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Lifetimes of core-excited states in semi-magic 95Rh

dc.contributor.authorErtoprak, A.
dc.contributor.authorQi, C.
dc.contributor.authorCederwall, B.
dc.contributor.authorDoncel, M.
dc.contributor.authorJakobsson, U.
dc.contributor.authorNyakó, B. M.
dc.contributor.authorJaworski, G.
dc.contributor.authorDavies, P.
dc.contributor.authorde France, G.
dc.contributor.authorKuti, I.
dc.contributor.authorNapoli, D. R.
dc.contributor.authorWadsworth, R.
dc.contributor.authorGhugre, S. S.
dc.contributor.authorRaut, R.
dc.contributor.authorAkkus, B.
dc.contributor.authorAl Azri, H.
dc.contributor.authorAlgora, A.
dc.contributor.authorde Angelis, G.
dc.contributor.authorAtac, A.
dc.contributor.authorBäck, T.
dc.contributor.authorBoso, A.
dc.contributor.authorClément, E.
dc.contributor.authorDebenham, D. M.
dc.contributor.authorDombrádi, Zs.
dc.contributor.authorErtürk, S.
dc.contributor.authorGadea, A.
dc.contributor.authorGhazi, Moradi F.
dc.contributor.authorGottardo, A.
dc.contributor.authorHüyük, T.
dc.contributor.authorIdeguchi, E.
dc.contributor.authorLi, H.
dc.contributor.authorMichelagnoli, C.
dc.contributor.authorModamio, V.
dc.contributor.authorNyberg, J.
dc.contributor.authorPalacz, M.
dc.contributor.authorPetrache, C. M.
dc.contributor.authorRecchia, F.
dc.contributor.authorSandzelius, M.
dc.contributor.authorSiciliano, M.
dc.contributor.authorSohler, D.
dc.contributor.authorTimár, J.
dc.contributor.authorValiente-Dobón, J. J.
dc.contributor.authorXiao, Z. G.
dc.date.accessioned2020-11-24T09:42:29Z
dc.date.available2020-11-24T09:42:29Z
dc.date.issued2020
dc.identifier.citationErtoprak, A., Qi, C., Cederwall, B., Doncel, M., Jakobsson, U., Nyakó, B. M., Jaworski, G., Davies, P., de France, G., Kuti, I., Napoli, D. R., Wadsworth, R., Ghugre, S.S., Raut, R., Akkus, B., Al Azri, H., Algora, A., de Angelis, G., Atac, A., . . . Xiao, Z. G. (2020). Lifetimes of core-excited states in semi-magic 95Rh. <i>European Physical Journal A</i>, <i>56</i>(11), Article 291. <a href="https://doi.org/10.1140/epja/s10050-020-00297-4" target="_blank">https://doi.org/10.1140/epja/s10050-020-00297-4</a>
dc.identifier.otherCONVID_47079972
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/72758
dc.description.abstractLifetimes of negative-parity states have been determined in the neutron deficient semi-magic (N = 50) nucleus 95Rh. The fusion-evaporation reaction 58Ni(40Ca,3p) was used to populate high-spin states in 95Rh at the Grand Accélérateur National d’Ions Lourds (GANIL) accelerator facility. The results were obtained using the Doppler Shift Attenuation Method (DSAM) based on the Doppler broadened line shapes produced during the slowing down process of the residual nuclei in a thick 6mg/cm2 metallic target. B(M1) and B(E2) reduced transition strengths are compared with predictions from large-scale shell-model calculations.en
dc.format.mimetypeapplication/pdf
dc.languageeng
dc.language.isoeng
dc.publisherSpringer
dc.relation.ispartofseriesEuropean Physical Journal A
dc.rightsCC BY 4.0
dc.subject.otherlifetimes
dc.subject.othercore-excited states
dc.titleLifetimes of core-excited states in semi-magic 95Rh
dc.typeresearch article
dc.identifier.urnURN:NBN:fi:jyu-202011246730
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineKiihdytinlaboratoriofi
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.numberinseries11
dc.relation.volume56
dc.type.versionpublishedVersion
dc.rights.copyright© 2020 the Authors
dc.rights.accesslevelopenAccessfi
dc.type.publicationarticle
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.doi10.1140/epja/s10050-020-00297-4
jyx.fundinginformationOpen access funding provided by Royal Institute of Technology. his work was supported by the Swedish Research Council under Grant Nos. 621-2014-5558, 621-2012-3805, and 621-2013-4323 and the Göran Gustafsson foundation, the Scientific Research Projects Coordination Unit of Istanbul University Project No. 47886 and 48101, the UK STFC under grants number ST/L005727/1 and ST/P003885/1, the Spanish Ministerio de Economía y Competitividad under grant FPA2014-52823-C2-1-P and the program Severo Ochoa (SEV-2014-0398), Ministerio de Ciencia e Innovación, and Generalitat Valenciana, Spain, under the Grants FPA2017-84756-C4, PROMETEO/2019/005 and by the EU FEDER funds, the Scientific and Technological Council of Turkey (Proj. no. 114F473), the National Science Centre, Poland (NCN), 2017/25/B/ST2/01569, 2016/22/M/ST2/00269, 2013/08/M/ST2/00257, COPIGAL and COPIN-IN2P3 projects. B.M.Ny., I.K., Zs.D. and J.T. acknowledge the support of the National Research, Development and Innovation Fund of Hungary, financed under the K18 funding scheme with project no. K128947, as well as by the European Regional Development Fund (Contract No. GINOP-2.3.3-15-2016-00034), while I.K. was also supported by the National Research, Development and Innovation Office NKFIH, contract number PD 124717. The computations were performed on resources provided by the Swedish National Infrastructure for Computing (SNIC) at PDC, KTH, Stockholm.
dc.type.okmA1


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