Abstract

Various quasipotential two-body scattering equations are studied at the one-loop level for the case of tt- and uu-channel exchange potentials. We find that the quasipotential equations devised to satisfy the one-body limit for the tt-channel exchange potential can be in large disagreement with the field-theoretical prediction in the case of uu-channel exchange interactions. Within the spectator model, the description of the uu-channel case improves if another choice of the spectator particle is made. Since the appropriate choice of the spectator depends strongly on the type of interaction used, one faces a problem when both types of interaction are contained in the potential. Equal-time formulations are presented, which, in the light-heavy particle system corresponding to the mass situation of the πN\pi N system, approximate in a reasonable way the field-theoretical result for both types of interactions.Comment: Revtex, 20 pages, 12 PostScript figures, to appear in Phys. Rev.

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