condensate of the eigenvalues of the scalar field, proportional to $
\frac{N_f}{N} $. This condensate leads to the mass unit, which goes to zero as
fractional power of $ \frac{N_f}{N} $, thus defining the new kind of the local
limit of this lattice theory. There is a strong coupling region below this mass
scale, which revives the hopes of induction of realistic QCD.
