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Search for a 2-quasiparticle high-Kisomer inRf256
Author(s) -
Andrew Robinson,
T. L. Khoo,
D. Seweryniak,
I. Ahmad,
Mitsuteru Asai,
B. B. Back,
M. P. Carpenter,
P. Chowdhury,
C. N. Davids,
J. P. 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,
А. Лопез-Мартенс,
P. Marley,
E. A. McCutchan,
P. Papadakis,
D. Peterson,
J. Qian,
D. Rostron,
Urmila Shirwadkar,
I. Stefanescu,
S. K. Tandel,
X. Wang,
S. Zhu
Publication year - 2011
Publication title -
physical review. c. nuclear physics/physical review. c, nuclear physics
Language(s) - English
Resource type - Journals
eISSN - 1089-490X
pISSN - 0556-2813
DOI - 10.1103/physrevc.83.064311
Subject(s) - physics , quasiparticle , condensed matter physics , superconductivity
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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