The local density of states is calculated for the Hubbard model in the
limit of infinite dimensions. The noninteracting density of states is
treated as a parameter and is assumed to be rectangular. The calculat
ion is performed using a nonperturbative self-energy solution. At zero
temperature the density of states may be determined analytically. It
is found that the bandwidth broadens due to many-body correlations whi
le the central peak narrows. The possibility of a Mott metal-insulator
transition for the Hubbard model is investigated.