Valley charge-transfer insulator in twisted double bilayer WSe2

被引:0
作者
Wei, Lingnan [1 ]
Li, Qingxin [1 ]
Rehman, Majeed Ur [2 ]
He, Yangchen [3 ]
An, Dongdong [1 ]
Li, Shiwei [1 ]
Watanabe, Kenji [4 ]
Taniguchi, Takashi [5 ]
Claassen, Martin [6 ]
Novoselov, Kostya S. [7 ]
Kennes, Dante M. [8 ,9 ,10 ]
Rubio, Angel [10 ,11 ]
Rhodes, Daniel A. [3 ]
Xian, Lede [2 ,10 ,12 ]
Yu, Geliang [1 ,13 ]
Wang, Lei [1 ,13 ]
机构
[1] Nanjing Univ, Collaborat Innovat Ctr Adv Microstruct, Sch Phys, Natl Lab Solid State Microstruct, Nanjing, Peoples R China
[2] Songshan Lake Mat Lab, Dongguan, Guangdong, Peoples R China
[3] Univ Wisconsin, Dept Mat Sci & Engn, Madison, WI USA
[4] Natl Inst Mat Sci, Res Ctr Elect & Opt Mat, Tsukuba, Japan
[5] Natl Inst Mat Sci, Res Ctr Mat Nanoarchitecton, Tsukuba 3050003, Japan
[6] Univ Penn, Dept Phys & Astron, Philadelphia, PA USA
[7] Natl Univ Singapore, Dept Mat Sci & Engn, Singapore, Singapore
[8] Rhein Westfal TH Aachen, Inst Theorie Stat Phys, Aachen, Germany
[9] JARA Fundamentals Future Informat Technol, Aachen, Germany
[10] Max Planck Inst Struct & Dynam Matter, Ctr Free Electron Laser Sci CFEL, Hamburg, Germany
[11] Simons Fdn, Flatiron Inst, New York, NY 10010 USA
[12] Tsientang Inst Adv Study, Hangzhou, Zhejiang, Peoples R China
[13] Jiangsu Phys Sci Res Ctr, Nanjing, Peoples R China
基金
中国国家自然科学基金; 国家重点研发计划; 欧洲研究理事会;
关键词
TRANSITION; SUPERCONDUCTIVITY; CRYSTAL; STATES; MOTT;
D O I
10.1038/s41467-025-56490-w
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
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) WSe2, with twist angles near 60 degrees, as a controllable platform in which the K-valley band can be tuned to close vicinity of the Gamma-valley moir & eacute; flat band. At half-filling, correlations split the Gamma-valley flat band into upper and lower Hubbard bands and a charge-transfer insulator forms between the Gamma-valley upper Hubbard band and K-valley band. Using gate control, we continuously move the K-valley band across the Gamma-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.
引用
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页数:7
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