We study the ground state of the two-dimensional Anderson-Hubbard mode
l using a quantum real space renormalization group method. We obtain t
he phase diagram near half filling. The system is always insulating wi
th disorder. At half filling, the system undergoes a transition from a
gapless (Anderson) insulator to an incompressible (Mott-Hubbard) insu
lator as the interaction U reaches a critical value U(c). Away from ha
lf filling, the insulating phase is always gapless and is found to be
controlled by the Anderson fixed point at half filling. This result is
similar to that obtained in the corresponding one-dimensional system
and suggests strongly the importance of the electron-electron correlat
ion in this gapless insulating phase.