Geometry and electronic structures of rare earth-doped boron-based clusters <inline-formula><tex-math id="M2">\begin{document}$ {\text{REB}}_n^ - $\end{document}</tex-math></inline-formula> (RE = La, Sc; <i>n</i> = 6, 8)

稀土 兴奋剂 原子物理学 物理 化学 材料科学 结晶学 矿物学 凝聚态物理 核物理学
作者
Chen Zi-Jun,LI Hui-fang,Xie Zhen-Ming,Yong‐Hang Zhang,Hao Zheng,Kai‐Le Jiang,Bo Zhang,Jiaming Zhang,Huai‐Qian Wang
出处
期刊:Chinese Physics [Science Press]
卷期号:73 (19): 193601-193601 被引量:1
标识
DOI:10.7498/aps.73.20240962
摘要

Rare earth doped boron clusters have attracted much attention due to their special optical, electrical and magnetic properties. The geometric structures, stability, electronic properties and aromaticity of negative rare earth doped boron clusters <inline-formula><tex-math id="M11">\begin{document}$ {\text{REB}}_n^ - $\end{document}</tex-math></inline-formula> (RE = La, Sc; <i>n</i> = 6, 8) are investigated with the artificial bee colony algorithm combined with density functional theory calculations at the PBE0/RE/SDD//B/6-311+G* level of theory. Calculations show that the ground state structures of <inline-formula><tex-math id="M12">\begin{document}$ {\text{REB}}_n^ - $\end{document}</tex-math></inline-formula> (RE = La, Sc; <i>n</i> = 6, 8) are all of <i>C</i><sub>2</sub> symmetry, and the doped lanthanide atom is located in a “boat-shaped” structure at the top center. By comparing with the experimental photoelectron spectra, it is confirmed that the ground state structure of <inline-formula><tex-math id="M13">\begin{document}$ {\text{LaB}}_{8}^ - $\end{document}</tex-math></inline-formula> is a “zither-like” three-dimensional structure, and the ground state structure of <inline-formula><tex-math id="M14">\begin{document}$ {\text{ScB}}_{8}^ - $\end{document}</tex-math></inline-formula> is an “umbrella” structure with <i>C</i><sub>7<i>v</i></sub> symmetry formed by the scandium atom at the “umbrella handle”. The electron localization between RE—B is not as good as that between B—B. The simulated photoelectron spectra have similar spectral characteristics to the experimental results. The lowest energy structures of <inline-formula><tex-math id="M15">\begin{document}$ {\text{LaB}}_{6}^ - $\end{document}</tex-math></inline-formula> and <inline-formula><tex-math id="M16">\begin{document}$ {\text{ScB}}_{6}^ - $\end{document}</tex-math></inline-formula> are <i>σ</i>-π double aromatic clusters, and the structures exhibit aromaticity. The density of states of low-energy isomers shows that the open shell <inline-formula><tex-math id="M17">\begin{document}$ {\text{ScB}}_{8}^ - $\end{document}</tex-math></inline-formula> density of states spectrum exhibits spin polarization phenomenon, which is expected to assemble magnetic material components. These studies contribute to understanding the evolution of structure and properties of nanomaterials, and provide important theoretical support for designing nanomaterials with practical value.
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