We describe the excitation spectrum of a two-component neutral Fermi gas wi
th attractive interactions in the superfluid phase at finite temperature by
deriving a suitable Random-Phase approximation in the collisionless regime
with the technique of functional derivatives. The obtained spectrum for th
e homogeneous gas at small wavevectors contains the Bogoliubov-Anderson pho
non and is essentially different from the spectrum predicted by the static
Bogoliubov theory, which instead shows an unphysically large response. We a
dapt the results for the homogeneous system to obtain the dynamic structure
factor of a harmonically confined superfluid and we identify in the spectr
um a unique feature of the superfluid phase.