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Triaxial superdeformed bands in odd-odd Lu~(160~168) isotopes

机译:Lu〜(160〜168)同位素的三轴超形变能带

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The triaxial superdeformed rotational bands in the odd-odd Lu~(160~168) isotopes are investigated by performing the configuration dependent three-dimensional total routhian surface calculations. About fifty low lying triaxial superdeformed bands have been found for these odd-odd nuclei within the excitation energy of 3 MeV above the normal deformed yrast bands. The calculated equilibrium elongation, triaxial and hexadecapole deformations for these triaxial superdeformed bands are close to the values of ε_2~0.4, γ~20° and ε4~0.03, respectively. The configurations of calculated triaxial superdeformed bands have been assigned based on the total routhian surface calculations and the analysis of quasiparticle routhians in the rotating frame. The observed yrast triaxial superdeformed band of ~(164)Lu, where the linking transitions between superdeformed and normal deformed states are measured, have been reproduced by the present calculation in the relative energy to the normal deformed band. We show that the stability of superdeformed triaxial shapes in the odd-odd Lu isotopes is similar to that presented in odd-even Lu nuclei, and thus the wobbling excitations could be expected to occur in odd-odd Lu isotopes. The deformation driving effect of the proton high-j low-K orbit play an important role in the formation of the triaxial superdeformed states in both odd-odd and odd-even Lu isotopes, while the shell effect is a fundamental factor for the triaxial superdeformed shapes. The shell gaps and the positions of the deformation driving intruder orbits which are responsible for the triaxial superdeformed minima have been localized, particularly, the neutron N=94 gap and the position of the proton [660]1/2 orbit in the deformed single particle diagram provide the basis for a microscopic understanding of the observed triaxial superdeformed bands in the mass region.
机译:通过进行与构型有关的三维总鲁氏面计算,研究了奇数Lu〜(160〜168)同位素中的三轴超形变旋转带。对于这些奇数原子核,在正常变形的拉谱带之上3 MeV的激发能范围内,已经发现了大约五十个低三轴超形变带。这些三轴超形变带的平衡伸长率,三轴和十六极变形的计算值分别接近ε_2〜0.4,γ〜20°和ε4〜0.03。基于总的Routhian面计算和对旋转框架中准粒子Routhian的分析,已分配了计算的三轴超形变带的配置。观测到的〜(164)Lu的拉斯特三轴超形变带,已测量了超形变和正常形变态之间的连接跃迁,并通过本次计算以与正常形变带的相对能量进行了再现。我们表明奇异Lu同位素中超变形三轴形状的稳定性与奇偶Lu核中呈现的相似,因此可以预期在奇异Lu同位素中会发生摆动激发。质子高j低K轨道的形变驱动效应在奇奇和奇偶Lu同位素的三轴超形变态的形成中起着重要作用,而壳效应是三轴超形变的基本因素。形状。已经确定了负责产生三轴超形变最小值的壳间隙和变形驱动入侵者轨道的位置,特别是中子N = 94间隙和质子[660] 1/2轨道在变形的单个粒子中的位置该图为微观理解在质量区域中观察到的三轴超形变带提供了基础。

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