  We continue investigating the Standard Model for one generation of fermions
and two parity-transformed Higgs doublets K and H advocated for in a previous
work, using the one-to-one correspondence, demonstrated there, between their
components and bilinear quark operators. We show that all masses and couplings,
in particular those of the two Higgs bosons $\varsigma$ and $\xi$, are
determined by low energy considerations. The mass of the "quasi-standard" Higgs
boson, $\xi$, is $m_\xi \approx m_\pi$; it is coupled to u and d quarks with
identical strengths. The mass of the lightest one, $\varsigma$, is $m_\varsigma
\approx m_\pi \frac{f_\pi}{2\sqrt{2}m_W/g} \approx\ 34\,KeV$; it is very weakly
coupled to matter except hadronic matter. The ratio of the two Higgs masses is
that of the two scales involved in the problem, the weak scale
$\sigma=\frac{2\sqrt{2}m_W}{g}$ and the chiral scale $v=f_\pi$, which are also
the respective vacuum expectation values of the two Higgs bosons. They can
freely coexist and be accounted for. The dependence of $m_\varsigma$ and
$m_\xi$ on $m_\pi$, that is, on quark masses, suggests their evolution when
more generations are added. Fermions get their masses from both Higgs
multiplets. The theory definitely stays in the perturbative regime.
