Abstract
In this paper the author continues the study of the Faddeev-Lovelace equations for the one-dimensional boundary-condition model of three particles. The half-off-shell rearrangement and elastic amplitudes are constructed explicitly for the general case of a model with arbitrary mass ratios and arbitrary strengths for the two-body interactions. These exact amplitudes are shown to satisfy the modified form of the coupled Faddeev-Lovelace equations as well as the equation relating them to the probability amplitude of the dissociation process.
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