Abstract
We determine the triton binding energies for a class of potentials that arise from radial-distortion unitary transformations. These potentials are phase-shift equivalent to a two-term Yukawa potential, which represents an average of the $^{3}S_{1}$ and $^{1}S_{0}$ nucleon-nucleon potentials. We solve an angular-momentum-decomposed version of the Faddeev-Lovelace equations that we have developed, in order to obtain the three-body binding energy ${E}_{T}$. We observe that ${E}_{T}$ varies slightly with these potentials and we find that they yield similar deuteron wave functions in accord with the results reported by Haftel. We discuss some evidence on the sensitivity of nuclear matter and three-body calculations to off-shell variations of the two-body $t$ matrices.[NUCLEAR STRUCTURE $^{3}\mathrm{H}$; calculated binding energy. Solved Faddeev-Love-lace equations, angular-momentum decomposed. Deduced deuteron form factors.]
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