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Separation of the monopole contribution to the nuclear Hamiltonian

Andr'es P. Zuker·Marianne Dufour
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Abstract

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.

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Andr'es P. Zuker, Marianne Dufour. 1995-05-08. Separation of the monopole contribution to the nuclear Hamiltonian. https://arxiv.org/abs/nucl-th/9505012

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