Analytic results for Mott-Hubbard metal-insulator transitions in N-fol
d degenerate Hubbard models are obtained using the Gutzwiller approxim
ation. It is found that for any commensurate filling with integer (x)
electrons per site, there exists a metal-insulator transition at the c
ritical correlation energy U(c)(N,x)={[square-root x(2N - x + 1) + squ
are-root (x + 1)(2N - X)]2/(2N - x)}\epsilon(x)BAR\, where epsilonBAR
is the energy per particle in the absence of correlation. U(c) increas
es with x reaching the maximum at the half filling x = N. Therefore, i
t is possible for a system to be metallic at half filling and insulati
ng away from half filling. This provides an explanation for the unusua
l metal-insulator transitions observed in fullerides A(x)C60.