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dc.contributor.authorKurpeta, J.
dc.contributor.authorUrban, W.
dc.contributor.authorPlochocki, A.
dc.contributor.authorRzaca-Urban, T.
dc.contributor.authorSmith, A. G.
dc.contributor.authorSmith, J. F.
dc.contributor.authorSimpson, G. S.
dc.contributor.authorAhmad, I.
dc.contributor.authorGreene, J. P.
dc.contributor.authorJokinen, Ari
dc.contributor.authorPenttilä, Heikki
dc.date.accessioned2016-02-09T09:14:53Z
dc.date.available2016-02-09T09:14:53Z
dc.date.issued2014
dc.identifier.citationKurpeta, J., Urban, W., Plochocki, A., Rzaca-Urban, T., Smith, A. G., Smith, J. F., Simpson, G. S., Ahmad, I., Greene, J. P., Jokinen, A., & Penttilä, H. (2014). Neutron configurations in 113Pd. <i>Physical Review C</i>, <i>90</i>(6), Article 064315. <a href="https://doi.org/10.1103/PhysRevC.90.064315" target="_blank">https://doi.org/10.1103/PhysRevC.90.064315</a>
dc.identifier.otherCONVID_24448755
dc.identifier.otherTUTKAID_64620
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/48697
dc.description.abstractExcited states in 113Pd, populated in β− decay of 113Rh and in spontaneous fission of 248Cm and 252Cf, have been studied by means of γ spectroscopy at the IGISOL facility of Jyvaskylä University and using large arrays of Ge detectors (Eurogam2 and Gammasphere, respectively). The position of the 11/2− yrast excitation in 113Pd, proposed recently at 166.1 keV by other authors, has been corrected to 98.9 keV. The decay of this level has been discussed to explain the observed transition intensities. The 7/2− member of the yrast, unique-parity configuration has been identified at 84.9 keV and a band on top of this level proposed. On top of the 1/2+, first excited state a band has been built and a new 3/2+ bandhead has been proposed at 151.9 keV. A possible oblate-shape origin of these low-energy bandsheads has been discussed.
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review C
dc.subject.otherisotopes of palladium
dc.titleNeutron configurations in 113Pd
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201602031408
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineFysiikkafi
dc.contributor.oppiaineKiihdytinlaboratoriofi
dc.contributor.oppiainePhysicsen
dc.contributor.oppiaineAccelerator Laboratoryen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.date.updated2016-02-03T07:15:20Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn0556-2813
dc.relation.numberinseries6
dc.relation.volume90
dc.type.versionpublishedVersion
dc.rights.copyright© 2014 American Physical Society. Published in this repository with the kind permission of the publisher.
dc.rights.accesslevelopenAccessfi
dc.relation.doi10.1103/PhysRevC.90.064315
dc.type.okmA1


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