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Separation of the monopole contribution to the nuclear Hamiltonian

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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http://hal.in2p3.fr/in2p3-00087665
Contributor : Dominique Girod <>
Submitted on : Wednesday, July 26, 2006 - 11:39:14 AM
Last modification on : Thursday, April 23, 2020 - 2:26:21 PM

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A.P. Zuker, M. Dufour. Separation of the monopole contribution to the nuclear Hamiltonian. 1995. ⟨in2p3-00087665⟩

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