Separation of the monopole contribution to the nuclear Hamiltonian

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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.
20 Pages, RevTeX 3.0

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Nuclear Theory

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http://salesiana.dossiersoluciones.com/handle/123456789/82569

Consulte el texto completo en el siguiente enlace:

https://arxiv.org/abs/nucl-th/9505012
 http://arxiv.org/abs/nucl-th/9505012

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arXiv