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16(+) Spin-Gap Isomer in (96)Cd

  作者 Singh, BSN; Liu, Z; Wadsworth, R; Grawe, H; Brock, TS; Boutachkov, P; Braun, N; Blazhev, A; Gorska, M; Pietri, S; Rudolph, D; Domingo-Pardo, C; Steer, SJ; Atac, A; Bettermann, L; Caceres, L; Eppinger, K; Engert, T; Faestermann, T; Farinon, F; Finke, F; Geibel, K; Gerl, J; Gernhauser, R; Goel, N; Gottardo, A; Grebosz, J; Hinke, C; Hoischen, R; Ilie, G; Iwasaki, H; Jolie, J; Kaskas, A; Kojouharov, I; Krucken, R; Kurz, N; Merchan, E; Nociforo, C; Nyberg, J; Pfutzner, M; Prochazka, A; Podolyak, Z; Regan, PH; Reiter, P; Rinta-Antila, S; Scholl, C; Schaffner, H; Soderstrom, PA; Warr, N; Weick, H; Wollersheim, HJ; Woods, PJ; Nowacki, F; Sieja, K  
  选自 期刊  PHYSICAL REVIEW LETTERS;  卷期  2011年107-17;  页码  172502-172502  
  关联知识点  
 

[摘要]A beta-decaying high-spin isomer in (96)Cd, 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 (124)Xe on a (9)Be target. From the half-life and the observed gamma decays in the daughter nucleus, (96)Ag, 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.

 
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