论文标题

元素同位素的核时光左右$ n $ = 40

Nuclear Moments of Germanium Isotopes around $N$ = 40

论文作者

Kanellakopoulos, A., Yang, X. F., Bissell, M. L., Reitsma, M. L., Bai, S. W., Billowes, J., Blaum, K., Borschevsky, A., Cheal, B., Devlin, C. S., Ruiz, R. F. Garcia, Heylen, H., Kaufmann, S., König, K., Koszorús, Á., Lechner, S., Malbrunot-Ettenauer, S., Neugart, R., Neyens, G., Nörtershäuser, W., Ratajczyk, T., Rodríguez, L. V., Sels, S., Wang, S. J., Xie, L., Xu, Z. Y., Yordanov, D. T.

论文摘要

在Isolde-Cern上,对$^{69,71,73} $ ge同位素($ z = 32 $)进行了线性激光光谱测量。 $ 4S^2 4p^2 \,^3p_1 \ rightArrow 4S^2 4p 5s \,^3p_1^o $的超细结构用269 nm的激光探测到也应介绍的频率和频率加倍技术。使用最先进的原子相对论的Fock空间耦合群集计算计算了两个原子水平的超细场。从这些计算和先前测量的精度超精细参数确定了一个新的$^{73} $ ge Quadrupole矩,产生$ q _ {\ rm s} $ = $ - $ 0.198(4)b,与分子量表的文献价值达成了极好的一致性。 $^{69} $ ge的矩进行了修订:$μ$ = +0.920(5)$μ_{n} $和$ q _ {\ rm s} $ = +0.114(8)b,以及$^{71} $的GE。 $ n = 40 $的实验力矩使用Jun45相互作用来解释大规模壳模型,尽管其$ g $ - factors躺在有效的单颗粒值附近,但揭示了相当混合的波函数配置。通过与相邻的异酮进行比较,从镍的单粒子性质到锗中变形的结构变化大约在$ n = 40 $左右。

Collinear laser spectroscopy measurements were performed on $^{69,71,73}$Ge isotopes ($Z = 32$) at ISOLDE-CERN. The hyperfine structure of the $4s^2 4p^2 \, ^3P_1 \rightarrow 4s^2 4p 5s \, ^3P_1^o$ transition of the germanium atom was probed with laser light of 269 nm, produced by combining the frequency-mixing and frequency-doubling techniques. The hyperfine fields for both atomic levels were calculated using state-of-the-art atomic relativistic Fock-space coupled-cluster calculations. A new $^{73}$Ge quadrupole moment was determined from these calculations and previously measured precision hyperfine parameters, yielding $Q_{\rm s}$ = $-$0.198(4) b, in excellent agreement with the literature value from molecular calculations. The moments of $^{69}$Ge have been revised: $μ$ = +0.920(5) $μ_{N}$ and $Q_{\rm s}$= +0.114(8) b, and those of $^{71}$Ge have been confirmed. The experimental moments around $N = 40$ are interpreted with large-scale shell-model calculations using the JUN45 interaction, revealing rather mixed wave function configurations, although their $g$-factors are lying close to the effective single-particle values. Through a comparison with neighboring isotones, the structural change from the single-particle nature of nickel to deformation in germanium is further investigated around $N = 40$.

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