  An effective field theory is derived that describes the quantum critical
behavior of itinerant ferromagnets as the transition is approached from the
ferromagnetic phase. This complements a recent study of the critical behavior
on the paramagnetic side of the phase transition, and investigates the role of
the ferromagnetic Goldstone modes near criticality. We find that the Goldstone
modes have no direct impact on the critical behavior, and that the critical
exponents are the same as determined by combining results from the paramagnetic
phase with scaling arguments.
