具有反对称分子动力学的O18的低能偶极子激发模式

Y. Shikata, Y. Kanada-En’yo
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引用次数: 0

摘要

在反对称分子动力学框架下,结合$\beta$约束和$K$ -投影后的变化,利用生成坐标法研究了$^{18}$ O中的低能偶极子(LED)激发。我们得到了两种LED状态,即具有显性壳模型结构的$1_1^-$状态和具有较大$^{14}\textrm{C}+\alpha$簇成分的$1_2^-$状态。这两种状态都具有显著的环向偶极子(TD)和压缩偶极子(CD)强度,表明TD和CD模式在$^{18}$ o的LED激发下不是分开的,而是混合的。这与像$^{10}$ Be这样变形良好的原子核的CD和TD模式不同,在很大程度上变形的状态下,CD和TD模式分别以$K^{\pi}=0^-$和$K^{\pi}=1^-$的形式产生。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Low-energy dipole excitation mode in O18 with antisymmetrized molecular dynamics
Low-energy dipole (LED) excitations in $^{18}$O were investigated using a combination of the variation after $K$-projection in the framework of antisymmetrized molecular dynamics with $\beta$-constraint with the generator coordinate method. We obtained two LED states, namely, the $1_1^-$ state with a dominant shell-model structure and the $1_2^-$ state with a large $^{14}\textrm{C}+\alpha$ cluster component. Both these states had significant toroidal dipole (TD) and compressive dipole (CD) strengths, indicating that the TD and CD modes are not separated but mixed in the LED excitations of $^{18}$O. This is unlike the CD and TD modes for well-deformed nuclei such as $^{10}$Be, where the CD and TD modes are generated as $K^{\pi}=0^-$ and $K^{\pi}=1^-$ excitations, respectively, in a largely deformed state.
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