  The studies of the quantum corrections for the anisotropy
parameter,$\eta(=\xi_R/\xi_B)$, for the improved actions, $\beta (C_0
L({Plaq.}) + C_1 L({Rect.}))$, are proceeded in the medium to strong coupling
region on anisotropic lattices. The global features for the $\eta$ parameters
as a function of $\beta$ and the coefficient $C_{1}$ have been clarified. It
has been found by the perturbative analysis that as $C_1$ decreases, the slope
of the $\eta(\beta)$ becomes less steep and for the actions whose $C_{1}$ is
less than -0.160, $\eta$ decreases as $\beta$ decreases, contrary to the case
of the standard action. In the medium to strong coupling region, the $\eta$
parameter begins to increase as $\beta$ decreases for all $C_{1}$. This means
that for the actions with $C_{1} < -0.160$, the one-loop perturbative results
for $\eta$ break down qualitatively and the $\eta$ parameters have a dip. As a
result of this dip structure the $\eta$ for Iwasaki's action remains close to
unity in the wide range of $\beta$.
