Matches in SemOpenAlex for { <https://semopenalex.org/work/W4387013459> ?p ?o ?g. }
Showing items 1 to 80 of
80
with 100 items per page.
- W4387013459 endingPage "012092" @default.
- W4387013459 startingPage "012092" @default.
- W4387013459 abstract "Abstract The shell structure conceived by Mayer and Jensen in 1949 has been shown to be quite appropriate for stable and near-stable nuclei, but substantial deviations from it have also been observed more recently for exotic nuclei with notable neutron excess. Such changes of the basic picture of the nuclear shell structure, called the shell evolution, seem to be the subject studied most extensively and most elaborately by RI beam experiments worldwide. An overview of the shell evolution is presented in this talk, from both theoretical and experimental perspectives. The shell structure is shown to be varied, for instance, from the one presented by Mayer and Jensen, by particular types of the monopole components of the effective nucleon-nucleon interaction in nuclei. Among various contributions, the importance of the tensor force is illuminated here, with an outstanding example: the emergence of new neutron magic number 34 in neutron-rich Ca isotopes. The mechanism of the shell evolution produces significant impacts also on the nuclear shapes. Type II shell evolution shifts the excitation energies of intruder deformed bands, for instance, in some Ni isotopes. In other more general cases, the monopole interaction is shown to produce unexpected crucial effects on the patters of rotational bands of heavy deformed nuclei. In fact, the shape of the ellipsoidal deformation is investigated by large-scale shell model calculations, which is nothing but the Monte Carlo Shell Model. The unique role of the monopole component of the tensor force is clarified: the interplay between this monopole interaction and the quadrupole interaction provides us with various patterns of triaxial shapes for many nuclei, such as 166 Er, one of the traditional prolate deformed heavy nuclei. Thus, the prolate preponderance hypothesis by Aage Bohr is investigated for its microscopic validity. Some of the nuclear paradigms are changing now in this way, due to emerging aspects of nuclear-force effects." @default.
- W4387013459 created "2023-09-26" @default.
- W4387013459 creator A5036770921 @default.
- W4387013459 date "2023-09-01" @default.
- W4387013459 modified "2023-10-03" @default.
- W4387013459 title "Shell evolution and emerging paradigm changes" @default.
- W4387013459 cites W1635055852 @default.
- W4387013459 cites W1983078597 @default.
- W4387013459 cites W1983767566 @default.
- W4387013459 cites W1985289694 @default.
- W4387013459 cites W1993688832 @default.
- W4387013459 cites W2007027697 @default.
- W4387013459 cites W2015668050 @default.
- W4387013459 cites W2043211185 @default.
- W4387013459 cites W2049983086 @default.
- W4387013459 cites W2051307589 @default.
- W4387013459 cites W2069345952 @default.
- W4387013459 cites W2071148930 @default.
- W4387013459 cites W2073462286 @default.
- W4387013459 cites W2079749517 @default.
- W4387013459 cites W2090769236 @default.
- W4387013459 cites W2095270951 @default.
- W4387013459 cites W2468864692 @default.
- W4387013459 cites W2849772005 @default.
- W4387013459 cites W2911409795 @default.
- W4387013459 cites W2991158272 @default.
- W4387013459 cites W2998555783 @default.
- W4387013459 cites W3108675165 @default.
- W4387013459 cites W4214772081 @default.
- W4387013459 cites W4281565326 @default.
- W4387013459 cites W4313557731 @default.
- W4387013459 doi "https://doi.org/10.1088/1742-6596/2586/1/012092" @default.
- W4387013459 hasPublicationYear "2023" @default.
- W4387013459 type Work @default.
- W4387013459 citedByCount "0" @default.
- W4387013459 crossrefType "journal-article" @default.
- W4387013459 hasAuthorship W4387013459A5036770921 @default.
- W4387013459 hasBestOaLocation W43870134591 @default.
- W4387013459 hasConcept C121332964 @default.
- W4387013459 hasConcept C149298590 @default.
- W4387013459 hasConcept C152568617 @default.
- W4387013459 hasConcept C159985019 @default.
- W4387013459 hasConcept C184779094 @default.
- W4387013459 hasConcept C185544564 @default.
- W4387013459 hasConcept C192562407 @default.
- W4387013459 hasConcept C2781052500 @default.
- W4387013459 hasConcept C39984356 @default.
- W4387013459 hasConcept C62520636 @default.
- W4387013459 hasConcept C67327403 @default.
- W4387013459 hasConceptScore W4387013459C121332964 @default.
- W4387013459 hasConceptScore W4387013459C149298590 @default.
- W4387013459 hasConceptScore W4387013459C152568617 @default.
- W4387013459 hasConceptScore W4387013459C159985019 @default.
- W4387013459 hasConceptScore W4387013459C184779094 @default.
- W4387013459 hasConceptScore W4387013459C185544564 @default.
- W4387013459 hasConceptScore W4387013459C192562407 @default.
- W4387013459 hasConceptScore W4387013459C2781052500 @default.
- W4387013459 hasConceptScore W4387013459C39984356 @default.
- W4387013459 hasConceptScore W4387013459C62520636 @default.
- W4387013459 hasConceptScore W4387013459C67327403 @default.
- W4387013459 hasIssue "1" @default.
- W4387013459 hasLocation W43870134591 @default.
- W4387013459 hasOpenAccess W4387013459 @default.
- W4387013459 hasPrimaryLocation W43870134591 @default.
- W4387013459 hasRelatedWork W1966160131 @default.
- W4387013459 hasRelatedWork W1987906394 @default.
- W4387013459 hasRelatedWork W1998992221 @default.
- W4387013459 hasRelatedWork W2021205638 @default.
- W4387013459 hasRelatedWork W2073458141 @default.
- W4387013459 hasRelatedWork W2082149885 @default.
- W4387013459 hasRelatedWork W2173869177 @default.
- W4387013459 hasRelatedWork W2356933146 @default.
- W4387013459 hasRelatedWork W3160306610 @default.
- W4387013459 hasRelatedWork W569423035 @default.
- W4387013459 hasVolume "2586" @default.
- W4387013459 isParatext "false" @default.
- W4387013459 isRetracted "false" @default.
- W4387013459 workType "article" @default.