  We consider a weakly interacting two-component Fermi gas of dipolar particles
(magnetic atoms or polar molecules) in the two-dimensional geometry. The
dipole-dipole interaction (together with the short-range interaction at
Feshbach resonances) for dipoles perpendicular to the plane of translational
motion may provide a superfluid transition. The dipole-dipole scattering
amplitude is momentum dependent, which violates the Anderson theorem claiming
the independence of the transition temperature on the presence of weak
disorder. We have shown that the disorder can strongly increase the critical
temperature (up to 10 nK at realistic densities). This opens wide possibilities
for the studies of the superfluid regime in weakly interacting Fermi gases,
which was not observed so far.
