  We discuss the application of the momentum-shell renormalization group method
to the interacting homogeneous Bose gas in the symmetric and in the
symmetry-broken phases. It is demonstrated that recently discussed
discrepancies are artifacts of not taking proper care of infrared divergencies
appearing at finite temperature. If these divergencies are taken into account
and treated properly by means of the epsilon-expansion, the resulting
renormalization group equations and the corresponding universal properties are
identical in the symmetric and the symmetry-broken phases.
