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https://doi.org/10.1016/0370-2693(92)91404-w
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Cite Journal: Physics Letters B |  Publication Date: Oct 1, 1992 |
 Citations: 258 |
Affiliation: The University of Texas at Austin
We obtain the nuclear potential coming from the general chiral invariant effective lagrangian up to third order. It consists of a stronger two-body potential and a weaker three-body force. It accounts for the known spin-isospin dependence in the form of contact terms but also yields novel features of finite range.
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