Search for a 2-quasiparticle high-K isomer in (256)Rf

A. P. Robinson,T. L. Khoo,D. Seweryniak, I. Ahmad,M. Asai, B. B. Back,M. P. Carpenter,P. Chowdhury, C. N. Davids,J. Greene,P. T. Greenlees,K. Hauschild, A. Heinz,R. -D. Herzberg,R. V. F. Janssens, D. G. Jenkins,G. D. Jones,S. Ketelhut, F. G. Kondev,T. Lauritsen, C. J. Lister, A. Lopez-Martens, P. Marley,E. McCutchan,P. Papadakis,D. Peterson,J. Qian, D. Rostron, U. Shirwadkar,I. Stefanescu,S. K. Tandel,X. Wang, S. Zhu

PHYSICAL REVIEW C(2011)

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摘要
The energies of 2-quasiparticle (2-qp) states in heavy shell-stabilized nuclei provide information on the single-particle states that are responsible for the stability of superheavy nuclei. We have calculated the energies of 2-qp states in (256)Rf, which suggest that a long-lived, low-energy 8(-) isomer should exist. A search was conducted for this isomer through a calorimetric conversion electron signal, sandwiched in time between implantation of a (256)Rf nucleus and its fission decay, all within the same pixel of a double-sided Si strip detector. A 17(5)-mu s isomer was identified. However, its low population, similar to 5(2)% that of the ground state instead of the expected similar to 30%, suggests that it is more likely a 4-qp isomer. Possible reasons for the absence of an electromagnetic signature of a 2-qp isomer decay are discussed. These include the favored possibility that the isomer decays by fission, with a half-life indistinguishably close to that of the ground state. Another possibility, that there is no 2-qp isomer at all, would imply an abrupt termination of axially symmetric deformed shapes at Z = 104, which describes nuclei with Z = 92-103 very well.
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