Abstract
Topological insulators (TIs) are quantum materials with insulating bulk and topologically protected metallic surfaces with Diraclike band structure. The most challenging problem faced by current investigations of these materials is to establish the existence of significant bulk conduction. Here we show how the band structure of topological insulators can be engineered by molecular beam epitaxy growth of (Bi_{1−x}Sb_{x})_{2}Te_{3} ternary compounds. The topological surface states are shown to exist over the entire composition range of (Bi_{1−x}Sb_{x})_{2}Te_{3}, indicating the robustness of bulk Z_{2} topology. Most remarkably, the band engineering leads to ideal TIs with truly insulating bulk and tunable surface states across the Dirac point that behaves like onequarter of graphene. This work demonstrates a new route to achieving intrinsic quantum transport of the topological surface states and designing conceptually new topologically insulating devices based on wellestablished semiconductor technology.
Introduction
The topological surface states of threedimensional topological insulators (TIs) possess a single spinpolarized Dirac cone originated from strong spin–orbit coupling^{1,2,3}. The unique surface states are expected to host exotic topological quantum effects^{4,5,6}, and find applications in spintronics and quantum computation. The experimental realization of these ideas requires fabrication of versatile devices based on bulkinsulating TIs with tunable surface states. However, the currently available TI materials exemplified by Bi_{2}Se_{3} and Bi_{2}Te_{3} (ref. 7) always show conductive bulk states due to the defectinduced charge carriers. Tuning the band structure of the TIs to eliminate the bulk states is one of the most urgent tasks in the field, but the problem remains unsolved despite extensive efforts involving nanostructuring^{8}, chemical doping^{9,10,11,12,13,14,15} and electrical gating^{16,17,18,19}.
Energy band engineering in conventional semiconductor is a powerful approach for tailoring the electronic structure of materials^{20}. A notable example is the isostructural isovalent alloy of the III–V semiconductors Al_{x}Ga_{1−x} as grown on GaAs by molecular beam epitaxy (MBE), in which the energy gap can be tuned continuously by the mixing ratio of AlAs and GaAs. Such energy band tuning has been essential for heterostructures, which were later used for discovery of fractional quantum Hall effect and invention of highspeed electronics.
Inspired by this idea, we conceived a new route for engineering the band structure of TIs by fabricating alloys of Bi_{2}Te_{3} and Sb_{2}Te_{3}. Both TIs are V–VI compounds with the same crystal structure and close lattice constants^{7}, making it ideal to form (Bi_{1−x}Sb_{x})_{2}Te_{3} ternary compounds with arbitrary mixing ratio and negligible strain (Fig. 1a). The potential advantages of mixing the two TIs can be anticipated from their complementary electronic properties. Figure 1b illustrates the band structure of pure Bi_{2}Te_{3} (refs 7,10,21), which reveals two major drawbacks of the surface Dirac band in Bi_{2}Te_{3}. First, the Dirac point (DP) is buried in the bulk valence band (BVB), hence, cannot be accessed by transport experiment and, more seriously, the Fermi level (E_{F}) lies in the bulk conduction band (BCB) due to the electrontype bulk carriers induced by Te vacancies. On the other hand, the band structure of pure Sb_{2}Te_{3} (refs 7,21), is drastically different. As shown schematically in Figure 1c, here the DP lies within the bulk gap and the E_{F} lies in the BVB due to the holetype bulk carriers induced by Sb–Te antisite defects. Intuitively, by mixing the two compounds one can simultaneously achieve charge compensation and tune the position of the DP, which may lead eventually to an ideal TI with exposed DP and insulating bulk.
Here we report the band structure engineering in TIs by fabricating alloys of Bi_{2}Te_{3} and Sb_{2}Te_{3} using stateoftheart MBE. Transport and angleresolved photoemission spectroscopy (ARPES) measurements show that the band engineering technique allows us to achieve ideal TIs with truly insulating bulk. The surface states can be tuned systematically across the DP and the transport properties are consistent with that of a single spinpolarized Dirac cone.
