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dc.contributor.authorR. J. Carrollen_US
dc.contributor.authorZs Podolyáken_US
dc.contributor.authorT. Berryen_US
dc.contributor.authorH. Graween_US
dc.contributor.authorT. Alexanderen_US
dc.contributor.authorA. N. Andreyeven_US
dc.contributor.authorS. Ansarien_US
dc.contributor.authorM. J.G. Borgeen_US
dc.contributor.authorM. Bruneten_US
dc.contributor.authorJ. R. Creswellen_US
dc.contributor.authorL. M. Fraileen_US
dc.contributor.authorC. Fahlanderen_US
dc.contributor.authorH. O.U. Fynboen_US
dc.contributor.authorE. R. Gambaen_US
dc.contributor.authorW. Gelletlyen_US
dc.contributor.authorR. B. Gersten_US
dc.contributor.authorM. Górskaen_US
dc.contributor.authorA. Gredleyen_US
dc.contributor.authorP. T. Greenleesen_US
dc.contributor.authorL. J. Harkness-Brennanen_US
dc.contributor.authorM. Huyseen_US
dc.contributor.authorS. M. Judgeen_US
dc.contributor.authorD. S. Judsonen_US
dc.contributor.authorJ. Konkien_US
dc.contributor.authorJ. Kurcewiczen_US
dc.contributor.authorI. Kutien_US
dc.contributor.authorS. Lalkovskien_US
dc.contributor.authorI. H. Lazarusen_US
dc.contributor.authorR. Licǎen_US
dc.contributor.authorM. Lunden_US
dc.contributor.authorM. Madurgaen_US
dc.contributor.authorN. Margineanen_US
dc.contributor.authorR. Margineanen_US
dc.contributor.authorI. Marroquinen_US
dc.contributor.authorC. Mihaien_US
dc.contributor.authorR. E. Mihaien_US
dc.contributor.authorE. Nácheren_US
dc.contributor.authorA. Negreten_US
dc.contributor.authorC. Nitaen_US
dc.contributor.authorS. Pascuen_US
dc.contributor.authorR. D. Pageen_US
dc.contributor.authorZ. Patelen_US
dc.contributor.authorA. Pereaen_US
dc.contributor.authorJ. Phrompaoen_US
dc.contributor.authorM. Piersaen_US
dc.contributor.authorV. Pucknellen_US
dc.contributor.authorP. Rahkilaen_US
dc.contributor.authorE. Rapisardaen_US
dc.contributor.authorP. H. Reganen_US
dc.contributor.authorF. Rotaruen_US
dc.contributor.authorM. Rudigieren_US
dc.contributor.authorC. M. Shanden_US
dc.contributor.authorR. Shearmanen_US
dc.contributor.authorS. Stegemannen_US
dc.contributor.authorT. Storaen_US
dc.contributor.authorCh Sottyen_US
dc.contributor.authorO. Tengbladen_US
dc.contributor.authorP. Van Duppenen_US
dc.contributor.authorV. Vediaen_US
dc.contributor.authorR. Wadsworthen_US
dc.contributor.authorP. M. Walkeren_US
dc.contributor.authorN. Warren_US
dc.contributor.authorF. Wearingen_US
dc.contributor.authorH. De Witteen_US
dc.date.accessioned2021-01-27T04:02:33Z-
dc.date.available2021-01-27T04:02:33Z-
dc.date.issued2020-11-02en_US
dc.identifier.issn10797114en_US
dc.identifier.issn00319007en_US
dc.identifier.other2-s2.0-85096099077en_US
dc.identifier.other10.1103/PhysRevLett.125.192501en_US
dc.identifier.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=85096099077&origin=inwarden_US
dc.identifier.urihttp://cmuir.cmu.ac.th/jspui/handle/6653943832/71664-
dc.description.abstract© 2020 authors. Published by the American Physical Society. Published by the American Physical Society under the terms of the "https://creativecommons.org/licenses/by/4.0/"Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. The β decay of Hg208 into the one-proton hole, one neutron-particle Tl81208127 nucleus was investigated at CERN-ISOLDE. Shell-model calculations describe well the level scheme deduced, validating the proton-neutron interactions used, with implications for the whole of the N>126, Z<82 quadrant of neutron-rich nuclei. While both negative and positive parity states with spin 0 and 1 are expected within the Qβ window, only three negative parity states are populated directly in the β decay. The data provide a unique test of the competition between allowed Gamow-Teller and Fermi, and first-forbidden β decays, essential for the understanding of the nucleosynthesis of heavy nuclei in the rapid neutron capture process. Furthermore, the observation of the parity changing 0+→0-β decay where the daughter state is core excited is unique, and can provide information on mesonic corrections of effective operators.en_US
dc.subjectPhysics and Astronomyen_US
dc.titleCompetition between Allowed and First-Forbidden β Decay: The Case of Hg 208 → Tl 208en_US
dc.typeJournalen_US
article.title.sourcetitlePhysical Review Lettersen_US
article.volume125en_US
article.stream.affiliationsDepartement Natuurkunde en Sterrenkundeen_US
article.stream.affiliationsUniversity of Jyvaskylaen_US
article.stream.affiliationsAarhus Universiteten_US
article.stream.affiliationsLunds Universiteten_US
article.stream.affiliationsUniversidad Complutense de Madriden_US
article.stream.affiliationsUniversity of Cologneen_US
article.stream.affiliationsUniversity of Surreyen_US
article.stream.affiliationsUniversity of Liverpoolen_US
article.stream.affiliationsEuropean Organization for Nuclear Researchen_US
article.stream.affiliationsUniversity of Yorken_US
article.stream.affiliationsJapan Atomic Energy Agencyen_US
article.stream.affiliationsThe University of Tennessee, Knoxvilleen_US
article.stream.affiliationsUniversity of Warsawen_US
article.stream.affiliationsNational Physical Laboratoryen_US
article.stream.affiliationsGSI Helmholtz Centre for Heavy Ion Research GmbHen_US
article.stream.affiliationsUniversity of Brightonen_US
article.stream.affiliationsHoria Hulubei National Institute of Physics and Nuclear Engineeringen_US
article.stream.affiliationsDaresbury Laboratoryen_US
article.stream.affiliationsHelsingin Yliopistoen_US
article.stream.affiliationsAtommagkutató Intézeten_US
article.stream.affiliationsChiang Mai Universityen_US
article.stream.affiliationsCSIC - Instituto de Estructura de la Materia (IEM)en_US
Appears in Collections:CMUL: Journal Articles

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