  The Mott metal-insulator transition in the two-band Hubbard model in infinite
dimensions is studied by using the linearized dynamical mean-field theory. The
discontinuity in the chemical potential for the change from hole to electron
doping is calculated analytically as a function of the on-site Coulomb
interaction $U$, and the charge-transfer energy $\Delta$ between the $d$- and
$p$-orbitals, transfer integrals $t_{pd}$, $t_{pp}$, $t_{dd}$ between $p$-$d$,
$p$-$p$ and $d$-$d$ sites respectively. The critical behaviour of the
quasiparticle weight is also obtained analytically.
