Sharpe Aaron L, Fox Eli J, Barnard Arthur W, Finney Joe, Watanabe Kenji, Taniguchi Takashi, Kastner Marc A, Goldhaber-Gordon David
Department of Applied Physics, Stanford University, 348 Via Pueblo Mall, Stanford, California 94305, United States.
Stanford Institute for Materials and Energy Science, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, United States.
Nano Lett. 2021 May 26;21(10):4299-4304. doi: 10.1021/acs.nanolett.1c00696. Epub 2021 May 10.
We have previously reported ferromagnetism evinced by a large hysteretic anomalous Hall effect in twisted bilayer graphene (tBLG). Subsequent measurements of a quantized Hall resistance and small longitudinal resistance confirmed that this magnetic state is a Chern insulator. Here, we report that when tilting the sample in an external magnetic field, the ferromagnetism is highly anisotropic. Because spin-orbit coupling is weak in graphene, such anisotropy is unlikely to come from spin but rather favors theories in which the ferromagnetism is orbital. We know of no other case in which ferromagnetism has a purely orbital origin. For an applied in-plane field larger than 5 T, the out-of-plane magnetization is destroyed, suggesting a transition to a new phase.
我们之前报道过,扭曲双层石墨烯(tBLG)中存在由大滞后反常霍尔效应所表现出的铁磁性。随后对量子化霍尔电阻和小纵向电阻的测量证实,这种磁态是一种陈绝缘体。在此,我们报道,当在外部磁场中倾斜样品时,铁磁性具有高度各向异性。由于石墨烯中的自旋 - 轨道耦合较弱,这种各向异性不太可能源于自旋,而更倾向于铁磁性是轨道性的理论。我们不知道还有其他铁磁性纯粹源于轨道的情况。对于大于5 T的面内施加磁场,面外磁化被破坏,这表明向一个新相发生了转变。