To add my 2 cents. I think what the OP is alluding to (or at least, the article quoted by the OP is alluding to) is the fact that strictly speaking, stationary solutions of the hamiltonian are, well, stationary. So even excited states should be "stable" and remain there for ever, even if there exist lower states. But that is of course assuming that the hamiltonian describing the system is exact. The point is that, in *atomic* physics, it is the coupling to the QED field, which can be shown to be responsible for electronic transitions from excited states to ground states (spontaneous decay). I suppose (but I never read anything about it) that something similar is also at work in the nuclear case.
So spontaneous decay is attributed to the coupling between the empty (vacuum) field and the system at hand (say, the electron cloud in the case of atomic transitions, and the nuclear structure in the case of radioactivity), and it is indeed the quantum nature of the field to which it couples which makes the transitions possible (which would otherwise remain locked up in their stationary state).