We calculate the zero-temperature gap and quasiparticle weight of the half-
filled Hubbard model with a random dispersion relation. After extrapolation
to the thermodynamic limit, we obtain reliable bounds on these quantities
for the Hubbard model in infinite dimensions. Our data indicate that the Mo
tt-Hubbard transition is continuous; i.e., the quasiparticle weight becomes
zero at the same critical interaction strength at which the gap opens.