论文标题

$^{40} $ ca中从超级形式的频段过渡的电动单极过渡

Electric monopole transition from the superdeformed band in $^{40}$Ca

论文作者

Ideguchi, E., Kibédi, T., Dowie, J. T. H., Hoang, T. H., Raju, M. Kumar, Aoi, N., Mitchell, A. J., Stuchbery, A. E., Shimizu, N., Utsuno, Y., Akber, A., Bignell, L. J., Coombes, B. J., Eriksen, T. K., Gray, T. J., Lane, G. J., McCormick, B. P.

论文摘要

连接第三个0 $^+$ Level的过渡,电动单极($ e0 $)的过渡强度$ρ^2 $,它是“ SuperDeformed”频段的头部,与“球形” 0 $^+$ offer offer magic $^{40} $ ca中的“球形” 0 $^+$地面状态通过$ e^+e^+e^+e^+e^ - $ paigh-$ $ paigh-$ $ paigh-$ $ $ $ e^ - $ $ $ $ $ $ $ $。测量值$ρ^2(e0; 0^+_ 3 \ to 0^+_ 1)〜= 〜2.3(5)\ times10^{ - 3} $,是最小的$ρ^2(e0; 0^+\ to 0^to 0^+)$。相反,从第二个0 $^+$状态观察到的$ e0 $过渡强度是“正常”变形的频段负责人,是一个更大的数量级,$ρ^2(e0; 0^+_ 2 \ _ 2 \ to 0^+_ 1)进行了大规模的壳模型(LSSM)计算,以了解激发态的显微镜结构,并在它们之间进行构型混合; $^{40} $ CA中的实验$ρ^2 $值,而相邻的同位素是通过LSSM计算很好地复制的。异常小的$ρ^2(e0; 0^+_ 3 \至0^+_ 1)$值是由于形状折叠式结构的混合中的破坏性干扰,这些结构基于几种不同的多颗粒 - multihole激发。该观察结果超出了对$ E0 $强度的通常处理,在这种情况下,两态形状混合不会导致破坏性干扰。

The electric monopole ($E0$) transition strength $ρ^2$ for the transition connecting the third 0$^+$ level, a "superdeformed" band head, to the "spherical" 0$^+$ ground state in doubly magic $^{40}$Ca has been determined via $e^+e^-$ pair-conversion spectroscopy. The measured value, $ρ^2(E0; 0^+_3 \to 0^+_1)~=~2.3(5)\times10^{-3}$, is the smallest $ρ^2(E0; 0^+ \to 0^+)$ found in $A<50$ nuclei. In contrast, the $E0$ transition strength to the ground state observed from the second 0$^+$ state, a band head of "normal" deformation, is an order of magnitude larger, $ρ^2(E0; 0^+_2 \to 0^+_1)~=~25.9(16)\times~10^{-3}$, which shows significant mixing between these two states. Large-Scale Shell Model (LSSM) calculations were performed to understand the microscopic structure of the excited states, and the configuration mixing between them; experimental $ρ^2$ values in $^{40}$Ca and neighboring isotopes were well reproduced by the LSSM calculations. The unusually small $ρ^2(E0; 0^+_3 \to 0^+_1)$ value is due to destructive interference in the mixing of shape-coexisting structures, which are based on several different multiparticle-multihole excitations. This observation goes beyond the usual treatment of $E0$ strengths, where two-state shape mixing cannot result in destructive interference.

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