Strongly correlated Hofstadter subbands in minimally twisted bilayer graphene

被引:0
|
作者
Shen, Cheng [1 ,5 ]
Guan, Yifei [1 ]
Pizzirani, Davide [2 ]
Zhou, Zekang [1 ]
Barman, Punam [1 ]
Watanabe, Kenji [3 ]
Taniguchi, Takashi [4 ]
Wiedmann, Steffen [2 ]
Yazyev, Oleg V. [1 ]
Banerjee, Mitali [1 ]
机构
[1] Ecole Polytech Fed Lausanne EPFL, Inst Phys, CH-1015 Lausanne, Switzerland
[2] Radboud Univ Nijmegen, High Field Magnet Lab HFML EMFL, Toernooiveld 7, NL-6525ED Nijmegen, Netherlands
[3] Natl Inst Mat Sci, Res Ctr Funct Mat, 1-1 Namiki, Tsukuba 3050044, Japan
[4] Natl Inst Mat Sci, Int Ctr Mat Nanoarchitecton, 1-1 Namiki, Tsukuba 3050044, Japan
[5] Univ Elect Sci & Technol China, Sch Phys, Chengdu 610054, Peoples R China
基金
瑞士国家科学基金会;
关键词
FRACTIONAL CHERN INSULATORS; DIRAC FERMIONS; SUPERCONDUCTIVITY; STATES; SPIN;
D O I
10.1103/PhysRevB.110.L161402
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The moir & eacute; superlattice in twisted bilayer graphene has been proven to be a versatile platform for exploring exotic quantum phases. Extensive investigations have been invoked focusing on the zero-magnetic-field phase diagram at the magic twist angle around theta = 1.1 degrees, which has been indicated to be an exclusive regime for exhibiting a flat band with the interplay of strong electronic correlation and untrivial topology in the experiment so far. In contrast, electronic bands in non-magic-angle twisted bilayer graphene host dominant electronic kinetic energy compared to Coulomb interaction. By quenching the kinetic energy and enhancing Coulomb exchange interactions by means of an applied perpendicular magnetic field, here we unveil gapped flat Hofstadter subbands at large magnetic flux that yield correlated insulating states in minimally twisted bilayer graphene at theta = 0.41 degrees. These states appear with isospin symmetry breaking due to strong Coulomb interactions. Our work provides a platform to study the phase transition of the strongly correlated Hofstadter spectrum.
引用
收藏
页数:7
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