Xu Yang, Ray Ariana, Shao Yu-Tsun, Jiang Shengwei, Lee Kihong, Weber Daniel, Goldberger Joshua E, Watanabe Kenji, Taniguchi Takashi, Muller David A, Mak Kin Fai, Shan Jie
School of Applied and Engineering Physics, Cornell University, Ithaca, NY, USA.
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
Nat Nanotechnol. 2022 Feb;17(2):143-147. doi: 10.1038/s41565-021-01014-y. Epub 2021 Nov 29.
Moiré engineering of van der Waals magnetic materials can yield new magnetic ground states via competing interactions in moiré superlattices. Theory predicts a suite of interesting phenomena, including multiflavour magnetic states, non-collinear magnetic states, moiré magnon bands and magnon networks in twisted bilayer magnetic crystals, but so far such non-trivial magnetic ground states have not emerged experimentally. Here, by utilizing the stacking-dependent interlayer exchange interactions in two-dimensional magnetic materials, we demonstrate a coexisting ferromagnetic (FM) and antiferromagnetic (AF) ground state in small-twist-angle CrI bilayers. The FM-AF state transitions to a collinear FM ground state above a critical twist angle of about 3°. The coexisting FM and AF domains result from a competition between the interlayer AF coupling, which emerges in the monoclinic stacking regions of the moiré superlattice, and the energy cost for forming FM-AF domain walls. Our observations are consistent with the emergence of a non-collinear magnetic ground state with FM and AF domains on the moiré length scale. We further employ the doping dependence of the interlayer AF interaction to control the FM-AF state by electrically gating a bilayer sample. These experiments highlight the potential to create complex magnetic ground states in twisted bilayer magnetic crystals, and may find application in future gate-voltage-controllable high-density magnetic memory storage.
范德华磁性材料的莫尔工程可以通过莫尔超晶格中的竞争相互作用产生新的磁性基态。理论预测了一系列有趣的现象,包括多味磁态、非共线磁态、莫尔磁振子能带以及扭曲双层磁性晶体中的磁振子网络,但迄今为止,这种非平凡的磁性基态尚未在实验中出现。在这里,通过利用二维磁性材料中依赖于堆叠的层间交换相互作用,我们在小扭曲角的CrI双层中展示了一种共存的铁磁(FM)和反铁磁(AF)基态。在约3°的临界扭曲角以上,FM - AF态转变为共线FM基态。共存的FM和AF畴是由莫尔超晶格单斜堆叠区域中出现的层间AF耦合与形成FM - AF畴壁的能量成本之间的竞争导致的。我们的观察结果与在莫尔长度尺度上出现具有FM和AF畴的非共线磁性基态一致。我们还利用层间AF相互作用的掺杂依赖性,通过对双层样品进行电门控来控制FM - AF态。这些实验突出了在扭曲双层磁性晶体中创造复杂磁性基态的潜力,并可能在未来的栅极电压可控高密度磁存储中得到应用。