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dc.contributor.authorKumar, Anil
dc.contributor.authorSrivastava, Praveen C.
dc.contributor.authorKostensalo, Joel
dc.contributor.authorSuhonen, Jouni
dc.date.accessioned2020-06-12T06:25:57Z
dc.date.available2020-06-12T06:25:57Z
dc.date.issued2020
dc.identifier.citationKumar, A., Srivastava, P. C., Kostensalo, J., & Suhonen, J. (2020). Second-forbidden nonunique β− decays of 24Na and 36Cl assessed by the nuclear shell model. <i>Physical Review C</i>, <i>101</i>(6), Article 064304. <a href="https://doi.org/10.1103/PhysRevC.101.064304" target="_blank">https://doi.org/10.1103/PhysRevC.101.064304</a>
dc.identifier.otherCONVID_35916876
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/69895
dc.description.abstractWe have performed a systematic study of the log f t values, shape factors, and electron spectra for the second-forbidden nonunique β− decays of 24Na(4+) →24Mg(2+) and 36Cl(2+) →36Ar(0+) transitions under the framework of the nuclear shell model. We have performed the shell model calculations in the sd model space, using more recent microscopic effective interactions such as Daejeon16, chiral N3LO, and JISP16. These interactions are derived from the no-core shell model wave functions using Okubo-Lee-Suzuki transformation. For comparison, we have also shown the results obtain from the phenomenological USDB interaction. To test the predictive power of these interactions first we have computed low-lying energy spectra of parent and daughter nuclei involved in these transitions. The computed results for energy spectra, nuclear matrix elements, log f t values, shape factors, electron spectra, and decomposition of the integrated shape factor are reported and compare with the available experimental data.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review C
dc.rightsIn Copyright
dc.subject.otherbeta decay
dc.subject.othernuclear structure and decays
dc.titleSecond-forbidden nonunique β− decays of 24Na and 36Cl assessed by the nuclear shell model
dc.typeresearch article
dc.identifier.urnURN:NBN:fi:jyu-202006124140
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.issn2469-9985
dc.relation.numberinseries6
dc.relation.volume101
dc.type.versionpublishedVersion
dc.rights.copyright© 2020 American Physical Society
dc.rights.accesslevelopenAccessfi
dc.type.publicationarticle
dc.subject.ysoydinfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p14759
dc.rights.urlhttp://rightsstatements.org/page/InC/1.0/?language=en
dc.relation.doi10.1103/PhysRevC.101.064304
jyx.fundinginformationA.K. would like to thank the Ministry of Human Resource Development (MHRD), Government of India, for financial support for his thesis work. P.C.S. acknowledges a research grant from SERB (India), CRG/2019/000556. We would like to thank X. Mougeot for providing the experimental shape factor data of 36Cl.
dc.type.okmA1


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