Results
Sample structure
During the MBE growth of the (Bi_{1−x}Sb_{x})_{2}Te_{3} films, the growth rate is calibrated by a realtime reflection highenergyelectron diffraction intensity oscillation measured on the (00) diffraction. Supplementary Figure S1 shows a typical 1×1 reflection highenergyelectron diffraction pattern taken on a (Bi_{1−x}Sb_{x})_{2}Te_{3} film with five quintuple layers (QLs) thickness. The sharpness of the feature provides a clear evidence for the high quality of the sample. The five QL thickness is used for all (Bi_{1−x}Sb_{x})_{2}Te_{3} films studied in this work because in this ultrathin regime the surface states dominate charge transport, and meanwhile the films are thick enough that the top and bottom surfaces are completely decoupled. Further discussion about the film thickness issue can be found in the Supplementary Information.
Electronic structure
The electronic structures of the (Bi_{1−x}Sb_{x})_{2}Te_{3} films are measured by ARPES on a sample setup as illustrated in Supplementary Figure S2. The ARPES band maps of eight (Bi_{1−x}Sb_{x})_{2}Te_{3} films with 0≤x≤1 are shown in Figure 2a to h. The pure Bi_{2}Te_{3} film shows welldefined surface states with massless Diraclike dispersion (Fig. 2a), similar to that of the cleaved Bi_{2}Te_{3} crystal^{10}. With the addition of Sb, the Diraclike topological surface states can be clearly observed in all (Bi_{1−x}Sb_{x})_{2}Te_{3} films from x=0 to 1, whereas the Dirac cone geometry changes systematically. With increasing x, the slope of the Dirac line shape becomes steeper, indicating an increase of the Dirac fermion velocity v_{D} defined by the linear dispersion ɛ=v_{D}·k near the DP. Meanwhile, the E_{F} moves downwards from the BCB, indicating the reduction of the electrontype bulk carriers. Moreover, the DP moves upwards relative to the BVB due to the increasing weight of the Sb_{2}Te_{3} band structure. When the Sb content is increased to x=0.88 (Fig. 2e), both the DP and E_{F} lie within the bulk energy gap. The system is now an ideal TI with a truly insulating bulk and a nearly symmetric surface Dirac cone with exposed DP. Notably, when x increases from x=0.94 (Fig. 2f) to 0.96 (Fig. 2(g), E_{F} moves from above the DP to below it, indicating a crossover from electron to holetype Dirac fermion gas. The charge neutrality point (CNP) where E_{F} meets DP can thus be identified to be located between x=0.94 and 0.96.
It is quite remarkable that the topological surface states exist in the entire composition range of (Bi_{1−x}Sb_{x})_{2}Te_{3}, which implies that the nontrivial Z_{2} topology of the bulk band is very robust against alloying. This is in contrast to the Bi_{1−x}Sb_{x} alloy, the first discovered threedimensional TI in which the topological surface states only exist within a narrow composition range near x=0.10 (refs 22,23). Figure 3a to c summarizes the characteristics of the surface Dirac band in the (Bi_{1−x}Sb_{x})_{2}Te_{3} compounds, which are extracted following the procedure presented in the Supplementary Information and illustrated in Supplementary Figures S3 and S4. The position of the DP rises continuously from below the top of BVB near the Γ point at x=0 to way above that at x=1 (Fig. 3a). This is accompanied by a drastic change of the relative position of E_{F} and DP (Fig. 3b), which determines the type and density of Dirac fermions. Furthermore, v_{D} increases from 3.3×10^{5} m s^{−1} at x=0 to 4.1×10^{5} m s^{−1} at x=1 (Fig. 3c). As the three defining properties of the Dirac cone are systematically varied between that of pure Bi_{2}Te_{3} and Sb_{2}Te_{3}, the (Bi_{1−x}Sb_{x})_{2}Te_{3} ternary compounds are effectively a series of new TIs. The bulk electronic structures, including the geometry of BCB and BVB as well as the energy gap between them, are also expected to change with x. They are of interests in their own rights, but will not be the main focus of the current work.
Transport properties
The systematic Dirac band evolution also manifests itself in the transport properties. Figure 4 displays the variation of twodimensional sheet resistance (R_{□}) with temperature (T) for eight QL (five) (Bi_{1−x}Sb_{x})_{2}Te_{3} films with 0≤x≤1. In pure Bi_{2}Te_{3} the resistance shows metallic behaviour at high T and becomes weakly insulating at very low T. With increasing x, the R_{□} value keeps rising and the insulating tendency becomes stronger, reflecting the depletion of electrontype bulk carriers and surface Dirac fermions. At x=0.94 when E_{F} lies just above DP, the resistance reaches the maximum value and shows insulating behaviour over the whole T range. With further increase of Sb content from x=0.96 to 1, the resistance decreases systematically because now E_{F} passes DP and more holetype carriers start to populate the surface Dirac band. The high T metallic behaviour is recovered in pure Sb_{2}Te_{3} when the holetype carrier density becomes sufficiently high.
