We construct an effective Lagrangian for low energy hadronic interactions
through an infinite expansion in inverse powers of the low energy cutoff
Λχ of all possible chiral invariant non-renormalizable interactions
between quarks and mesons degrees of freedom. We restrict our analysis to the
leading terms in the 1/Nc expansion. The effective expansion is in
(\mu^2/\cutoff^2 )^P \ln (\cutoff^2/\mu^2 )^Q. Concerning the next-to-leading
order, we show that, while the pure \mu^2/\cutoff^2 corrections cannot be
traced back to a finite number of non renormalizable interactions, those of
order (\mu^2/\cutoff^2 ) \ln (\cutoff^2/\mu^2 ) receive contributions from a
finite set of 1/\cutoff^2 terms. Their presence modifies the behaviour of
observable quantities in the intermediate Q2 region. We explicitely discuss
their relevance for the two point vector currents Green's function.Comment: 41 pages, 11 figures, preprint ROM2F 93/3