Abstract:
It is suggested to describe scattering in a few-body system by means of the projection
formalism based on separation of a finite-dimensional “inner” subspace. If this
“inner” subspace is sufficiently large, the kernels of the modified integral equations
of the Faddeev–Yakubovsky type become small, thereby justifying the use of the
perturbation theory. The expressions for the zero-order amplitudes are obtained which
are completely determined by the inhomogeneous terms in the equations and approach
the exact amplitudes when the “inner” subspace is enlarging.