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dc.contributor.authorSpagnoletti, P.
dc.contributor.authorButler, P. A.
dc.contributor.authorGaffney, L. P.
dc.contributor.authorAbrahams, K.
dc.contributor.authorBowry, M.
dc.contributor.authorCederkäll, J.
dc.contributor.authorChupp, T.
dc.contributor.authorde Angelis, G.
dc.contributor.authorDe Witte, H.
dc.contributor.authorGarrett, P. E.
dc.contributor.authorGoldkuhle, A.
dc.contributor.authorHenrich, C.
dc.contributor.authorIllana, A.
dc.contributor.authorJohnston, K.
dc.contributor.authorJoss, D. T.
dc.contributor.authorKeatings, J. M.
dc.contributor.authorKelly, N. A.
dc.contributor.authorKomorowska, M.
dc.contributor.authorKonki, J.
dc.contributor.authorKröll, T.
dc.contributor.authorLozano, M.
dc.contributor.authorSingh, B. S. Nara
dc.contributor.authorO'Donnell, D.
dc.contributor.authorOjala, J.
dc.contributor.authorPage, R. D.
dc.contributor.authorPedersen, L. G.
dc.contributor.authorRaison, C.
dc.contributor.authorReiter, P.
dc.contributor.authorRodriguez, J. A.
dc.contributor.authorRosiak, D.
dc.contributor.authorRothe, S.
dc.contributor.authorScheck, M.
dc.contributor.authorSeidlitz, M.
dc.contributor.authorShneidman, T. M.
dc.contributor.authorSiebeck, B.
dc.contributor.authorSinclair, J.
dc.contributor.authorSmith, J. F.
dc.contributor.authorStryjczyk, M.
dc.contributor.authorVan Duppen, P.
dc.contributor.authorViñals, S.
dc.contributor.authorVirtanen, V.
dc.contributor.authorWrzosek-Lipska, K.
dc.contributor.authorWarr, N.
dc.contributor.authorZielińska, M.
dc.date.accessioned2022-03-01T10:59:40Z
dc.date.available2022-03-01T10:59:40Z
dc.date.issued2022
dc.identifier.citationSpagnoletti, P., Butler, P. A., Gaffney, L. P., Abrahams, K., Bowry, M., Cederkäll, J., Chupp, T., de Angelis, G., De Witte, H., Garrett, P. E., Goldkuhle, A., Henrich, C., Illana, A., Johnston, K., Joss, D. T., Keatings, J. M., Kelly, N. A., Komorowska, M., Konki, J., . . . Zielińska, M. (2022). Coulomb excitation of 222Rn. <i>Physical Review C</i>, <i>105</i>(2), Article 024323. <a href="https://doi.org/10.1103/PhysRevC.105.024323" target="_blank">https://doi.org/10.1103/PhysRevC.105.024323</a>
dc.identifier.otherCONVID_104444529
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/80026
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 2360−210+300efm3 and 2300−500+300efm3 while a smaller value, 1200−900+500efm3, was found for the 2+→1− transition. In addition, four excited non-yrast states were identified in this work via γ−γ coincidences.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society (APS)
dc.relation.ispartofseriesPhysical Review C
dc.rightsCC BY 4.0
dc.subject.otherelectromagnetic transitions
dc.subject.othernuclear structure & decays
dc.subject.otherA ≥ 220
dc.titleCoulomb excitation of 222Rn
dc.typeresearch article
dc.identifier.urnURN:NBN:fi:jyu-202203011744
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.numberinseries2
dc.relation.volume105
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2022
dc.rights.accesslevelopenAccessfi
dc.type.publicationarticle
dc.relation.grantnumber654002
dc.relation.grantnumber654002
dc.relation.grantnumber771036
dc.relation.grantnumber771036
dc.relation.grantnumber307685
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/654002/EU//
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/771036/EU//MAIDEN
dc.subject.ysoydinfysiikka
dc.subject.ysoradon
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p14759
jyx.subject.urihttp://www.yso.fi/onto/yso/p6953
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevC.105.024323
dc.relation.funderEuropean Commissionen
dc.relation.funderEuropean Commissionen
dc.relation.funderResearch Council of Finlanden
dc.relation.funderEuroopan komissiofi
dc.relation.funderEuroopan komissiofi
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramResearch infrastructures, H2020en
jyx.fundingprogramERC Consolidator Granten
jyx.fundingprogramAcademy Project, AoFen
jyx.fundingprogramResearch infrastructures, H2020fi
jyx.fundingprogramERC Consolidator Grantfi
jyx.fundingprogramAkatemiahanke, SAfi
jyx.fundinginformationThis work was supported by the following Research Councils and Grants: Science and Technology Facilities Council (STFC; UK) Grants No. ST/P004598/1, No. ST/L005808/1, and No. ST/R004056/1; Federal Ministry of Education and Research (BMBF; Germany) Grants No. 05P18RDCIA, No. 05P15PKCIA, and No. 05P18PKCIA and the “Verbundprojekt 05P2018”; National Science Centre (Poland) Grant No. 2015/18/M/ST2/00523; European Union's Horizon 2020 Framework research and innovation programme 654002 (ENSAR2) and 771036 (ERC CoG MAIDEN); Marie Skłodowska-Curie Actions COFUND grant (EU-CERN) 665779; Research Foundation Flanders (FWO, Belgium), by GOA/2015/010 (BOF KU Leuven) and the Interuniversity Attraction Poles Programme initiated by the Belgian Science Policy Office (BriX network P7/12); Russian Foundation for Basic Research Grant No. 17-52-12015; Academy of Finland Grant No. 307685.
dc.type.okmA1


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