Näytä suppeat kuvailutiedot

dc.contributor.authorAhlgren Cederlöf, E.
dc.contributor.authorBäck, T.
dc.contributor.authorNyberg, J.
dc.contributor.authorQi, C.
dc.contributor.authorAtaç, A.
dc.contributor.authorBadran, H.
dc.contributor.authorBraunroth, T.
dc.contributor.authorCalverley, T.
dc.contributor.authorCox, D. M.
dc.contributor.authorDoncel, M.
dc.contributor.authorGrahn, T.
dc.contributor.authorGreenlees, P.
dc.contributor.authorHilton, J.
dc.contributor.authorJulin, R.
dc.contributor.authorJuutinen, S.
dc.contributor.authorKonki, J.
dc.contributor.authorLi, H.
dc.contributor.authorMatta, S.
dc.contributor.authorModamio, V.
dc.contributor.authorNara Singh, B. S.
dc.contributor.authorPakarinen, J.
dc.contributor.authorPapadakis, P.
dc.contributor.authorPartanen, J.
dc.contributor.authorRahkila, P.
dc.contributor.authorRuotsalainen, P.
dc.contributor.authorSandzelius, M.
dc.contributor.authorSarén, J.
dc.contributor.authorScholey, C.
dc.contributor.authorStolze, S.
dc.contributor.authorSubramaniam, P.
dc.contributor.authorUusitalo, J.
dc.contributor.authorValiente-Dobón, J. J.
dc.date.accessioned2024-01-24T12:21:20Z
dc.date.available2024-01-24T12:21:20Z
dc.date.issued2023
dc.identifier.citationAhlgren Cederlöf, E., Bäck, T., Nyberg, J., Qi, C., Ataç, A., Badran, H., Braunroth, T., Calverley, T., Cox, D. M., Doncel, M., Grahn, T., Greenlees, P., Hilton, J., Julin, R., Juutinen, S., Konki, J., Li, H., Matta, S., Modamio, V., . . . Valiente-Dobón, J.J. (2023). Lifetime measurement of the yrast 2+ state in 118Te. <i>European Physical Journal A</i>, <i>59</i>, Article 300. <a href="https://doi.org/10.1140/epja/s10050-023-01212-3" target="_blank">https://doi.org/10.1140/epja/s10050-023-01212-3</a>
dc.identifier.otherCONVID_201934639
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/93027
dc.description.abstractThe electromagnetic transition probabilities of the yrast 2+ states in the midshell Te isotopes, two protons above the closed shell at Sn, are of great importance for the understanding of nuclear collectivity in these isotopes and the role played by the neutron-proton interactions and crossshell excitations. However, the large uncertainty of the experimental data for the midshell nucleus 118Te and the missing data for 116Te make it difficult to pin down the general trend of the evolution of transition probabilities as a function of the neutron number. In this work, the lifetime of the yrast 2+ state in 118Te was measured, with the aim of reducing the uncertainty of the previous measurement. The result is τ2+ = 7.46(19) ps. In addition, the lifetime of the 4+ state was measured to be τ4+ = 4.25(23) ps. The experimental transition rates are extracted from the measured lifetimes and compared with systematic large-scale shell-model calculations. The trend of the B(E2; 0+ → 2+) values in the midshell area is in good agreement with the calculations and the calculated B4/2 ratio provide evidence for 118Te as a near perfect harmonic vibrator.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherSpringer
dc.relation.ispartofseriesEuropean Physical Journal A
dc.rightsCC BY 4.0
dc.titleLifetime measurement of the yrast 2+ state in 118Te
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-202401241517
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineFysiikkafi
dc.contributor.oppiaineYdin- ja kiihdytinfysiikan huippuyksikköfi
dc.contributor.oppiaineKiihdytinlaboratoriofi
dc.contributor.oppiainePhysicsen
dc.contributor.oppiaineCentre of Excellence in Nuclear and Accelerator Based Physicsen
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.issn1434-6001
dc.relation.volume59
dc.type.versionpublishedVersion
dc.rights.copyright© The Author(s) 2023
dc.rights.accesslevelopenAccessfi
dc.relation.grantnumber654002
dc.relation.grantnumber654002
dc.relation.projectidinfo:eu-repo/grantAgreement/EC/H2020/654002/EU//
dc.subject.ysoydinfysiikka
dc.subject.ysotelluuri
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p14759
jyx.subject.urihttp://www.yso.fi/onto/yso/p22857
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1140/epja/s10050-023-01212-3
dc.relation.funderEuropean Commissionen
dc.relation.funderEuroopan komissiofi
jyx.fundingprogramResearch infrastructures, H2020en
jyx.fundingprogramResearch infrastructures, H2020fi
jyx.fundinginformationThis work was supported by the UKRI STFC, through Grants No. ST/T001739/1 and ST/P005101/1; and by the EU HORIZON2020 programme “Infrastructures”, project No. 654002 (ENSAR2). The computations were enabled by resources provided by the National Academic Infrastructure for Supercomputing in Sweden (NAISS) and the Swedish National Infrastructure for Computing (SNIC) at PDC, KTH. Open access funding provided by Royal Institute of Technology.
dc.type.okmA1


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