Non-yrast states and shape co-existence in <sup>172</sup>Os

dc.contributor.authorDavidson, P. M.en
dc.contributor.authorDracoulis, G. D.en
dc.contributor.authorKibédi, T.en
dc.contributor.authorByrne, A. P.en
dc.contributor.authorAnderssen, S. S.en
dc.contributor.authorBaxter, A. M.en
dc.contributor.authorFabricius, B.en
dc.contributor.authorLane, G. J.en
dc.contributor.authorStuchbery, A. E.en
dc.date.accessioned2025-12-31T19:41:11Z
dc.date.available2025-12-31T19:41:11Z
dc.date.issued1994-02-07en
dc.description.abstractPrevious studies of 172Os noted an anomaly in the behaviour of the moment of inertia of the yrast band at low spin. A phenomenological model of shape coexistence based on interacting rotational bands was proposed to explain this anomaly and this model predicted low-lying non-yrast states. In order to test these predictions, the β-decay of 172Ir has been used to populate 172Os. Excited states have been observed and classified into positive-parity "quasi-β" and "quasi-γ" bands and a negative-parity band. The energies of the quasi-β band states are seen to be in general agreement with the predictions of the phenomenological model and the model is refined to take into account the new data. The bands involved are determined to have significantly different moments of inertia.en
dc.description.statusPeer-revieweden
dc.format.extent17en
dc.identifier.issn0375-9474en
dc.identifier.otherORCID:/0000-0002-9205-7500/work/165612946en
dc.identifier.otherORCID:/0000-0002-0198-9901/work/165613733en
dc.identifier.scopus0001956254en
dc.identifier.urihttps://hdl.handle.net/1885/733798027
dc.language.isoenen
dc.sourceNuclear Physics, Section Aen
dc.subjectNuclear structureen
dc.titleNon-yrast states and shape co-existence in <sup>172</sup>Osen
dc.typeJournal articleen
dspace.entity.typePublicationen
local.bibliographicCitation.lastpage106en
local.bibliographicCitation.startpage90en
local.contributor.affiliationDavidson, P. M.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationDracoulis, G. D.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationKibédi, T.; Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationByrne, A. P.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationAnderssen, S. S.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationBaxter, A. M.; Quantum Science, Department of Quantum Science & Technology, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationFabricius, B.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationLane, G. J.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationStuchbery, A. E.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.identifier.citationvolume568en
local.identifier.doi10.1016/0375-9474(94)90005-1en
local.identifier.pure14d4bac0-92d6-4899-b62e-84b1a0444df3en
local.identifier.urlhttps://www.scopus.com/pages/publications/0001956254en
local.type.statusPublisheden

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