双层石墨烯
极地的
凝聚态物理
材料科学
超晶格
分子物理学
双层
魔法角
单层
堆积
扫描隧道显微镜
结晶学
物理
石墨烯
化学
纳米技术
谱线
核磁共振
量子力学
膜
生物化学
作者
Xingju Zhao,Yang Yang,Dong‐Bo Zhang,Su‐Huai Wei
标识
DOI:10.1103/physrevlett.124.086401
摘要
The existence of Bloch flat bands of electrons provides a facile pathway to obtain exotic quantum phases owing to strong correlation. Despite the established magic angle mechanism for twisted bilayer graphene, understanding of the emergence of flat bands in twisted bilayers of two-dimensional polar crystals remains elusive. Here, we show that due to the polarity between constituent elements in the monolayer, the formation of complete flat bands in twisted bilayers is triggered as long as the twist angle is less than a certain critical value. Using the twisted bilayer of hexagonal boron nitride (hBN) as an example, our simulations using the density-functional tight-binding method reveal that the flat band originates from the stacking-induced decoupling of the highest occupied (lowest unoccupied) states, which predominantly reside in the regions of the moiré superlattice where the anion (cation) atoms in both layers are overlaid. Our findings have important implications for the future search for and study of flat bands in polar materials.
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