Separation of the monopole contribution to the nuclear Hamiltonian
| dc.creator | Zuker, Andr'es P. | |
| dc.creator | Dufour, Marianne | |
| dc.date | 1995-05-08 | |
| dc.date.accessioned | 2026-07-07T05:41:26Z | |
| dc.date.available | 2026-07-07T05:41:26Z | |
| dc.description | It is shown that the nuclear Hamiltonian can be separated rigorously as ${\cal H}={\cal H}_m+{\cal H}_M.$ For sufficiently smooth forces the monopole part ${\cal H}_m $is entirely responsible for Hartree-Fock selfconsistency and hence saturation properties. The multipole part ${\cal H}_M$ contains the ``residual'' terms - pairing, quadrupole, etc. - that will be analyzed in a companion paper. We include a review of the basic results often needed when working with multipole decompositions and average monopole properties. | |
| dc.description | 20 Pages, RevTeX 3.0 | |
| dc.identifier | https://arxiv.org/abs/nucl-th/9505012 | |
| dc.identifier | http://arxiv.org/abs/nucl-th/9505012 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/82569 | |
| dc.subject | Nuclear Theory | |
| dc.title | Separation of the monopole contribution to the nuclear Hamiltonian | |
| dc.type | text |