Abstract
Supersymmetric quantum mechanics links two Hamiltonians with the same scattering (phase equivalence) but different number of bound states. We examine the Green’s functions for these Hamiltonians as a prelude to embedding the two-body dynamics in a many-body system. We study the effect of the elimination of a two-body bound state near zero energy for the Efimov effect and Beg’s theorem.
- Received 20 November 1990
DOI:https://doi.org/10.1103/PhysRevC.43.2077
©1991 American Physical Society

