A scalar field theory with a chi (dagger)chi phi interaction is known to be
unstable. Yet it has been used frequently without any sign of instability
in standard textbook examples and research articles. In order to reconcile
these seemingly conflicting results, we show that the theory is stable if t
he Fock space of all intermediate states is limited to a finite number of c
losed <<chi>(chi )over bar>loops associated with a field chi that appears q
uadradically in the interaction, and that instability arises only when inte
rmediate states include these loops to all orders. In particular, the quenc
hed approximation is stable.