The properties of $\gamma$ instability in rapidly rotating even-even $^{ 132-138}$Nd isotopes have been investigated using the pairing-deformation self-consistent total-Routhian-surface calculations in a deformation space of ($\beta_2, \gamma, \beta_4$). It is found that even-even $^{ 134-138}$Nd nuclei exhibit the triaxiality in both ground and excited states, even up to high-spin ones. The lightest isotope possesses a well-deformed prolate shape without $\gamma$ deformation component. The current numerical results are compared with previous calculations and available observables, showing basically a general agreement with the observed trend of $\gamma$ correlations. The existing differences between theory and experiment are analyzed and discussed briefly.
Categories: nucl-th