  The polarization produced by the relative displacement of the potentials
trapping two spin species of a dilute Fermi gas with $N_\ua=N_\da$ is
calculated at unitarity by assuming phase separation between the superfluid and
a spin polarized phase at zero temperature. Due to the energy cost associated
with pair breaking, the dipole magnetic polarizability vanishes in the linear
limit and exhibits important deviations from the ideal gas behaviour even for
displacements of the order of the size of the atomic cloud. The magnetic
behaviour in the presence of different trapping frequencies for the two spin
species is also discussed.
