We investigate, in the context of QCD sum rules, the role of Goldstone
bosons arising from chiral symmetry breaking, especially on the need
of matching the world of hadrons to that of some effective chiral quar
k theory. We describe how such matching yields predictions on induced
condensates which reproduce the observed value of the strong pi NN cou
pling constant. Our result indicate that the observed large pi NN coup
ling comes primarily from the nonperturbative induced-condensate effec
t. On the other hand, the prediction on the parity-violating weak pi N
N coupling, f(pi NN) similar to (3.0+/-0.5) x 10(-7) is in good agreem
ent with the value (similar to 2 x 10(-7)) Obtained by Adelberger and
Haxton from an overall fit to the existing data, but may appear to be
slightly too large (but not yet of statistical significance) as compar
ed to the most recent null experiment. Altogether, we wish to argue th
at the proposal of matching onto a chirally broken effective theory sh
ould enable us to treat, in a quantitative and consistent manner, the
various nonleptonic strong and weak processes involving Goldstone boso
ns.