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High-Kmultiquasiparticle configurations and limiting moments of inertia in178W
Author(s) -
D. M. Cullen,
S. L. King,
A. T. Reed,
J.A. Sampson,
P. M. Walker,
C. Wheldon,
F. R. Xu,
G.D. Dracoulis,
I.-Y. Lee,
A. O. Macchiavelli,
R. W. MacLeod,
A. N. Wilson,
C. J. Barton
Publication year - 1999
Publication title -
physical review c
Language(s) - English
Resource type - Journals
eISSN - 1089-490X
pISSN - 0556-2813
DOI - 10.1103/physrevc.60.064301
Subject(s) - physics , nucleon , moment of inertia , energy (signal processing) , particle physics , atomic physics , quantum mechanics
Three new high-$K$ multiquasiparticle intrinsic states, ${K}^{\ensuremath{\pi}}{=(29}^{+}),$ ${K}^{\ensuremath{\pi}}{=30}^{+},$ and ${K}^{\ensuremath{\pi}}{=(34}^{+}),$ have been assigned in ${}^{178}\mathrm{W}.$ The configurations of these states are based on ten, eight, and ten, unpaired nucleons, respectively, and they represent the highest-seniority intrinsic K states observed to date. The $\ensuremath{\gamma}$-ray intensity branching ratios and associated $|{g}_{K}\ensuremath{-}{g}_{R}|$ values have been used to contribute to the specifications of the underlying single-particle configurations of the states. Configuration-constrained potential energy surface calculations indicate that the nucleus retains stably deformed axially symmetric shapes. This evidence, coupled with the experimental $\ensuremath{\gamma}$-ray decay rates, suggests that K remains a good quantum number in these highest-seniority intrinsic state configurations. The aligned angular momenta of the ${K}^{\ensuremath{\pi}}{=(29}^{+}),$ ${K}^{\ensuremath{\pi}}{=30}^{+},$ and ${K}^{\ensuremath{\pi}}{=(34}^{+})$ bands are observed to be lower than those of the other eight quasiparticle, ${K}^{\ensuremath{\pi}}{=25}^{+}$ and ${K}^{\ensuremath{\pi}}{=28}^{\ensuremath{-}}$ bands in ${}^{178}\mathrm{W}.$ These differences are interpreted as the effects of reduced pairing due to blocking by the constituent particles. While the dynamic moments of inertia are similar, they remain substantially less than those of a classical rigid rotor, apparently saturating at a value of about $56{\ensuremath{\Elzxh}}^{2} {\mathrm{MeV}}^{\ensuremath{-}1}.$

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