Here is a set up analgous to the situation of Dirac operator, which in fact I do not really know whether applies to your case because I did not encounter nonlinear operatos before. Let
$$
P:\Gamma(E)\rightarrow \Gamma(F)
$$
be an elliptic differential operator. Then in particular $P$ is Fredholm and it has finite dimensional kernel and cokernel. So we can decompose a section $\phi \in \Gamma(E)$ by
$$
\phi=\phi_1+\phi_2, \phi_1\in \ker (P), \pi(\phi)=\phi_2
$$
and similarly for $\phi\in \Gamma(F)$ we can define $\pi'$ to be the projection map.
Now the associated Green's operator $G:\Gamma(F)\rightarrow \Gamma(E)$ is defined by
$$
G\circ P=Id-\pi, P\circ G=Id-\pi'
$$
I think one way to think about this is via Hodge decomposition theorem: For sufficiently nice elliptic operators (like Dirac operators, Generalized Laplacian operators, etc) over a compact manifold we should have
$$
\Gamma(E)=\ker(P)\oplus Im(P^{*})
$$
where $P^{*}$ is understood as the dual of $P$ in some sense. Then you can think of the Green's operator as a some kind of an inverse to $P$ by omitting elements from the kernel of $P^{*}$. For reference you can check Melrose's notes on index theorem, or the Mathoverflow link.