  Recently, we pointed out that chiral transformation properties of strong
penguin operators change in the transition from unquenched to (partially)
quenched QCD. As a consequence, new penguin-like operators appear in the
(partially) quenched theory, along with new low-energy constants, which should
be interpreted as a quenching artifact. Here, we extend the analysis to the
contribution of the new low-energy constants to the K^0 -> pi^+ pi^- amplitude,
at leading order in chiral perturbation theory, and for arbitrary (momentum
non-conserving) kinematics. Using these results, we provide a detailed
discussion of the intrinsic systematic error due to this (partial) quenching
artifact. We also give a simple recipe for the determination of the
leading-order low-energy constant parameterizing the new operators in the case
of strong $LR$ penguins.
