Strong interfacial charge transfer from CrSBr induces extreme hole doping and quantum-Hall states in graphene heterostructures
Ziqi Liu , Yuchen Gao , Chengfeng Zhu , Yichang Sun , Kenji Watanabe , Takashi Taniguchi , Zuxin Chen , Pingfan Gu , Yu Ye
InfoScience ›› 2026, Vol. 3 ›› Issue (1) : e70007
Magnetic van der Waals (vdW) semiconductors offer unique opportunities to integrate spin and charge degrees of freedom in atomically thin devices. Here, we fabricate dual-gated heterostructures consisting of exfoliated CrSBr, stacked beneath monolayer graphene and encapsulated by hexagonal boron nitride (h-BN). Magnetotransport measurements performed at temperatures down to 2 K and magnetic fields up to 13.5 T demonstrate that CrSBr acts as an exceptionally strong p-type doping source to graphene in this vdW heterostructure, driving the graphene Fermi level deep into the valence band with hole density reaching ~1013 cm−2. High-frequency Shubnikov-de Haas oscillations and well-quantized quantum Hall plateaus were observed, confirming the high quality of the doped graphene channel. Furthermore, nearly field-independent resistance ridges emerged at a top gate bias of ≈ −3 V, which we attribute to graphene/h-BN moiré minibands with a twist angle of >3°. These miniband features become experimentally accessible solely due to the extreme p-doping by CrSBr, a regime that is inaccessible via conventional gating techniques.
2d materials / heterostructure / moirésuperlattices / p-doping / quantum Hall effects
| [1] |
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| [2] |
|
| [3] |
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| [4] |
|
| [5] |
|
| [6] |
|
| [7] |
|
| [8] |
|
| [9] |
|
| [10] |
|
| [11] |
|
| [12] |
|
| [13] |
|
| [14] |
|
| [15] |
|
| [16] |
|
| [17] |
|
| [18] |
|
| [19] |
|
| [20] |
|
| [21] |
|
| [22] |
|
| [23] |
|
| [24] |
|
| [25] |
|
| [26] |
|
| [27] |
|
| [28] |
|
| [29] |
|
| [30] |
|
| [31] |
|
| [32] |
|
| [33] |
|
| [34] |
|
| [35] |
|
| [36] |
|
| [37] |
|
| [38] |
|
| [39] |
|
| [40] |
|
2025 The Author(s). InfoScience published by UESTC and John Wiley & Sons Australia, Ltd.
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