Figure 5a displays the variation of the Hall resistance (R_{yx}) with magnetic field (H) measured on the five QL (Bi_{1−x}Sb_{x})_{2}Te_{3} films at T=1.5 K. For films with x≤0.94, the R_{yx} value is always negative, indicating the existence of electrontype carriers. The weakfield slope of the Hall curves, or the Hall coefficient R_{H}, increases systematically with x in this regime. As the twodimensional carrier density n_{2D} can be derived from R_{H} as n_{2D}=1/eR_{H} (e is the elementary charge), this trend confirms the decrease of electrontype carrier density with Sb doping. As x increases slightly from 0.94 to 0.96, the Hall curve suddenly jumps to the positive side with a very large slope, which indicates the reversal to holetype Dirac fermions with a small carrier density. At even higher x, the slope of the positive curves decreases systematically due to the increase of holetype carrier density.
The evolution of the Hall effect is totally consistent with the surface band structure revealed by ARPES in Figure 2. To make a more quantitative comparison between the two experiments, we use the n_{2D} derived from the Hall effect to estimate the Fermi wavevector k_{F} of the surface Dirac band. By assuming zero bulk contribution and an isotropic circular Dirac cone structure (Fig. 5b), k_{F} can be expressed as
Here D is the degeneracy of the Dirac fermion and is the carrier density per surface if we assume that the top and bottom surfaces are equivalent. Figure 5c shows that when we choose D=1, the k_{F} values derived from the Hall effect match very well with that directly measured by ARPES. This remarkable agreement suggests that the transport properties of the TI surfaces are consistent with that of a single spinpolarized Dirac cone, or a quarter of graphene, as expected by theory.
Figure 5d to f summarizes the evolution of the low T transport properties with Sb content x. The resistance value shows a maximum at x=0.94 with R_{□}> 10 kΩ and decreases systematically on both sides. Correspondingly, the carrier density n_{2D} reaches a minimum at x=0.96 with n_{2D}=1.4×10^{12} cm^{−2} and increases on both sides. Using the measured R_{□} and n_{2D}, the mobility μ of the Dirac fermions can be estimated by using the Drude formula σ_{2D}=n_{2D}eμ, where σ_{2D}=1/R_{□}. As a function of x the mobility also peaks near the CNP and decreases rapidly on both sides. The 'V'shaped dependence of the transport properties on the Sb content x clearly demonstrates the systematic tuning of the surface band structure across the CNP.
Discussion
The good agreement with ARPES suggests that the transport results are consistent with the properties of the surface Dirac fermions without bulk contribution. Moreover, the alloying allows us to approach the close vicinity of the CNP, which gives a very low n_{2D} in the order of 1×10^{12} cm^{−2}. The (Bi_{1−x}Sb_{x})_{2}Te_{3} compounds thus represent an ideal TI system to reach the extreme quantum regime because now a strong magnetic field can squeeze the Dirac fermions to the lowest few Landau levels. Indeed, the Hall resistance of the x=0.96 film shown in Figure 5a is close to 7 kΩ at 15 T, which is a significant fraction of the quantum resistance. Future transport measurements on (Bi_{1−x}Sb_{x})_{2}Te_{3} films with higher mobility to even stronger magnetic field hold great promises for uncovering the unconventional quantum Hall effect of the topological surface states^{24,25}.
The band structure engineering offers many enticing opportunities for designing conceptually new experimental or device schemes based on the TIs. For example, we can apply the idea of compositionally graded doping (CGD) in conventional semiconductor devices^{20} to the TIs to achieve spatially variable Dirac cone structures. Figure 6a illustrates the schematic of vertical CGD TIs, in which the top and bottom surfaces have opposite types of Dirac fermions and can be used for studying the proposed topological exciton condensation^{26}. The spatial asymmetry of the surface Dirac bands can also be used to realize the electrical control of spin current by using the spinmomentum locking in the topological surfaces for spintronic applications^{27}. Figure 6b illustrates the schematic of horizontal CGD TIs, by which a topological p–n junction between hole and electrontype TIs can be fabricated.
