We define nonlinear changes of variables in Berezin integrals, assumin
g as new integration variables multilinear functions of the defining e
lements of the Grassmann algebra. We apply such a change of variables
to QCD by introducing as integration variables trilinear and bilinear
functions of the quark field, with the quantum numbers of the nucleon
and the meson respectively, and we suggest a perturbative scheme using
these functions as free states.