Using first-principles electronic structure calculations, we predict half-fluorinated GaBi honeycomb under tensile strain to harbor a quantum anomalous Hall (QAH) insulator phase. We show that this QAH phase is driven by a single inversion in the band structure at the Γ point. Moreover, we have computed the electronic spectrum of a half-fluorinated GaBi nanoribbon with zigzag edges, which shows that only one edge band crosses the Fermi level within the band gap. Our results suggest that half-fluorination of the GaBi honeycomb under tensile strain could provide a new platform for developing novel spintronics devices based on the QAH effect.
Topological materials are attracting intense current interest in search of new materials platforms for energy-efficient device applications1,2,3,4,5. These include two-dimensional (2D) topological insulators (TIs), also called quantum spin Hall (QSH) insulators3,6,7, topological superconductors2, topological crystalline insulators (TCIs)8,9, and quantum anomalous Hall (QAH)5,10 insulators, among others. At the heart of these developments is the discovery of the quantum Hall effect, which led to the realization of the topological nature of the underlying electronic structures and the associated dissipationless spin-transport around the edges of a 2D insulator under a strong magnetic field11,12.
QAH effect is similar to the quantum Hall effect except that in the case of the QAH the driving magnetic field is generated internally in the material through spin-orbit coupling (SOC), while in the more conventional quantum Hall case the magnetic field is applied externally13. The existence of a QAH insulator phase was first inferred via an analysis of a tight-binding model on a honeycomb lattice14,15, where the Hall conductance was found to be quantized even in the absence of an external magnetic field16. The natural place to search for materials realization of the QAH phase is a ferromagnetic insulator with a topologically non-trivial band structure17,18,19. A strong enough magnetization in the QSH phase could then perhaps drive the material into the QAH phase17.
QAH effect was first realized in magnetically doped TI thin films13,18,20,21,22,23,24, and has been the subject of extensive theoretical studies19,25,26,27. In principle, we might expect the QAH effect to be more robust compared to the QSH effect where one needs to be in the submicron regime in order to prevent spin-flip scattering17. Notably, quantization can be achieved even at low mobility17,21. In any event, the fact remains that the presently available QAH materials are constrained to very low temperatures and are based on magnetic doping of thin TI films. There is great need thus to find new QAH materials based on non-magnetic thin films, which would be viable for room temperature applications.
Several thin films of elements of groups IV28,29 and V30,31,32, which have been predicted to be QSH insulators, have also been predicted to harbor the QAH phase33,34,35,36. In contrast, even though a number of alloys of elements of groups III and V have been predicted to support QSH phases37,38,39,40,41 in freestanding37 and functionalized forms38,40,41, the possible existence of QAH phases in these alloys has, to our knowledge, not been explored.
With this motivation, here we examine the possible presence of QAH phases in thin films of GaBi III-V honeycombs using first-principles calculations, including effects of half-fluorination of the films. The Chern numbers in a number of cases are computed to show that the films support the QAH phase over a reasonable range of lattice constant values. We further confirm our results by computing edge states for fluorinated GaBi nanoribbons. Our results imply that on a suitable substrate, which will induce the appropriate tensile strain, the GaBi III-V films could provide a new materials platform for applications based on the QAH effect.
Figure 1(a,b) show the top views of the 2D crystal structure of our GaBi honeycomb with fluorine atoms adsorbed on Bi and Ga layer, respectively. Figure 1(c) shows the side view of the fully-fluorinated GaBi. For half-fluorinations, F atoms can be adsorbed either on Bi (denoted by GaBi-F) or on Ga (denoted by BiGa-F). The side-views of different fluorinations of GaBi are shown in Fig. 1(d–i). There are three types of possible configurations: planar (PL), buckled (BK), and inversely buckled (IBK) honeycomb. Here, BK [(e) & (h)] refers to cases where the adsorbed F atom retains the buckling of the original un-passivated GaBi structure37,38, while IBK [(f) & (i)] refers to the case in which the buckled honeycomb is inverted after half-passivation.
The computed total energies in Fig. 2 show that half-fluorination of Ga atoms is energetically more favorable than that of Bi atoms. For half-fluorination of Ga, the inversely buckled honeycomb is seen in Fig. 2 to transform into the buckled honeycomb as the lattice constant is increased. In sharp contrast, half-fluorination of Bi, transforms the buckled honeycomb into the inversely buckled honeycomb. By tracking evolution of the band structure and computing the corresponding Chern numbers as a function of strain, we can identify the emergence of topological phases in these films. The resulting phase diagram for half-fluorination on Ga (labeled as BiGa-F) is shown in Fig. 2(a). For the planar case, we obtain a QAH semi-metal for lattice constant (a) values below 4.70 Å. PL then yields a QAH insulator between a = 4.70 to 5.325 Å and, eventually turns into a trivial insulator above a = 5.325 Å. As for the buckled structure, it is a trivial insulator over the range a = 4.80–5.26 Å, but it becomes a QAH insulator for a = 5.26 to 5.50 Å. The inversely buckled honeycomb (red squares in Fig. 2(a)) is very unstable and transforms into the buckled honeycomb beyond a = 4.5 Å. On the other hand, for F adsorbed on Bi atoms, shown in Fig. 2(b), (labeled as GaBi-F), we obtain a metallic state for all configurations. For this reason, for the remainder of this study, we will focus on films with half-fluorination of Ga. Notably, we also find QAH phases for half-hydrogenation and half-halogenation with Cl or Br on Ga (see Figs S1 and S6 in the Supplementary Information).
