We calculate the zero-temperature phase diagram of the disordered Bose-Hubb
ard model in one dimension using the density matrix renormalization group.
For integer filling the Mott insulator is always separated from the superfl
uid by a Bose glass phase. There is a re-entrance of the Bose glass both as
a function of the repulsive interaction and of disorder. At half-filling w
here no Mott insulator exists, the superfluid density has a maximum where t
he kinetic and repulsive energies are about the same. Superfluidity is supp
ressed both for small and very strong repulsion but is always monotonic in
disorder.