  Starting from the historical Fermi four-fermion low-energy effective
electroweak interactions Lagrangian for the third generation of quarks,
augmented by an NJL type interaction responsible for dynamical symmetry
breaking and heavy quark mass generation, and fixing the scalar (Higgs) field
v.e.v. at v = 247 GeV, we show that: (1) heavy quark bound states Q\bar Q with
quantum numbers of the W^\pm bosons exist for arbitrarily weak (positive)
vector coupling G_F, so long as the quark mass is sufficiently large; (2) a
massive composite neutral vector boson (Z^0) appears; (3) a massless composite
parity-conserving neutral vector boson (\gamma) appears, the composite
Higgs-Kibble ghosts decouple from the quarks and other particles, the
longitudinal components of the vector boson propagators vanish, as G_F \to
G_F^expt = 1/(\sqrt2 v^2), which also implies that the cutoff \Lambda \to
\infty. Thus, the Fermi interaction model is equivalent to a locally gauge
invariant theory but with definite values of coupling constants and masses. The
model discussed here was chosen for illustrative purposes and is not equivalent
to the Standard Model.
