Abstract
Topological flat bands formed in two-dimensional lattice systems offer an opportunity to study fractional phases of matter in the absence of an external magnetic field. Examples include fractional quantum anomalous Hall effects and fractional topological insulators. Recently, fractional quantum anomalous Hall effects have been experimentally realized in both twisted bilayer MoTe2 and rhombohedral-stacked multilayer graphene on hexagonal boron nitride. These studies focus mainly on the first moiré flat band, but there is a possibility that non-Abelian states could occur in the second moiré band. Here we present a systematic transport study of twisted bilayer MoTe2 devices, focusing on the second moiré band. We observe ferromagnetism in the second moiré band, and a Chern insulator state driven by out-of-plane magnetic fields at a filling factor of three holes per moiré unit cell. Between fillings of 2.2 and 2.7 holes per moiré unit cell, we observe a finite temperature resistivity minimum with a 1/T scaling law at low temperatures and a large out-of-plane negative magnetoresistance. Applying an out-of-plane electric field can induce quantum phase transitions at both integer and fractional filling factors. Our studies lay the groundwork for realizing tunable topological states and other unexpected magnetic phases beyond the first moiré flat band based in twisted MoTe2.
| Original language | English |
|---|---|
| Pages (from-to) | 542-548 |
| Number of pages | 7 |
| Journal | Nature Physics |
| Volume | 21 |
| Issue number | 4 |
| DOIs | |
| State | Published - Apr 2025 |
Funding
We thank F. Wu, Z. Liu, X. Xu and M. Qin for helpful discussions. This work is supported by the National Key R&D Program of China (grant nos. 2022YFA1402702, 2022YFA1405400, 2021YFA1401400, 2021YFA1400100, 2022YFA1402404, 2019YFA0308600, 2022YFA1402400, 2020YFA0309000 and 2021YFA1202902), the National Natural Science Foundation of China (grant nos. 12350403, 92265102, 12174249, 12174250, 12141404, 12374045, 12374292 and 124B1030), the Innovation Program for Quantum Science and Technology (grant nos. 2021ZD0302600 and 2021ZD0302500), the Natural Science Foundation of Shanghai (grant nos. 24QA2703700, 22PJ1406700, 24LZ1401100 and 22ZR1430900). T.L., S.J. and X.L. acknowledge the Shanghai Jiao Tong University 2030 Initiative Program. T.L. and S.J. acknowledge the Yangyang Development Fund. N.M. acknowledges the financial support from the Alexander von Humboldt Foundation. Yixin Zhang and Yang Zhang acknowledge support from Max Planck partner lab grant for quantum materials. K.W. and T.T. acknowledge support from the JSPS KAKENHI (grant nos. 21H05233 and 23H02052) and World Premier International Research Center Initiative (WPI), MEXT, Japan. A portion of this work was carried out at the Synergetic Extreme Condition User Facility (SECUF, https://cstr.cn/31123.02.SECUF).