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dc.contributor.authorBonnard, J.
dc.contributor.authorDobaczewski, J.
dc.contributor.authorDanneaux, G.
dc.contributor.authorKortelainen, M.
dc.date.accessioned2023-07-05T05:54:46Z
dc.date.available2023-07-05T05:54:46Z
dc.date.issued2023
dc.identifier.citationBonnard, J., Dobaczewski, J., Danneaux, G., & Kortelainen, M. (2023). Nuclear DFT electromagnetic moments in heavy deformed open-shell odd nuclei. <i>Physics Letters B</i>, <i>843</i>, Article 138014. <a href="https://doi.org/10.1016/j.physletb.2023.138014" target="_blank">https://doi.org/10.1016/j.physletb.2023.138014</a>
dc.identifier.otherCONVID_183620548
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/88233
dc.description.abstractWithin the nuclear DFT approach, we determined the magnetic dipole and electric quadrupole moments for paired nuclear states corresponding to the proton (neutron) quasiparticles blocked in the π11/2− (ν13/2+) intruder configurations. We performed calculations for all deformed open-shell odd nuclei with 63 ≤ Z ≤ 82 and 82 ≤ N ≤ 126. Time-reversal symmetry was broken in the intrinsic reference frame and self-consistent shape and spin core polarizations were established. We determined spectroscopic moments of angular-momentum-projected wave functions and compared them with available experimental data. We obtained good agreement with data without using effective g-factors or effective charges in the dipole or quadrupole operators, respectively. We also showed that the intrinsic magnetic dipole moments, or those obtained for conserved intrinsic time-reversal symmetry, do not represent viable approximations of the spectroscopic ones.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherElsevier BV
dc.relation.ispartofseriesPhysics Letters B
dc.rightsCC BY 4.0
dc.subject.othermean field
dc.subject.otherelectromagnetic moments
dc.subject.othersymmetry restoration
dc.titleNuclear DFT electromagnetic moments in heavy deformed open-shell odd nuclei
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202307054372
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn0370-2693
dc.relation.volume843
dc.type.versionpublishedVersion
dc.rights.copyright© 2023 The Author(s). Published by Elsevier B.V. Funded by SCOAP3.
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber339243
dc.subject.ysoydinfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p14759
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.datasethttps://webfiles.york.ac.uk/HFODD/Projects/GadLead/
dc.relation.doi10.1016/j.physletb.2023.138014
dc.relation.funderResearch Council of Finlanden
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundinginformationThis work was partially supported by the STFC Grant Nos. ST/P003885/1 and ST/V001035/1, by the Polish National Science Centre under Contract No. 2018/31/B/ST2/02220, by a Leverhulme Trust Research Project Grant, and by the Academy of Finland under the Academy Project No. 339243. We acknowledge the CSC-IT Center for Science Ltd., Finland, for the allocation of computational resources. This project was partly undertaken on the Viking Cluster, which is a high performance compute facility provided by the University of York. We are grateful for computational support from the University of York High Performance Computing service, Viking and the Research Computing team.
dc.type.okmA1


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