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16+ Spin-Gap Isomer in 96Cd

Authors :
Singh, B. S. Nara
Liu, Z.
Wadsworth, R.
Grawe, H.
Brock, T. S.
Boutachkov, P.
Braun, N.
Blazhev, A.
Gorska, M.
Pietri, S.
Rudolph, D.
Domingo-Pardo, C.
Steer, S. J.
Atac, A.
Bettermann, L.
Caceres, L.
Eppinger, K.
Engert, T.
Faestermann, T.
Farinon, F.
Finke, F.
Geibel, K.
Gerl, J.
Gernhaeuser, R.
Goel, N.
Gottardo, A.
Grebosz, J.
Hinke, C.
Hoischen, R.
Ilie, G.
Iwasaki, H.
Jolie, J.
Kaskas, A.
Kojouharov, I.
Kruecken, R.
Kurz, N.
Merchan, E.
Nociforo, C.
Nyberg, Johan
Pfuetzner, M.
Prochazka, A.
Podolyak, Zs.
Regan, P. H.
Reiter, P.
Rinta-Antila, S.
Scholl, C.
Schaffner, H.
Söderström, Per-Anders
Warr, N.
Weick, H.
Wollersheim, H. -J
Woods, P. J.
Nowacki, F.
Sieja, K.
Source :
Physical Review Letters; 107(17), no 172502 (2011)
Publication Year :
2011
Publisher :
American Physical Society, 2011.

Abstract

A beta-decaying high-spin isomer in Cd-96, with a half-life T-1/2 = 0.29(-0.10)(+0.11) s, has been established in a stopped beam rare isotope spectroscopic investigations at GSI (RISING) experiment. The nuclei were produced using the fragmentation of a primary beam of Xe-124 on a Be-9 target. From the half-life and the observed gamma decays in the daughter nucleus, Ag-96, we conclude that the beta-decaying state is the long predicted 16(+) "spin-gap'' isomer. Shell-model calculations, using the Gross-Frenkel interaction and the pi nu(p(1/2,)g(9/2)) model space, show that the isoscalar component of the neutron-proton interaction is essential to explain the origin of the isomer. Core excitations across the N = Z = 50 gaps and the Gamow-Teller strength, Bd(GT) distributions have been studied via large-scale shell-model calculations using the pi nu(g, d, s) model space to compare with the experimental B(GT) value obtained from the half-life of the isomer.

Details

Language :
English
ISSN :
10797114
Database :
OpenAIRE
Journal :
Physical Review Letters; 107(17), no 172502 (2011)
Accession number :
edsair.pmid.dedup....ac5f772b00ed5ad225a047953bd64828