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dc.contributor.authorLAFTCHIEV, H.
hal.structure.identifierInstitut de Physique Nucléaire d'Orsay [IPNO]
dc.contributor.authorLIBERT, J.
hal.structure.identifierCentre d'Etudes Nucléaires de Bordeaux Gradignan [CENBG]
dc.contributor.authorQUENTIN, P.
dc.contributor.authorTHUY LONG, Ha
dc.date.issued2010
dc.identifier.issn0375-9474
dc.description.abstractEnThe so-called Higher Tamm–Dancoff Approximation (HTDA) has been designed to describe microscopically correlations within a particle number conserving approach. It relies upon a truncated n particle–n hole expansion of the nuclear wavefunction, where the single particle basis is optimized self-consistently by using the Skyrme mean field associated with the single-particle density matrix of the correlated wavefunction. It is applied here for the first time in a rotating frame, i.e. within a self-consistent cranking approach (cranked HTDA or CHTDA) aimed at describing the collective rotational motion in well-deformed nuclei. Moments of inertia predicted by cranked HTDA in the Yrast superdeformed (SD) bands of some Anot, vert, similar190 nuclei are compared with those deduced from experimental SD sequences as well as those produced by current cranked Hartree–Fock–Bogoliubov approaches under similar hypotheses.
dc.language.isoen
dc.publisherElsevier
dc.subject.enMicroscopic mean field
dc.subject.enCollective nuclear rotation
dc.subject.enPairing correlations
dc.subject.enNuclear shell model
dc.subject.enTamm–Dancoff approximation
dc.title.enA particle-number conserving description of rotational correlated states
dc.typeArticle de revue
dc.identifier.doi10.1016/j.nuclphysa.2010.04.014
dc.subject.halPhysique [physics]/Physique Nucléaire Expérimentale [nucl-ex]
bordeaux.journalNuclear Physics A
bordeaux.page33-57
bordeaux.volume845
bordeaux.peerReviewedoui
hal.identifierin2p3-00511783
hal.version1
hal.popularnon
hal.audienceNon spécifiée
hal.origin.linkhttps://hal.archives-ouvertes.fr//in2p3-00511783v1
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