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WFRF:(Jakobsson P. J)
 

Sökning: WFRF:(Jakobsson P. J) > Collectivity in the...

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FältnamnIndikatorerMetadata
00004953naa a2200889 4500
001oai:lup.lub.lu.se:bf96aca5-c473-49b7-a740-0ae23a2138f9
003SwePub
008160401s2015 | |||||||||||000 ||eng|
024a https://lup.lub.lu.se/record/75968362 URI
024a https://doi.org/10.1103/PhysRevC.91.0643132 DOI
040 a (SwePub)lu
041 a engb eng
042 9 SwePub
072 7a art2 swepub-publicationtype
072 7a ref2 swepub-contenttype
100a Gaffney, L. P.4 aut
2451 0a Collectivity in the light radon nuclei measured directly via Coulomb excitation
264 1c 2015
520 a Background: Shape coexistence in heavy nuclei poses a strong challenge to state-of-the-art nuclear models, where several competing shape minima are found close to the ground state. A classic region for investigating this phenomenon is in the region around Z = 82 and the neutron midshell at N = 104. Purpose: Evidence for shape coexistence has been inferred from a-decay measurements, laser spectroscopy, and in-beam measurements. While the latter allow the pattern of excited states and rotational band structures to be mapped out, a detailed understanding of shape coexistence can only come from measurements of electromagnetic matrix elements. Method: Secondary, radioactive ion beams of Rn-202 and Rn-204 were studied by means of low-energy Coulomb excitation at the REX-ISOLDE in CERN. Results: The electric-quadrupole (E2) matrix element connecting the ground state and first excited 2(1)(+) state was extracted for both Rn-202 and Rn-204, corresponding to B(E2; 2(1)(+) -> 0(1)(+)) = 29(-8)(+8) and 43(-12)(+17) W.u., respectively. Additionally, E2 matrix elements connecting the 2(1)(+) state with the 4(1)(+) and 2(2)(+) states were determined in Rn-202. No excited 0(+) states were observed in the current data set, possibly owing to a limited population of second-order processes at the currently available beam energies. Conclusions: The results are discussed in terms of collectivity and the deformation of both nuclei studied is deduced to be weak, as expected from the low-lying level-energy schemes. Comparisons are also made to state-of-the-art beyond-mean-field model calculations and the magnitude of the transitional quadrupole moments are well reproduced.
650 7a NATURVETENSKAPx Fysikx Subatomär fysik0 (SwePub)103012 hsv//swe
650 7a NATURAL SCIENCESx Physical Sciencesx Subatomic Physics0 (SwePub)103012 hsv//eng
700a Robinson, A. P.4 aut
700a Jenkins, D. G.4 aut
700a Andreyev, A. N.4 aut
700a Bender, M.4 aut
700a Blazhev, A.4 aut
700a Bree, N.4 aut
700a Bruyneel, B.4 aut
700a Butler, P. A.4 aut
700a Cocolios, T. E.4 aut
700a Davinson, T.4 aut
700a Deacon, A. N.4 aut
700a De Witte, H.4 aut
700a DiJulio, Douglasu Lund University,Lunds universitet,Kärnfysik,Fysiska institutionen,Institutioner vid LTH,Lunds Tekniska Högskola,Nuclear physics,Department of Physics,Departments at LTH,Faculty of Engineering, LTH4 aut0 (Swepub:lu)nucl-ddi
700a Diriken, J.4 aut
700a Ekström, Andreasu Lund University,Lunds universitet,Kärnfysik,Fysiska institutionen,Institutioner vid LTH,Lunds Tekniska Högskola,Nuclear physics,Department of Physics,Departments at LTH,Faculty of Engineering, LTH4 aut0 (Swepub:lu)nucl-ade
700a Fransen, Ch.4 aut
700a Freeman, S. J.4 aut
700a Geibel, K.4 aut
700a Grahn, T.4 aut
700a Hadinia, B.4 aut
700a Hass, M.4 aut
700a Heenen, P. -H.4 aut
700a Hess, H.4 aut
700a Huyse, M.4 aut
700a Jakobsson, U.4 aut
700a Kesteloot, N.4 aut
700a Konki, J.4 aut
700a Kroell, Th.4 aut
700a Kumar, V.4 aut
700a Ivanov, O.4 aut
700a Martin-Haugh, S.4 aut
700a Muecher, D.4 aut
700a Orlandi, R.4 aut
700a Pakarinen, J.4 aut
700a Petts, A.4 aut
700a Peura, P.4 aut
700a Rahkila, P.4 aut
700a Reiter, P.4 aut
700a Scheck, M.4 aut
700a Seidlitz, M.4 aut
700a Singh, K.4 aut
700a Smith, J. F.4 aut
700a Van de Walle, J.4 aut
700a Van Duppen, P.4 aut
700a Voulot, D.4 aut
700a Wadsworth, R.4 aut
700a Warr, N.4 aut
700a Wenander, F.4 aut
700a Wimmer, K.4 aut
700a Wrzosek-Lipska, K.4 aut
700a Zielinska, M.4 aut
710a Kärnfysikb Fysiska institutionen4 org
773t Physical Review C (Nuclear Physics)g 91:6q 91:6x 0556-2813
856u http://dx.doi.org/10.1103/PhysRevC.91.064313x freey FULLTEXT
8564 8u https://lup.lub.lu.se/record/7596836
8564 8u https://doi.org/10.1103/PhysRevC.91.064313

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