1998
DOI: 10.1016/s0370-2693(98)00030-6
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Identification of 181Hg and shape coexistence in odd-A Hg isotopes [Phys. Lett. B 410 (1997) 103]

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“…A variable moment of inertia (VMI) fit to the levels assumed to be unperturbed members of the prolate intruder bands was used to extrapolate energies of unperturbed 0 + band-heads (figure 10). Values of 1201 (30), 717 (20) and 425 (13) keV were obtained for the prolate bands in 176 Hg, 178 Hg and 180 Hg, respectively, revealing a rapid increase in the excitation energy of the prolate intruder structure with decreasing neutron number. In the Nilsson-Strutinsky calculations at zero spin of [13,38] the experimentally determined prolate band-head energies for even-mass Hg nuclei are quite well reproduced.…”
Section: Band-head Energiesmentioning
confidence: 96%
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“…A variable moment of inertia (VMI) fit to the levels assumed to be unperturbed members of the prolate intruder bands was used to extrapolate energies of unperturbed 0 + band-heads (figure 10). Values of 1201 (30), 717 (20) and 425 (13) keV were obtained for the prolate bands in 176 Hg, 178 Hg and 180 Hg, respectively, revealing a rapid increase in the excitation energy of the prolate intruder structure with decreasing neutron number. In the Nilsson-Strutinsky calculations at zero spin of [13,38] the experimentally determined prolate band-head energies for even-mass Hg nuclei are quite well reproduced.…”
Section: Band-head Energiesmentioning
confidence: 96%
“…The placement and the cascade character of the 529.9 and 400.9 keV γ rays remain tentative. N 126 taken from [15,16,[22][23][24][25][26][27][28][29][30][31][32][33] and this paper. The excitation energies of the 2 + , 4 + , 6 + and 8 + levels for the even-N isotopes are plotted together with the energies of the 17/2 + , 21/2 + , 25/2 + and 29/2 + levels relative to the lowest-lying 13/2 + states in odd-N isotopes.…”
Section: Nucleus 176mentioning
confidence: 99%