材料科学
薄膜
凝聚态物理
密度泛函理论
光电发射光谱学
费米能级
纳米技术
化学物理
光电子学
X射线光电子能谱
化学工程
化学
计算化学
电子
物理
工程类
量子力学
作者
Takemi Kato,K. Nakayama,Yongkai Li,Zhiwei Wang,K. Sugawara,Kiyohisa Tanaka,T. Takahashi,Yugui Yao,T. Sato
标识
DOI:10.1002/advs.202309003
摘要
Abstract Applying lattice strain to thin films, a critical factor to tailor their properties such as stabilizing a structural phase unstable at ambient pressure, generally necessitates heteroepitaxial growth to control the lattice mismatch with substrate. Therefore, while homoepitaxy, the growth of thin film on a substrate made of the same material, is a useful method to fabricate high‐quality thin films, its application to studying strain‐induced structural phases is limited. Contrary to this general belief, here the quasi‐homoepitaxial growth of Cs and Rb thin films is reported with substantial in‐plane compressive strain. This is achieved by utilizing the alkali‐metal layer existing in bulk crystal of kagome metals A V 3 Sb 5 ( A = Cs and Rb) as a structural template. The angle‐resolved photoemission spectroscopy measurements reveal the formation of metallic quantum well states and notable thickness‐dependent quasiparticle lifetime. Comparison with density functional theory calculations suggests that the obtained thin films crystalize in the face‐centered cubic structure, which is typically stable only under high pressure in bulk crystals. These findings provide a useful approach for synthesizing highly strained thin films by quasi‐homoepitaxy, and pave the way for investigating many‐body interactions in Fermi liquids with tunable dimensionality.
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