Does The 3N-Force Have A Hard Core?
| dc.creator | Eden, J. A. | |
| dc.creator | Gari, M. F. | |
| dc.date | 1996-01-17 | |
| dc.date.accessioned | 2026-07-07T11:15:38Z | |
| dc.date.available | 2026-07-07T11:15:38Z | |
| dc.description | The meson-nucleon dynamics that generates the hard core of the RuhrPot two-nucleon interaction is shown to vanish in the irreducible 3N force. This result indicates a small 3N force dominated by conventional light meson-exchange dynamics and holds for an arbitrary meson-theoretic Lagrangian. The resulting RuhrPot 3N force is defined in the appendix. A completely different result is expected when the Tamm-Dancoff/Bloch-Horowitz procedure is used to define the NN and 3N potentials. In that approach, (e.g. full Bonn potential) both the NN {\it and} 3N potentials contain non-vanishing contributions from the coherent sum of meson-recoil dynamics and the possibility of a large hard core requiring explicit calculation cannot be ruled out. | |
| dc.description | 16 pages REVTeX + 3 ps figs | |
| dc.identifier | https://arxiv.org/abs/nucl-th/9601025 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/9601025 | |
| dc.identifier | Phys.Rev.C53:1510-1518,1996 | |
| dc.identifier | doi:10.1103/PhysRevC.53.1510 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/192446 | |
| dc.subject | Nuclear Theory | |
| dc.title | Does The 3N-Force Have A Hard Core? | |
| dc.type | text |