Evolution of flat bands in MoSe$_2$/WSe$_2$ moiré lattices: A study combining machine learning and band unfolding methods

Shengguo Yang, Jiaxin Chen, Chao-Fei Liu, Mingxing Chen
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Abstract

Moir\'e lattices have served as the ideal quantum simulation platform for exploring novel physics due to the flat electronic bands resulting from the long wavelength moir\'e potentials. However, the large sizes of this type of system challenge the first-principles methods for full calculations of their electronic structures, thus bringing difficulties in understanding the nature and evolution of the flat bands. In this study, we investigate the electronic structures of moir\'e patterns of MoSe$_2$/WSe$_2$ by combining ab initio and machine learning methods. We find that a flat band with a bandwidth of about 5 meV emerges below the valence band edge at the K point for the H-stacking at a twist angle of 3.89$^{\circ}$. Then, it shifts dramatically as the twist angle decreases and becomes about 20 meV higher than the valence band maximum for the twist angle of 3.15$^{\circ}$. Multiple ultra-flat bands emerge as the twist angle is reduced to 1.7$^{\circ}$. Band unfolding reveals that the ultra-flat bands formed by the $\Gamma$ and K valleys show distinct behaviors. The $\Gamma$-valley flat bands are sensitive to the interlayer coupling, thus experiencing dramatic changes as the twist angle decreases. In contrast, the K-valley flat band, which shows a weak dependence on the interlayer coupling, is mainly modulated by the long wavelength moir\'e potential. Therefore, a relatively small angle (2.13$^{\circ}$) is required to generate the K-valley flat band, which experiences a transition from the honeycomb to the triangular lattice as the twist angle decreases.
MoSe$_2$/WSe$_2$ 摩尔晶格中平带的演变:结合机器学习和波段展开方法的研究
由于长波长摩尔电势产生的平坦电子带,摩尔晶格已成为探索新物理学的理想量子模拟平台。然而,这类系统的巨大尺寸对全面计算其电子结构的第一性原理方法提出了挑战,从而给理解平坦带的性质和演化带来了困难。在本研究中,我们结合 ab initio 和机器学习方法研究了 MoSe$_2$/WSe$_2$ 的 Moir\'e 模式的电子结构。我们发现,在扭曲角度为 3.89$^{\circ}$ 时,H-叠层在 K 点价带边缘下方出现了一个带宽约为 5meV 的平带。然后,它随着扭曲角度的减小而急剧移动,并在扭曲角度为 3.15$^{\circ}$ 时比价带最大值高出约 20 meV。当扭转角减小到 1.7$^{\circ}$ 时,出现了多个超平带。波段展开显示,由 $\Gamma$ 和 K 谷形成的超扁平波段表现出截然不同的行为。Gamma谷平带对层间耦合很敏感,随着扭转角的减小而发生剧烈变化。相比之下,K 谷平带对层间耦合的依赖性较弱,主要受长波长摩尔电势的调制。因此,产生 K 谷平带需要很小的角度(2.13^{\circ}$),随着扭转角的减小,K 谷平带经历了从蜂巢到三角晶格的转变。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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