In order to understand the role of buckling in driving the topological phase transition, we consider in Fig. 2 how the band structure of the film with fixed a = 4.80 Å evolves as the buckling distance, δ, is decreased from 0.72 Å until the structure becomes planar. The band gap is seen to close at δ = 0.15 Å as, see Fig. 2(e). By plotting the px-orbital contributions (green circles), we can differentiate between the trivial band gap in Fig. 2(c,d) and the inverted band gap in Fig. 2(f). We will return below to show that the Berry curvature near the inverted band gap region assumes large values, yielding a Chern number of −1. For the three aforementioned crystal structures, the topological phase transitions due to strains in the PL, BK and IBK structures are further discussed in Figs S2–S4 in Supplementary Information. In particular, Fig. S3 demonstrates the transition from an insulator to a QAH insulator in the buckled BiGa-F with a critical point at a = 5.26 Å. In Fig. S4, the planar honeycomb is seen to go from a QAH semi-metal to a QAH insulator, and to then transition from a QAH insulator to a trivial insulator with increasing lattice constant. In short, for the half-fluorinated and planar GaBi films, we obtain a stable QAH phase over a reasonable range of lattice constants from 4.7 Å to 5.325 Å. Notably, the BiGa-F film at a = 4.80 Å exhibits a band gap of 56 meV, but this gap value increases to 105 meV at a = 5.50 Å, which is large enough for realizing the QAH phase above room-temperature.
Recent first-principles studies have shown that freestanding37 and functionalized GaBi38,40 non-magnetic films can support a robust QSH insulator phase. Half-fluorination or half-hydrogenation of GaBi on Ga (BiGa-F) leads to an intrinsic magnetization strong enough to drive the film into the QAH phase. In this connection, band structures of fluorinated GaBi films in a planar honeycomb are presented in Fig. 3. Fully-fluorinated GaBi (a = 4.80 Å) without and with SOC are considered in Fig. 3(a,d), respectively. Fully-fluorinated GaBi is gapless without SOC, but adding SOC in the calculations is seen to open a bulk band gap of ~0.77 eV; we have verified that the film exhibits a QSH phase with Z2 = 1. At the equilibrium lattice constant of half-fluorinated planar GaBi (4.80 Å), without SOC, we found the magnetic ground state in the spin-polarized calculations [Fig. 3(c)] to have a lower energy than the nonmagnetic state [Fig. 3(b)]. However, when the SOC was turned on in spin-polarized calculations [Fig. 3(e)], we obtained the QAH phase. Note that in Fig. 3(c,e), the spin-up and spin-down polarized states are marked with red and blue lines/circles, respectively.
Our non-spin-polarized band calculations without the SOC [Fig. 3(b)] show that the material is a zero-gap metal with degenerate states at the Fermi energy at Γ. When spin-polarization is included in the computations [Fig. 3(c)], the exchange field causes the electronic spectrum to split into two sets of bands with different spin polarizations with an intrinsic magnetization of approximately 0.7 μB per unit cell with co-existing gapped spin-up and gapless spin-down dispersions; the spin-down bands continue to be degenerate at Γ. Note that the px-orbitals (green circles) around Γ of the spin-down bands have become inverted compared to the corresponding bands in Fig. 3(a). Furthermore, the inclusion of SOC leads to an insulating state with a gap (~56 meV), see Fig. 3(e). We thus realize the QAH phase via a px-orbital inversion in the spin-up band in the presence of an SOC induced band gap. Further plots of px,y-orbital contributions are provided in Fig. S4 of the Supplementary Information.
We have considered effects of half-halogenations of the planar GaBi honeycomb using other elements of the halogen group (Cl, Br, and I). Like F and H atoms, we found more generally that half-halogenations all prefer to adsorb on Ga atoms. At their equilibrium lattice constants both half-chlorinated and half-brominated films are in the QAH phase, whereas half-iodinated films are trivial, although the QAH phase can be induced in half-iodinated films under a compressive strain. Detailed band structures of the halogenated films are given in Fig. S6 of the Supplementary Information.
