A method for reaction calculations is outlined in which it is not nece
ssary to obtain the complicated continuum wave function from the posit
ive-energy Schrodinger equation. Instead, one must solve a negative-en
ergy Schrodinger-type equation with a localized source term. Its solut
ions are localized. They are similar to bound-state wave functions and
are much easier to obtain, since here one does not need to impose lar
ge-distance boundary conditions. All the 2-->N reaction amplitudes are
expressed in a simple way in terms of these solutions. In calculating
inclusive cross sections of perturbation-induced reactions the diffic
ult summation over the final states is avoided as well. Some simple ap
plications of the method and its present status are discussed.