  The behavior of Fermi systems which approach the fermion condensation quantum
phase transition (FCQPT) from the disordered phase is considered. We show that
the quasiparticle effective mass $M^*$ diverges as $M^*\propto 1/|x-x_{FC}|$
where $x$ is the system density and $x_{FC}$ is the critical point at which
FCQPT occurs. Such a behavior is of general form and takes place in both three
dimensional (3D) systems and two dimensional (2D) ones. Since the effective
mass $M^*$ is finite, the system exhibits the Landau Fermi liquid behavior. At
$|x-x_{FC}|/x_{FC}\ll 1$, the behavior can be viewed as a highly correlated
one, because the effective mass is large and strongly depends on the density.
In case of electronic systems the Wiedemann-Franz law is held and
Kadowaki-Woods ratio is preserved. Beyond the region $|x-x_{FC}|/x_{FC}\ll 1$,
the effective mass is approximately constant and the system becomes
conventional Landau Fermi liquid.