We turn next to discuss the nature of edge states of GaBi nanoribbons. For this purpose, we use a tight-binding Hamiltonian, which is parameterized via Wannier functions, and as Fig. 4(a) shows, our tight-binding model reproduces the first-principles band structure quite well. The Berry curvature of the half-fluorinated GaBi film at a lattice constant of 4.80 Å along a few symmetry directions in the Brillouin zone (BZ) is shown in Fig. 4(b). The value of the Berry curvature is seen to be large around the band inversion region near the Γ point, and when this curvature is integrated over the first BZ, it yields a Chern number of −1 as expected. Chern number is an important quantity for monitoring the QAH effect because the Hall conductivity is proportional to the Chern number. In order to further insight into the nature of the QAH edge state in the half-fluorinated GaBi film as compared to the QSH edge states in a fully-fluorinated GaBi film, we constructed a nanoribbon with zigzag edge as shown in Fig. 4(e). Using our tight-binding model Hamiltonian to calculate the edge states, results for the fully-fluorinated and half-fluorinated nanoribbons are given in Fig. 4. The sizes of blue and red circles are proportional to the contributions of left and right hand side zigzag edges, respectively. Figure 4(c) shows the electronic structure of the fully-fluorinated QSH nanoribbon. The plot exhibits an odd number of band crossings with the Fermi level between π/a and Γ38 and the related time-reversed partners −π/a and Γ, and thus establishes clearly the existence of helical edge states. In Fig. 4(d), on the other hand, for each side of the half-fluorinated nanoribbon edge, we can see that there is only one chiral edge state connecting the conduction and valence bands, which lies in the middle of the band gap. Note that the number of chiral edge state gives the the absolute value of the Chern number.
In order to assess the robustness of our calculations to the underestimation of the band gap within the GGA, we have computed electronic structures and Berry curvatures of our fully-fluorinated as well as half-fluorinated GaBi films using the hybrid functional HSE0642. We find that our GGA-based results in Fig. 2 correctly capture the evolution of the topological phases with strain, some differences in the exact values of the strain at which various phase transitions occur for different exchange-correlation functionals notwithstanding.
Regarding experimental realization, our predicted half-passivated III-V honeycombs could be realized by growing these honeycombs on a suitable substrate. A recent study33 has shown that half-iodinated stanene could be realized in stanene grown on CdTe. In addition, one study43 SiC-H utilized ultra-high purity hydrogen etching to modify SiC(0001) into H-passivated SiC which is equivalent to half-hydrogenation, and might be appropriate for half-halogenations more generally. Studies toward realizing GaBi films via Bi-doped GaAs44, and related works attempting honeycomb-like InBi on Si(111)45, has been also reported. Most recently, another study46 explored the growth of TlBi film by depositing Bi on Tl-covered Si(111) surface for which a variety of different surface reconstructions such as, and 4 × 4 for Tl0.75Bi0.25 and Tl0.632Bi0.368, respectively, were observed. Our study demonstrates the tunability of the half-halogenated/half-hydrogenated III-V films, which implies a suitable substrate could induce the QAH phase in these III-V films.
Summary and Conclusions
We have presented an ab initio study of the electronic and topological properties of GaBi films functionalized through hydrogenation/halogenation. The presence of a QAH insulator phase is predicted in half-fluorinated GaBi honeycomb under tensile strain. This QAH phase is driven by a single inversion in the band structure at the Γ point. Our computations on a half-fluorinated GaBi nanoribbon with zigzag edges reveal that the edge state spectrum consists of a single chiral band crossing the Fermi level within the band gap. Our study suggests that half-fluorinated GaBi honeycombs could provide a new materials platform for exploiting the QAH effect in spintronics applications.
Our first-principles calculations were performed within the framework of the density functional theory (DFT) utilizing the generalized gradient approximation (GGA)47,48,49,50,51. Projector-augmented-wave (PAW)52 wave functions with energy cut-offs of 300 and 400 eV for hydrogenation and fluorination, respectively, were used in the Vienna Ab-Initio Simulation Package (VASP)53,54. Atomic positions were optimized for each lattice constant value considered until the residual forces were no greater than 10−3 eV/Å. Convergence criterion for self-consistency in electronic structure computations was set at 10−6 eV. A vacuum layer of at least 30 Å along the z direction was used to simulate thin films. A Γ-centered Monkhorst-Pack55 grid of 12 × 12 × 1 was used for 2D integrations in the Brillouin zone. Berry curvatures and edge states were calculated based on an effective tight-binding Hamiltonian obtained by using maximally-localized Wannier functions via the WANNIER90 package56. In connection with topological properties, Chern number C were computed for various cases using15,25,57:
How to cite this article: Chen, S.-P. et al. Prediction of Quantum Anomalous Hall Insulator in half-fluorinated GaBi Honeycomb. Sci. Rep. 6, 31317; doi: 10.1038/srep31317 (2016).
F.-C.C. acknowledges support from the National Center for Theoretical Sciences and the Ministry of Science and Technology of Taiwan under Grants Nos MOST-104-2112-M-110-002-MY3 and MOST-103-2112-M-110-008-MY3. He is also grateful to the National Center for High-performance Computing for computer time and facilities. The work at Northeastern University was supported by the US Department of Energy (DOE), Office of Science, Basic Energy Sciences grant number DE-FG02-07ER46352 (core research), and benefited from Northeastern University’s Advanced Scientific Computation Center (ASCC), the NERSC supercomputing center through DOE grant number DE-AC02-05CH11231, and support (applications to layered materials) from the DOE EFRC: Center for the Computational Design of Functional Layered Materials (CCDM) under DE-SC0012575. H.L. acknowledge the Singapore National Research Foundation for support under NRF Award No. NRF-NRFF2013-03.