  We consider a superfluid transition in two-component dipolar Fermi gases in a
two-dimensional lattice with a weak on-site disorder. The momentum dependent
dipole-dipole interaction amplitude violates the Anderson theorem and in the
weakly interacting regime this leads to an increase of the superfluid
transition temperature. We find that in a sufficiently deep lattice
(tight-binding regime) and in the low momentum limit superfluid properties can
be considered in the same way as in free space replacing the mass of atoms by
an effective mass in the lattice. The disorder-induced increase of the critical
temperature can be significantly more pronounced than in free space.