Methods
MBE sample growth
The MBE growth of TI films on insulating substrate has been reported before by the same group^{28}. The (Bi_{1−x}Sb_{x})_{2}Te_{3} films studied here are grown on sapphire (0001) in an ultrahigh vacuum MBEARPESSTM combined system with a base pressure of 1×10^{10} Torr. Before sample growth, the sapphire substrates are first degassed at 650 °C for 90 min and then heated at 850 °C for 30 min. Highpurity Bi (99.9999%), Sb (99.9999%) and Te (99.999%) are evaporated from standard Knudsen cells. To reduce Te vacancies, the growth is kept in Terich condition with the substrate temperature at 180 °C. The Bi:Sb ratio is controlled by the temperatures of the Bi and Sb Knudsen cells. The x value in the (Bi_{1−x}Sb_{x})_{2}Te_{3} film is determined through two independent methods, as discussed in detail in Supplementary Information.
ARPES measurements
The in situ ARPES measurements are carried out at room temperature by using a Scienta SES2002 electron energy analyser. A Helium discharge lamp with a photon energy of hν=21.218 eV is used as the photon source. The energy resolution of the electron energy analyser is set at 15 meV. All the spectra shown in the paper are taken along the KΓK direction. To avoid sample charging during ARPES measurements due to the insulating sapphire substrate, a 300nmthick titanium film is deposited at both ends of the substrate, which is connected to the sample holder. The sample is grounded through these contacts once a continuous film is formed. The sample setup for the ARPES measurements is illustrated schematically in the Supplementary Figure S2.
Transport measurements
The transport measurements are performed ex situ on the five QL (Bi_{1−x}Sb_{x})_{2}Te_{3} films grown on sapphire (0001) substrate. To avoid possible contamination of the TI films, a 20nm thick amorphous Te capping layer is deposited on top of the films before we take them out of the ultrahigh vaccum growth chamber for transport measurements. The Hall effect and resistance are measured using standard ac lockin method with the current flowing in the film plane and the magnetic field applied perpendicular to the plane. The schematic device setup for the transport measurements is shown in Supplementary Figure S5. The 20nm amorphous Te capping layer causes no significant change of the TI surface electronic structure and makes negligible contribution to the total transport signal, as shown in Supplementary Figure S6 and discussed in the Supplementary Information.
Additional information
How to cite this article: Zhang, J. et al. Band structure engineering in (Bi_{1−x}Sb_{x})_{2}Te_{3} ternary topological insulators. Nat. Commun. 2:574 doi: 10.1038/ncomms1588 (2011).
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Acknowledgements
We acknowledge S.C. Zhang and Y.B. Zhang for suggestions and comments. This work was supported by the National Natural Science Foundation of China, the Ministry of Science and Technology of China (grant number 2009CB929400) and the Chinese Academy of Sciences.
Author information
Author notes
 Jinsong Zhang
 & CuiZu Chang
These authors contributed equally to this work.
Affiliations
State Key Laboratory of Low Dimensional Quantum Physics, Department of Physics, Tsinghua University, Beijing 100084, People's Republic of China.
 Jinsong Zhang
 , CuiZu Chang
 , Zuocheng Zhang
 , Jing Wen
 , Minhao Liu
 , Xi Chen
 , QiKun Xue
 & Yayu Wang
Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China.
 CuiZu Chang
 , Xiao Feng
 , Kang Li
 , Ke He
 , Lili Wang
 , QiKun Xue
 & Xucun Ma
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Contributions
K.H., Y.W., X.C.M. and Q.K.X. designed the research. C.Z.C., J.W., X.F. and K.L. carried out the MBE growth of the samples and ARPES measurements. J.S.Z., Z.C.Z and M.H.L. carried out the transport measurements. L.L.W., X.C., and X.C.M. assisted in the experiments. K.H., Y.W. and Q.K.X. prepared the manuscript. All authors have read and approved the final version of the manuscript.
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The authors declare no competing financial interests.
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Supplementary Information
Supplementary Figures S1S6, Supplementary Methods and Supplementary References
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