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dc.date.accessioned2023-03-04T16:18:00Z
dc.date.available2023-03-04T16:18:00Z
dc.date.created2022-06-02T12:40:36Z
dc.date.issued2022
dc.identifier.citationButler, P.A. Gaffney, L.P. Abrahams, K. Bowry, M. Cederkäll, J. Chupp, T. De Angelis, Angelis De Witte, Witte Garrett, P.E. Goldkuhle, A. Henrich, C. Illana, A. Johnston, K. Joss, D.T. Keatings, J.M. Kelly, N.A. Komorowska, M. Konki, J. Kröll, T. Lozano, M. Singh, B. S. Nara O'Donnell, D. Ojala, J. Page, R.D. Pedersen, Line Gaard Raison, C. Reiter, P. Rodriguez, J.A. Rosiak, D. Rothe, S. Scheck, M. Seidlitz, M. Shneidman, T.M. Siebeck, B. Sinclair, J. Smith, J.F. Stryjczyk, M. Van Duppen, Duppen Viñals, S. Virtanen, V. Wrzosek-Lipska, K. Warr, N. Zielińska, M. . Coulomb excitation of Rn 222. Physical Review C. 2022, 105(2)
dc.identifier.urihttp://hdl.handle.net/10852/100836
dc.description.abstractThe nature of quadrupole and octupole collectivity in 222Rn was investigated by determining the electric-quadrupole (E2) and octupole (E3) matrix elements using subbarrier, multistep Coulomb excitation. The radioactive 222Rn beam, accelerated to 4.23 MeV/u, was provided by the HIE-ISOLDE facility at CERN. Data were collected in the Miniball γ-ray spectrometer following the bombardment of two targets, 120Sn and 60Ni. Transition E2 matrix elements within the ground-state and octupole bands were measured up to 10ℏ and the results were consistent with a constant intrinsic electric-quadrupole moment, 518(11)efm2. The values of the intrinsic electric-octupole moment for the 0+→3− and 2+→5− transitions were found to be respectively 2360+300−210efm3 and 2300+300−500efm3 while a smaller value, 1200+500−900efm3, was found for the 2+→1− transition. In addition, four excited non-yrast states were identified in this work via γ−γ coincidences.
dc.languageEN
dc.publisherAmerican Physical Society
dc.rightsAttribution 4.0 International
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.titleCoulomb excitation of Rn 222
dc.title.alternativeENEngelskEnglishCoulomb excitation of Rn 222
dc.typeJournal article
dc.creator.authorButler, P.A.
dc.creator.authorGaffney, L.P.
dc.creator.authorAbrahams, K.
dc.creator.authorBowry, M.
dc.creator.authorCederkäll, J.
dc.creator.authorChupp, T.
dc.creator.authorDe Angelis, Angelis
dc.creator.authorDe Witte, Witte
dc.creator.authorGarrett, P.E.
dc.creator.authorGoldkuhle, A.
dc.creator.authorHenrich, C.
dc.creator.authorIllana, A.
dc.creator.authorJohnston, K.
dc.creator.authorJoss, D.T.
dc.creator.authorKeatings, J.M.
dc.creator.authorKelly, N.A.
dc.creator.authorKomorowska, M.
dc.creator.authorKonki, J.
dc.creator.authorKröll, T.
dc.creator.authorLozano, M.
dc.creator.authorSingh, B. S. Nara
dc.creator.authorO'Donnell, D.
dc.creator.authorOjala, J.
dc.creator.authorPage, R.D.
dc.creator.authorPedersen, Line Gaard
dc.creator.authorRaison, C.
dc.creator.authorReiter, P.
dc.creator.authorRodriguez, J.A.
dc.creator.authorRosiak, D.
dc.creator.authorRothe, S.
dc.creator.authorScheck, M.
dc.creator.authorSeidlitz, M.
dc.creator.authorShneidman, T.M.
dc.creator.authorSiebeck, B.
dc.creator.authorSinclair, J.
dc.creator.authorSmith, J.F.
dc.creator.authorStryjczyk, M.
dc.creator.authorVan Duppen, Duppen
dc.creator.authorViñals, S.
dc.creator.authorVirtanen, V.
dc.creator.authorWrzosek-Lipska, K.
dc.creator.authorWarr, N.
dc.creator.authorZielińska, M.
cristin.unitcode185,15,4,0
cristin.unitnameFysisk institutt
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode1
dc.identifier.cristin2029046
dc.identifier.bibliographiccitationinfo:ofi/fmt:kev:mtx:ctx&ctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.jtitle=Physical Review C&rft.volume=105&rft.spage=&rft.date=2022
dc.identifier.jtitlePhysical Review C
dc.identifier.volume105
dc.identifier.issue2
dc.identifier.pagecount0
dc.identifier.doihttps://doi.org/10.1103/PhysRevC.105.024323
dc.type.documentTidsskriftartikkel
dc.type.peerreviewedPeer reviewed
dc.source.issn2469-9985
dc.type.versionPublishedVersion
cristin.articleid024323


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