Asymmetric Modulation on Exchange Field in a Graphene/BiFeO₃ Heterostructure by External Magnetic Field

Graphene, having all atoms on its surface, is favorable to extend the functions by introducing the spin–orbit coupling and magnetism through proximity effect. Here, we report the tunable interfacial exchange field produced by proximity coupling in graphene/BiFeO₃ heterostructures. The exchange field has a notable dependence with external magnetic field, and it is much larger under negative magnetic field than that under positive magnetic field. For negative external magnetic field, interfacial exchange coupling gives rise to evident spin splitting for <i>N</i> ≠ 0 Landau levels and a quantum Hall metal state for <i>N</i> = 0 Landau level. Our findings suggest graphene/BiFeO₃ heterostructures are promising for spintronics

Electronic Coupling between Graphene and Topological Insulator Induced Anomalous Magnetotransport Properties

It has been theoretically proposed that the spin textures of surface states in a topological insulator can be directly transferred to graphene by means of the proximity effect, which is very important for realizing a two-dimensional topological insulator based on graphene. Here we report the anomalous magnetotransport properties of graphene–topological insulator Bi₂Se₃ heterojunctions, which are sensitive to the electronic coupling between graphene and the topological surface state. The coupling between the p_<i>z</i> orbitals of graphene and the p orbitals of the surface states on the Bi₂Se₃ bottom surface can be enhanced by applying a perpendicular negative magnetic field, resulting in a giant negative magnetoresistance at the Dirac point up to about −91%. An obvious resistance dip in the transfer curve at the Dirac point is also observed in the hybrid devices, which is consistent with theoretical predictions of the distorted Dirac bands with nontrivial spin textures inherited from the Bi₂Se₃ surface states