We derive the random-phase approximation for spin excitations in general mu
lti-band Hubbard models, starting from a collinear ferromagnetic Hartree-Fo
ck ground state. The results are compared with those from a recently introd
uced variational many-body approach to spin waves in itinerant ferromagnets
. As we exemplify for Hubbard models with one and two bands, the two approa
ches lead to qualitatively different results. The discrepancies can be trac
ed back to the fact that the Hartree-Fock theory fails to describe properly
the local moments which naturally arise in a correlated-electron theory.