We consider non-zero temperature properties of the polarized two-component
Fermi gas. We point out that stable polarized paired states which are more
stable than their phase separated counterparts with unpolarized superfluid
region can exist below the critical temperature. We also solve the system
behavior in a trap using the local density approximation and find gradually
increasing polarization in the center of the system as the temperature is
increased. However, in the strongly interacting region the central polarization
increases most rapidly close to the mean-field critical temperature, which is
known to be substantially higher than the critical temperature for
superfluidity. This indicates that most of the phase separation occurs in the
fluctuation region prior to superfluidity and that the polarization in the
actual superfluid is modest.Comment: Final published versio