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Trapped Ion Quantum Computing
Reentrant Flat Bands with Nontrivial Topology and Electronic Correlations in Artificial Rhombohedral Trilayer Graphene.
PubMed
Authors: Li SY, Jiang J, Wang Z, Wang Y, Han Y, Li M, Hu J, Zhang Y, Watanabe K, Taniguchi T, Gao HJ, Jiang Y, Mao J
Year
2026
Paper ID
10258
Status
Peer-reviewed
Abstract Read
~2 min
Abstract Words
185
Citations
N/A
Abstract
Rhombohedral trilayer graphene provides a platform for exploring exotic quantum phases arising from the interplay of electron correlations and band topology. The development of strategies to engineer rhombohedral trilayer graphene with flat bands is important for both fundamental studies of correlated topological states and potential device applications. Here, we demonstrate that a slight rotation of monolayer graphene relative to a bilayer offers an effective approach to achieving this goal. In minimally twisted monolayer-bilayer graphene (mtMBG), significant structural relaxation gives rise to stable, large-scale ABA and ABC domain arrays. When the twist angle falls below a critical threshold, the ABC regions exhibit electronic properties akin to those of rhombohedral trilayer graphene, featuring robust and spatially uniform flat bands with tunable layer polarization. At partial filling, the conduction flat band progressively splits into four sub-bands, driven by electron-electron interactions and indicative of quantum phase transitions between correlated states. Moreover, spectroscopic signatures of electronic polarization and topological edge states at the domain walls separating the ABA and ABC regions are observed. These results establish mtMBG as a versatile platform for investigating emergent flat-band phenomena and related electronic states.
Why This Paper Matters
- This paper contributes to the Trapped-Ion Quantum Computing research area in the Quantum Articles archive.
- It adds a 2026 reference point for readers tracking recent quantum research.
- Rhombohedral trilayer graphene provides a platform for exploring exotic quantum phases arising from the interplay of electron correlations and band topology.
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