  Electron correlations in the two-orbital Hubbard model at half-filling are
investigated by combining dynamical mean field theory with the exact
diagonalization method. We systematically study how the interplay of the intra-
and inter-band Coulomb interactions, together with the Hund coupling, affects
the metal-insulator transition. It is found that if the intra- and inter-band
Coulomb interactions are nearly equal, the Fermi-liquid state is stabilized due
to orbital fluctuations up to fairly large interactions, while the system is
immediately driven to the Mott insulating phase away from this condition. The
effects of the isotropic and anisotropic Hund coupling are also addressed.
