Phase diagram and orbital Chern insulator in twisted double bilayer graphene
arXiv:2103.01429 · doi:10.1103/PhysRevB.103.115201
Abstract
Compared with twisted bilayer graphene, twisted double bilayer graphene (TDBG) provides another important platform to realize the moiré flat bands. In this paper, we first calculate the valley Chern number phase diagram of TDBG in the parameter space spanned by the twist angle and the interlayer electric potential. To include the effects of interactions, we then phenomenologically introduce the spin-splitting and valley-splitting. We find that when the valley splitting is larger than the bandwidth of the first conduction band so that a gap is opened and the spin splitting is relatively weak, the orbital Chern insulator emerges at half-filling, associated with a large orbital magnetization (OM). Further calculations suggest that there is no sign reversal of the OM when the Fermi energy goes from the bottom to the top of the half-filling gap, as the OM remains negative in both AB-AB stacking and AB-BA stacking. The implications of our results for the ongoing experiments are also discussed.
12 pages, 9 figures
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Cited by in corpus (10)
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- Exact Many-Body Ground States from Decomposition of Ideal Higher Chern Bands: Applications to Chirally Twisted Graphene Multilayers
- Nonlinear anomalous Hall effects probe topological phase-transitions in twisted double bilayer graphene
- Tailoring the band structure of twisted double bilayer graphene with pressure
- Narrow bands, electrostatic interactions and band topology in graphene stacks
- Perpendicular electric field drives Chern transitions and layer polarization changes in Hofstadter bands
- High-Chern number phase in the topological insulator multilayer structures
- Absence of Edge States in The Valley Chern Insulator in Moiré Graphene
- Unconventional Metallic Magnetism: Non-analyticity and Sign-changing Behavior of Orbital Magnetization in ABC Trilayer Graphene
- Analogue of atomic collapse for adatoms on rhombohedral multilayer graphene