Wave-function formalisms in the channel coupling array theory of many-body scattering

Abstract

Wave-function formalisms corresponding to different channel coupling array transition operators of many-body scattering theory are derived and discussed. The Kouri-Levin transition operators are seen to be in typical Lippmann-Schwinger form and allow for the introduction of wave-function components in a particularly straightforward way. The Baer-Kouri transition operators are not in the Lippmann-Schwinger form and an alternate procedure is used to derive their corresponding wave-function components. In the three-body case, the Kouri-Levin operators ${\stackrel{^}{T}}_{\mathrm{jk}}$ obtained from the Faddeev-Lovelace choice of channel coupling array are seen to lead to precisely the Faddeev wave-function components. The Bear-Kouri operators are shown to lead to wave-function components obeying inhomogeneous equations. These inhomogeneous equations are used to give an alternate explanation of the nonunitary amplitudes obtained in recent calculations based on approximate forms of the Baer-Kouri operators.NUCLEAR REACTIONS Many-body scattering theory, channel coupling array wave-function formalisms, aspects of the bound-state type of approximation method, explanation of some nonunitary numerical results of Baer and Kouri and of Lewanski and Tobocman.