We point out that the decay mode D-o-->K-o(K) over bar (o) has no factoriza
ble contribution. In chiral perturbation language, treating D-o as heavy, t
he O(p) contribution is zero. We calculate the nonfactorizable chiral loop
contributions of order O(p(3)). Then, we use a heavy-light type chiral quar
k model to calculate nonfactorizable tree level terms, also of order O(p(3)
), proportional to the gluon condensate. A priori, chiral loops are not exp
ected to give good precision because the energy release in this decay is al
most 800 MeV. Still, we find that both the chiral loops and the gluon conde
nsate contributions are of the same order of magnitude as the experimental
amplitude.