Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
Francis Bitter Magnet Laboratory, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
Nat Commun. 2016 Jun 27;7:12014. doi: 10.1038/ncomms12014.
When a topological insulator (TI) is in contact with a ferromagnet, both time-reversal and inversion symmetries are broken at the interface. An energy gap is formed at the TI surface, and its electrons gain a net magnetic moment through short-range exchange interactions. Magnetic TIs can host various exotic quantum phenomena, such as massive Dirac fermions, Majorana fermions, the quantum anomalous Hall effect and chiral edge currents along the domain boundaries. However, selective measurement of induced magnetism at the buried interface has remained a challenge. Using magnetic second-harmonic generation, we directly probe both the in-plane and out-of-plane magnetizations induced at the interface between the ferromagnetic insulator (FMI) EuS and the three-dimensional TI Bi2Se3. Our findings not only allow characterizing magnetism at the TI-FMI interface but also lay the groundwork for imaging magnetic domains and domain boundaries at the magnetic TI surfaces.
当拓扑绝缘体(TI)与铁磁体接触时,界面处的时间反演和反转对称性都被破坏。在 TI 表面形成能隙,其电子通过短程交换相互作用获得净磁矩。磁性 TI 可以容纳各种奇异的量子现象,如质量狄拉克费米子、马约拉纳费米子、量子反常霍尔效应和畴界上的手性边缘电流。然而,对埋层界面感应磁的选择性测量仍然是一个挑战。我们使用磁二次谐波产生,直接探测在铁磁绝缘体(FMI)EuS 和三维 TI Bi2Se3 之间界面诱导的面内和面外磁化。我们的发现不仅允许对 TI-FMI 界面的磁化进行特征描述,也为在磁性 TI 表面成像磁畴和畴界奠定了基础。