4.8 Article

Electrically tunable correlated and topological states in twisted monolayer-bilayer graphene

期刊

NATURE PHYSICS
卷 17, 期 3, 页码 374-+

出版社

NATURE RESEARCH
DOI: 10.1038/s41567-020-01062-6

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资金

  1. Programmable Quantum Materials, an Energy Frontier Research Center - US Department of Energy (DOE), Office of Science, Basic Energy Sciences (BES) [DE-SC0019443]
  2. NSF MRSEC [1719797]
  3. Army Research Office [W911NF-20-1-0211]
  4. Boeing Distinguished Professorship in Physics
  5. State of Washington
  6. NSF [DMR-1725221]
  7. Elemental Strategy Initiative by the MEXT, Japan [JPMXP0112101001]
  8. JSPS KAKENHI [JP20H00354]
  9. CREST, JST [JPMJCR15F3]

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Twisted monolayer-bilayer graphene (tMBG) systems exhibit various correlated metallic and insulating states, as well as topological magnetic states. The phase diagram of tMBG can be switched under different perpendicular electric fields, providing a tunable platform for investigating correlated and topological states.
Twisted van der Waals heterostructures with flat electronic bands have recently emerged as a platform for realizing correlated and topological states with a high degree of control and tunability. In graphene-based moire heterostructures, the correlated phase diagram and band topology depend on the number of graphene layers and the details of the external environment from the encapsulating crystals. Here, we report that the system of twisted monolayer-bilayer graphene (tMBG) hosts a variety of correlated metallic and insulating states, as well as topological magnetic states. Because of its low symmetry, the phase diagram of tMBG approximates that of twisted bilayer graphene when an applied perpendicular electric field points from the bilayer towards the monolayer graphene, or twisted double bilayer graphene when the field is reversed. In the former case, we observe correlated states that undergo an orbitally driven insulating transition above a critical perpendicular magnetic field. In the latter case, we observe the emergence of electrically tunable ferromagnetism at one-quarter filling of the conduction band, and an associated anomalous Hall effect. The direction of the magnetization can be switched by electrostatic doping at zero magnetic field. Our results establish tMBG as a tunable platform for investigating correlated and topological states.

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