/ 31Graphene and surface states of topological insulators (TIs) can be described by two-dimensional (2D) massless Dirac Hamiltonian at the low energy excitations, which can be further modulated by adatom adsorption or interfacing with other functional materials [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15]. Owing to the high carrier mobility and unique spin textures, TIs and graphene are promising for high speed electronics and spintronics [16]. Recent theories [8][9][10][11] have predicted the hybridization of graphene and TIs can create nontrivial spin textures in graphene, even leading to quantum spin Hall states [1]. Generally, the rigorous √3 × √3 supercell of graphene stacked with TI is adopted in the calculations [8][9][10][11]. For the incommensurate graphene-TI stacking,Zhang et al. [10] suggested that the renormalized bands of hybrid graphene still acquire the in-plane spin textures from the surface states of TI even in the presence of surface roughness at the heterointerface. The coupling between graphene and TI has been pursued via the angle resolved photoemission spectroscopy (ARPES) Gate-tunable conductivity of the hybrid device is shown in Fig. 1b These observations can be understood in the framework of the graphene-TI proximity effect that was theoretically predicted via band calculations in Refs. [8][9][10][11]. Under the magnetic field perpendicular to the graphene plane, the unevenly spaced energy spectrum is expressed as = ( )√2 ℏ 2 | | , where ℏ is reduced Planck's constant, the Fermi velocity is ~10 6 ⁄ , and the LL index N is positive for electrons and negative for holes [12,13]. The half-filled LLs, such as N = −3, −2, Fig. 3). We should realize that the possible coupling between graphene and TI surface states is the second (or higher) order effect [8][9][10][11]. The hopping process between the orbitals of carbon atoms in graphene and orbitals of the bottom surface states in Bi 2 Se 3 nanoribbons introduces significant influences on the transport properties in graphene near the Dirac point.Anomalous magnetotransport features at Dirac point. Now we discuss the magnetotransport at the Dirac point (or the zeroth LL) in the graphene hybrid device.The evolution of ( * ) curves near the Dirac point at various temperatures andunder negative magnetic fields is shown in Fig. 3a (see Supplementary Fig. 4 for the evolution of ( * )). The curves are shifted for clarity. The resistivity at the Dirac point ( ) versus B is extracted and shown in Fig. 3b,c. In the classical regime, the two-carrier model can be used to describe a zero-gap conductor with the same mobility for electrons and holes, giving Predicted by theoretical models [8][9][10][11], graphene can inherit spin-orbital textures from TI surface states near the Dirac point due to the proximity effect. Accordingly, we summarize the reforming band structures of graphene hybridized with TI surface in Fig. 4. As the interaction between graphene and TI is significant, the fourfold degeneracy of the original graphene bands (Fig. 4a) is par...