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Nuclear Shape Staggering in Very Neutron-Deficient Hg Isotopes Detected by Laser Spectroscopy
107
Citations
17
References
1977
Year
Nuclear Shape StaggeringMicrowave SpectroscopyCosmic AbundanceExperimental Nuclear PhysicsNuclear PhysicsPhysicsEngineeringNatural SciencesLaser SpectroscopySpectroscopyNuclear DataNeutron SourceTunable Dye LaserOdd Hg IsotopesNuclear ExperimentsNeutron ScatteringNuclear Engineering
The isotope shifts of $^{188}\mathrm{Hg}$, $^{186}\mathrm{Hg}$, and $^{184}\mathrm{Hg}$ in the 2537-\AA{} line have been measured by use of tunable dye laser at the on-line mass separator ISOLDE at CERN. The results are $\ensuremath{\delta}\ensuremath{\nu}(^{188}\mathrm{Hg}\ensuremath{-}^{204}\mathrm{Hg})=35.8(2)$ GHz; $\ensuremath{\delta}\ensuremath{\nu}(^{186}\mathrm{Hg}\ensuremath{-}^{204}\mathrm{Hg})=39.4(2)$ GHz; and $\ensuremath{\delta}\ensuremath{\nu}(^{184}\mathrm{Hg}\ensuremath{-}^{204}\mathrm{Hg})=43.1(2)$ GHz. These data combined with those obtained by $\ensuremath{\beta}$-radiation-detected optical pumping ($\ensuremath{\beta}$-RADOP) on the odd Hg isotopes yield a huge odd-even staggering for $^{185}\mathrm{Hg}$ of $\ensuremath{\gamma}=\frac{(2\ensuremath{\delta}{\ensuremath{\nu}}^{\frac{185}{184}})}{\ensuremath{\delta}{\ensuremath{\nu}}^{\frac{186}{184}}}=13(1)$ which has to be interpreted as nuclear shape staggering.
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