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扭曲双双层WSe中的谷电荷转移绝缘体

Valley charge-transfer insulator in twisted double bilayer WSe.

作者信息

Wei LingNan, Li Qingxin, Rehman Majeed Ur, He Yangchen, An Dongdong, Li Shiwei, Watanabe Kenji, Taniguchi Takashi, Claassen Martin, Novoselov Kostya S, Kennes Dante M, Rubio Angel, Rhodes Daniel A, Xian Lede, Yu Geliang, Wang Lei

机构信息

National Laboratory of Solid-State Microstructures, Collaborative Innovation Center of Advanced Microstructures, School of Physics, Nanjing University, Nanjing, China.

Songshan Lake Materials Laboratory, Dongguan, Guangdong, China.

出版信息

Nat Commun. 2025 Jan 30;16(1):1185. doi: 10.1038/s41467-025-56490-w.

Abstract

In flat-band systems, emergent physics can be substantially modified by the presence of another nearby electronic band. For example, a Mott˘Hubbard insulator can turn into a charge transfer insulator if other electronic states enter between the upper and lower Hubbard bands. Here, we introduce twisted double bilayer (TDB) WSe, with twist angles near 60°, as a controllable platform in which the K-valley band can be tuned to close vicinity of the Γ-valley moiré flat band. At half-filling, correlations split the Γ-valley flat band into upper and lower Hubbard bands and a charge-transfer insulator forms between the Γ-valley upper Hubbard band and K-valley band. Using gate control, we continuously move the K-valley band across the Γ-valley Hubbard bands, and observe a tunable charge-transfer insulator gap and subsequently a continuous phase transition to a metal. The tuning of Mott˘Hubbard to charge-transfer insulator establishes valley degree of freedom as a suitable knob for transitions between exotic correlated phases.

摘要

在平带系统中,邻近的另一个电子能带的存在会显著改变涌现的物理特性。例如,如果其他电子态进入上下哈伯德带之间,莫特-哈伯德绝缘体可以转变为电荷转移绝缘体。在此,我们引入扭曲双双层(TDB)WSe₂,其扭曲角接近60°,作为一个可控平台,其中K谷能带可被调谐到接近Γ谷莫尔平带的位置。在半填充时,关联作用将Γ谷平带分裂为上下哈伯德带,并且在Γ谷上哈伯德带和K谷能带之间形成电荷转移绝缘体。通过栅极控制,我们使K谷能带连续穿过Γ谷哈伯德带,并观测到一个可调谐的电荷转移绝缘体能隙,随后是向金属的连续相变。从莫特-哈伯德到电荷转移绝缘体的调谐确立了谷自由度作为在奇异关联相之间转变的合适旋钮。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/fcfe/11782666/f0dcd559c70d/41467_2025_56490_Fig1_HTML.jpg

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