We present a theory of the low-energy excitations of a ferromagnetic metal
nanoparticle. In addition to the particle-hole excitations, which occur in
a paramagnetic metal nanoparticle, we predict a branch of excitations invol
ving the magnetization-orientation collective coordinate. Tunneling matrix
elements are in general sizable for several different collective states ass
ociated with the same band configuration. We point out that the average cha
nge in ground state spin per added electron differs from noninteracting qua
siparticle expectations, and that the change in the spin polarization, due
to Zeeman coupling, is strongly influenced by Coulomb blockade physics.