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dc.contributor.authorBerry, T. A.
dc.contributor.authorPodolyák, Zs.
dc.contributor.authorCarroll, R. J.
dc.contributor.authorLica, R.
dc.contributor.authorBrown, B. A.
dc.contributor.authorGrawe, H.
dc.contributor.authorSotty, Ch.
dc.contributor.authorTimofeyuk, N. K.
dc.contributor.authorAlexander, T.
dc.contributor.authorAndreyev, A. N.
dc.contributor.authorAnsari, S.
dc.contributor.authorBorge, M. J. G.
dc.contributor.authorBrunet, M.
dc.contributor.authorCresswell, J. R.
dc.contributor.authorFahlander, C.
dc.contributor.authorFraile, L. M.
dc.contributor.authorFynbo, H. O. U.
dc.contributor.authorGamba, E.
dc.contributor.authorGelletly, W.
dc.contributor.authorGerst, R.-B.
dc.contributor.authorGórska, M.
dc.contributor.authorGredley, A.
dc.contributor.authorGreenlees, P.
dc.contributor.authorHarkness-Brennan, L. J.
dc.contributor.authorHuyse, M.
dc.contributor.authorJudge, S. M.
dc.contributor.authorJudson, D. S.
dc.contributor.authorKonki, J.
dc.contributor.authorKowalska, M.
dc.contributor.authorKurcewicz, J.
dc.contributor.authorKuti, I.
dc.contributor.authorLalkovski, S.
dc.contributor.authorLazarus, I.
dc.contributor.authorLund, M.
dc.contributor.authorMadurga, M.
dc.contributor.authorMarginean, N.
dc.contributor.authorMarginean, R.
dc.contributor.authorMarroquin, I.
dc.contributor.authorMihai, C.
dc.contributor.authorMihai, R. E.
dc.contributor.authorNácher, E.
dc.contributor.authorNegret, A.
dc.contributor.authorNae, S.
dc.contributor.authorNita, C.
dc.contributor.authorPascu, S.
dc.contributor.authorPage, R. D.
dc.contributor.authorPatel, Z.
dc.contributor.authorPerea, A.
dc.contributor.authorPhrompao, J.
dc.contributor.authorPiersa, M.
dc.contributor.authorPucknell, V.
dc.contributor.authorRahkila, P.
dc.contributor.authorRapisarda, E.
dc.contributor.authorRegan, P. H.
dc.contributor.authorRotaru, F.
dc.contributor.authorRudigier, M.
dc.contributor.authorShand, C. M.
dc.contributor.authorShearman, R.
dc.contributor.authorSimpson, E. C.
dc.contributor.authorStegemann, S.
dc.contributor.authorStora, T.
dc.contributor.authorTengblad, O.
dc.contributor.authorTurturica, A.
dc.contributor.authorVan Duppen, P.
dc.contributor.authorVedia, V.
dc.contributor.authorWalker, P. M.
dc.contributor.authorWarr, N.
dc.contributor.authorWearing, F. P.
dc.contributor.authorDe Witte, H.
dc.date.accessioned2020-05-20T11:24:26Z
dc.date.available2020-05-20T11:24:26Z
dc.date.issued2020
dc.identifier.citationBerry, T. A., Podolyák, Zs., Carroll, R. J., Lica, R., Brown, B. A., Grawe, H., Sotty, Ch., Timofeyuk, N. K., Alexander, T., Andreyev, A. N., Ansari, S., Borge, M. J. G., Brunet, M., Cresswell, J. R., Fahlander, C., Fraile, L. M., Fynbo, H. O. U., Gamba, E., Gelletly, W., . . . De Witte, H. (2020). Octupole states in 207Tl studied through β decay. <i>Physical Review C</i>, <i>101</i>(5), Article 054311. <a href="https://doi.org/10.1103/PhysRevC.101.054311" target="_blank">https://doi.org/10.1103/PhysRevC.101.054311</a>
dc.identifier.otherCONVID_35688927
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/69111
dc.description.abstractThe β decay of 207Hg into the single-proton-hole nucleus 207Tl has been studied through γ-ray spectroscopy at the ISOLDE Decay Station (IDS) with the aim of identifying states resulting from coupling of the πs−11/2, πd−13/2, and πh−111/2 shell model orbitals to the collective octupole vibration. Twenty-two states were observed lying between 2.6 and 4.0 MeV, eleven of which were observed for the first time, and 78 new transitions were placed. Two octupole states (s1/2-coupled) are identified and three more states (d3/2-coupled) are tentatively assigned using spin-parity inferences, while further h11/2-coupled states may also have been observed for the first time. Comparisons are made with state-of-the-art large-scale shell model calculations and previous observations made in this region, and systematic underestimation of the energy of the octupole vibrational states is noted. We suggest that in order to resolve the difference in predicted energies for collective and noncollective t=1 states (t is the number of nucleons breaking the 208Pb core), the effect of t=2 mixing may be reduced for octupole-coupled states. The inclusion of mixing with t=0,2,3 excitations is necessary to replicate all t=1 state energies accurately.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review C
dc.rightsCC BY 4.0
dc.subject.otherbeta decay
dc.subject.othercollective levels
dc.subject.othernuclear structure and decays
dc.subject.othernucleon distribution
dc.titleOctupole states in 207Tl studied through β decay
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202005203364
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineYdin- ja kiihdytinfysiikan huippuyksikköfi
dc.contributor.oppiaineFysiikkafi
dc.contributor.oppiaineKiihdytinlaboratoriofi
dc.contributor.oppiaineCentre of Excellence in Nuclear and Accelerator Based Physicsen
dc.contributor.oppiainePhysicsen
dc.contributor.oppiaineAccelerator Laboratoryen
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.numberinseries5
dc.relation.volume101
dc.type.versionpublishedVersion
dc.rights.copyright© Authors, 2020
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber654002
dc.relation.grantnumber654002
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/654002/EU//
dc.subject.ysoydinfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p14759
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevC.101.054311
dc.relation.funderEuropean Commissionen
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramResearch infrastructures, H2020en
jyx.fundingprogramResearch infrastructures, H2020fi
jyx.fundinginformationThe research leading to these results has received funding from the European Union’s Horizon 2020 Research and Innovation Programme under Grant Agreement No. 654002. Support from the European Union Seventh Framework through ENSAR Contract No. 262010, the Science and Technology Facilities Council (UK), the MINECO Projects No. FPA2015-64969-P and No. FPA2017-87568-P (Spain), FWOVlaanderen (Belgium), GOA/2015/010 (BOF KU Leuven), the Excellence of Science Programme (EOS-FWO), the Interuniversity Attraction Poles Programme initiated by the Belgian Science Policy Office (BriX network P7/12), the German BMBF under Contract No. 05P18PKCIA + “Verbundprojekt 05P2018,” the Polish National Science Centre under Contracts No. UMO-2015/18/M/ST2/00523 and No. UMO-2019/33/N/ST2/03023, the National Science Foundation (US) Grant No. PHY-1811855 and the Romanian IFA project CERN-RO/ISOLDE is acknowledged. P.H.R. and S.M.J. acknowledge support from the UK Department for Business, Energy and Industrial Strategy via the National Measurement Office.
dc.type.okmA1


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