  Considered is the ${\cal N}=1$ SQCD-like theory with $SU(N_c)$ colors and $0<
N_F<2N_c$ flavors of equal mass $0< m_Q\ll\Lambda_Q$ quarks. Besides, it
includes $N^2_F$ additional colorless but flavored fields $\Phi_{i}^{j}$, with
the large mass parameter $\mu_{\Phi}\gg\Lambda_Q$. The mass spectra of this
$\Phi$-theory are first directly calculated at $0<N_F<N_c$ where the quarks are
weakly coupled, in all different vacua with the unbroken or spontaneously
broken flavor symmetry $U(N_F)\rightarrow U(n_1)\times U(n_2)$.
  Further, the mass spectra of this direct $\Phi$-theory and its Seiberg's dual
variant, the $d\Phi$-theory, are calculated at $3N_c/2<N_F<2N_c$ and various
values of $\mu_{\Phi}/\Lambda_Q\gg 1$ (in strong coupling regimes), using the
dynamical scenario introduced by the author in his previous article \cite{ch3}.
This scenario assumes that quarks can be in two different standard phases only:
either this is the HQ (heavy quark) phase where they are confined, or they are
higgsed. Within the used dynamical scenario, it is shown that mass spectra of
the direct $\Phi$ and dual $d\Phi$ - theories are parametrically different.
  Besides it is shown in the direct $\Phi$-theory that a qualitatively new
phenomenon takes place: under appropriate conditions, the seemingly heavy and
dynamically irrelevant fields $\Phi$ 'return back' and there appear two
additional generations of light $\Phi$-particles with small masses $\mu^{\rm
pole}(\Phi)\ll\Lambda_Q$.
  Also considered is the $X$-theory which is the ${\cal N}=2$ SQCD with
$SU(N_c)$ colors and $0< N_F<2N_c$ flavors of light quarks, broken down to
${\cal N}=1$ by the large mass parameter of the adjoint scalar superfield $X,
\, \mu_X\gg\Lambda_2$. The tight interrelations between these $X$ and $\Phi$
theories are described, in particular, the conditions under which they are
equivalent.
