4.8 Article

Gate-Tunable Topological Flat Bands in Trilayer Graphene Boron-Nitride Moire Superlattices

期刊

PHYSICAL REVIEW LETTERS
卷 122, 期 1, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.122.016401

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资金

  1. National Research Foundation of Korea (NRF) - Ministry of Education [2018R1A6A1A06024977]
  2. Office of Science, Office of Basic Energy Sciences, Materials Sciences and Engineering Division of the U.S. Department of Energy [DE-AC02-05-CH11231]
  3. National Key Research Program of China [2016YFA0300703, 2018YFA0305600]
  4. NSF of China [U1732274, 11527805, 11425415, 11421404]
  5. Shanghai Municipal Science and Technology Commission [18JC1410300]
  6. Strategic Priority Research Program of the Chinese Academy of Sciences [XDB30000000]
  7. Samsung Science and Technology Foundation [SSTF-BA1802-06]
  8. [NRF-2016R1A2B4010105]
  9. [NRF-2017R1D1A1B03035932]
  10. National Research Foundation of Korea [2017R1D1A1B03035932, 2018R1A6A1A06024977] Funding Source: Korea Institute of Science & Technology Information (KISTI), National Science & Technology Information Service (NTIS)

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We investigate the electronic structure of the fiat bands induced by moire superlattices and electric fields in nearly aligned ABC trilayer graphene (TLG) boron-nitride (BN) interfaces where Coulomb effects can lead to correlated gapped phases. Our calculations indicate that valley-spin resolved isolated superlattice flat bands that carry a finite Chern number C = 3 proportional to the layer number can appear near charge neutrality for appropriate perpendicular electric fields and twist angles. When the degeneracy of the bands is lifted by Coulomb interactions, these topological bands can lead to anomalous quantum Hall phases that embody orbital and spin magnetism. Narrow bandwidths of similar to 10 meV achievable for a continuous range of twist angles theta less than or similar to 0.6 degrees with moderate interlayer potential differences of similar to 50 meV make the TLG-BN systems a promising platform for the study of electric-field tunable Coulomb-interaction-driven spontaneous Hall phases.

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