  We investigate the effect of weak disorder on the superfluid properties of
two-component quasi-two-dimensional dipolar Fermi gases. The dipole-dipole
interaction amplitude is momentum dependent, which violates the Anderson
theorem claiming that the weak disorder has practically no influence on the
superfluid transition temperature in the weakly interacting regime. We find
that for dipolar fermions the transition temperature in this regime can be
strongly increased by the disorder like in the purely two-dimensional case.
However, the effect becomes smaller with increasing the intercomponent
fermion-fermion interaction, and in the strongly interacting regime the
superfluid transition temperature in the weak disorder becomes very close to
that in the absence of disorder.
