Spin-dependentγsoftness or triaxiality in even-even132-138Nd nuclei

  • The properties of γinstability in rapidly rotating even-even 132-138Nd isotopes have been investigated using the pairing-deformation self-consistent total-Routhian-surface calculations in a deformation space of ( β 2, γ, β 4). It is found that even-even 134-138Nd nuclei exhibit triaxiality in both ground and excited states, even up to high-spin states. The lightest isotope possesses a well-deformed prolate shape without a γdeformation component. The current numerical results are compared with previous calculations and available observables such as quadrupole deformation β 2and the feature of γ-band levels, showing basically a general agreement with the observed trend of γcorrelations (e.g. the pattern of the odd-even energy staggering of the γband). The existing differences between theory and experiment are analyzed and discussed briefly.
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CHAI Qing-Zhen, WANG Hua-Lei, YANG Qiong and LIU Min-Liang. Spin-dependent γsoftness or triaxiality in even-even 132-138Nd nuclei[J]. Chinese Physics C, 2015, 39(2): 024101. doi: 10.1088/1674-1137/39/2/024101
CHAI Qing-Zhen, WANG Hua-Lei, YANG Qiong and LIU Min-Liang. Spin-dependent γsoftness or triaxiality in even-even 132-138Nd nuclei[J]. Chinese Physics C, 2015, 39(2): 024101. doi:10.1088/1674-1137/39/2/024101 shu
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Received: 2014-04-25
Revised: 1900-01-01
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    Spin-dependentγsoftness or triaxiality in even-even132-138Nd nuclei

      Corresponding author:WANG Hua-Lei,

      Abstract:The properties ofγinstability in rapidly rotating even-even132-138Nd isotopes have been investigated using the pairing-deformation self-consistent total-Routhian-surface calculations in a deformation space of (β2,γ,β4). It is found that even-even134-138Nd nuclei exhibit triaxiality in both ground and excited states, even up to high-spin states. The lightest isotope possesses a well-deformed prolate shape without aγdeformation component. The current numerical results are compared with previous calculations and available observables such as quadrupole deformationβ2and the feature ofγ-band levels, showing basically a general agreement with the observed trend ofγcorrelations (e.g. the pattern of the odd-even energy staggering of theγband). The existing differences between theory and experiment are analyzed and discussed briefly.

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