  We study the BCS gap equation for a Fermi gas with unequal population of
spin-up and spin-down states. For $\cosh(\delta_\mu/T) \leq 2$, with $T$ the
temperature and $\delta_\mu$ the chemical potential difference, the question of
existence of non-trivial solutions can be reduced to spectral properties of a
linear operator, similar to the unpolarized case studied previously in
\cite{FHNS,HHSS,HS}. For $\cosh(\delta_\mu/T) > 2$ the phase diagram is more
complicated, however. We derive upper and lower bounds for the critical
temperature, and study their behavior in the small coupling limit.
