- Nano Express
- Open Access
Influence of Thickness on the Electrical Transport Properties of Exfoliated Bi_{2}Te_{3} Ultrathin Films
- D. L. Mo^{1, 2},
- W. B. Wang^{1, 2} and
- Q. Cai^{1, 2}Email authorView ORCID ID profile
- Received: 20 April 2016
- Accepted: 26 July 2016
- Published: 2 August 2016
Abstract
In this work, the mechanical exfoliation method has been utilized to fabricate Bi_{2}Te_{3} ultrathin films. The thickness of the ultrathin films is revealed to be several tens of nanometers. Weak antilocalization effects and Shubnikov de Haas oscillations have been observed in the magneto-transport measurements on individual films with different thickness, and the two-dimensional surface conduction plays a dominant role. The Fermi level is found to be 81 meV above the Dirac point, and the carrier mobility can reach ~6030 cm^{2}/(Vs) for the 10-nm film. When the film thickness decreases from 30 to 10 nm, the Fermi level will move 8 meV far from the bulk valence band. The coefficient α in the Hikami-Larkin-Nagaoka equation is shown to be ~0.5, manifesting that only the bottom surface of the Bi_{2}Te_{3} ultrathin films takes part in transport conductions. These will pave the way for understanding thoroughly the surface transport properties of topological insulators.
Keywords
- Bi_{2}Te_{3} ultrathin films
- Exfoliation
- Thickness influence
- Weak antilocalization
- Shubnikov de Haas oscillations
Background
As a unique class of condense matter materials, topological insulators (TIs) have attracted considerable attention these years for their potential applications in spintronics and quantum computation [1, 2]. TIs are characterized by intrinsic insulating bulk states and metallic surface states due to strong spin-orbit coupling. Theoretically, the Dirac-like surface states of TIs are protected by charge symmetry and time reversal invariance, to guarantee it non-trivial. As a result, the electron spin is locked with its momentum and the backscattering induced by nonmagnetic impurities is prohibited. These special natures of TIs bring forth exotic phenomena, such as quantum spin Hall effect and Majorana fermions appearing in vortex cores between the interface of TI and superconductor [1–4]. After HgTe/CdTe quantum wells, Bi_{2}Se_{3}, Bi_{2}Te_{3}, and Sb_{2}Te_{3} as the second generation of three-dimensional TIs were proved with angle-resolved photoemission spectroscopy (ARPES) experiments to have the surface states exhibiting ideal single Dirac cone in energy band structures [5–7]. In recent years, mesoscopic quantum interference phenomena of these TI materials have been heatedly researched, such as Aharonov-Bohm oscillations, universal conductance fluctuations, weak antilocalization (WAL) effects and Shubnikov de Haas (SdH) oscillations, in which many relevant physical parameters have been obtained [8–13].
It is well-established that bismuth-telluride (Bi_{2}Te_{3}) is an important thermoelectric material. After confirmed as TI with very strong spin-orbit coupling, Bi_{2}Te_{3} becomes a proper platform for investigating WAL effects. The current researches usually focus on Bi_{2}Se_{3}, which has a relatively large band gap in bulk (~0.3 eV). The Bi_{2}Se_{3} and Bi_{2}Te_{3} samples are commonly fabricated through chemical solution synthesis, molecular beam epitaxy, and chemical vapor deposition [10, 14, 15]. To utilize surface states of TI, the Fermi level of surface states must be near the Dirac point. The chemical nature of graphene ensures that the Fermi level is located naturally at the Dirac point, but it is not the case for TIs [1]. And there is a major hindrance for researching the exotic transport properties of TI surface states. The conducting bulk is usually more prevalent due to the existence of vacancies and impurities. Therefore, it is difficult to control and manipulate independently the conduction from the topological surface/edge states [16]. In order to suppress the bulk contributions to electrical transport and focus on the transport properties of surface states, two solutions can be employed: to manipulate the Fermi level by elemental doping/electric gating or to increase the surface-to-volume ratio. The ARPES and Hall transport experiments on Bi_{2}Se_{3} showed that a small amount of Ca doping would result in insulating bulk, and the resistivity of the TI samples could be easily affected by Ca concentration [17]. It was found that the bulk conductance was suppressed by four orders of magnitude in the Cu doped Bi_{2}Te_{3} films [18]. When the thickness of TI films is decreased to nanoscale or the nanostructures of TI materials are constructed, the surface-to-volume ratio of the samples will become larger. And the contributions from the topological surface conduction will dominate the transport properties [19, 20].
It is well-known that Bi_{2}Te_{3} has a layered crystal structure, and the weak van der Waals interaction exists between its atomic quintuple layers [21, 22]. Therefore, Bi_{2}Te_{3} can be exfoliated into ultrathin films with the thickness even down to several quintuple layers. In recent years, the transport properties of Bi_{2}Te_{3} films have been studied widely. However, the explicit experimental investigations about the influence of the film thickness have not been reported on the electron transport of gapless surface states within our knowledge. The systematic explorations about thickness effects of TI thin films will be useful and compatible to device fabrication. In this work, the Bi_{2}Te_{3} ultrathin films are prepared by means of mechanical exfoliation. The film thickness is manifested ranging from 10 to 200 nm by using scanning electron microscopy, atomic force microscopy, and Raman spectroscopy, as well as its relations with the size. The relevant transport parameters have been obtained from the measurements of WAL effects and SdH oscillations, and the influences of film thickness are discussed on the transport properties of gapless surface states. It is shown that there is only the bottom surface participating in the observed WAL conduction for the Bi_{2}Te_{3} films as thin as 10 nm. The present results can provide a valuable insight into the applications of TIs in future electronic and spintronic devices.
Methods
Owing to the layered crystal structure, the Bi_{2}Te_{3} ultrathin films were produced by means of mechanical exfoliation from the commercial crystalline bulk Bi_{2}Te_{3} with a purity of 99.99 %. After exfoliation, the obtained micro-flakes of Bi_{2}Te_{3} were transferred onto a Si substrate with a 285-nm SiO_{2} layer on the surface. The morphology and thickness of Bi_{2}Te_{3} ultrathin films were characterized mainly with scanning electron microscopy (SEM), atomic force microscopy (AFM), and micro-Raman spectroscopy. SEM experiments were performed in a Zeiss Sigma SEM system with Raith Elphy Plus, which functioned at 5 kV for topography observation and 20 kV for electron beam lithography. The AFM observations were carried out in air using noncontact mode, and Raman spectra were obtained with a laser excitation at 632 nm. In order to investigate the electrical transport properties, the four-terminal contacts were fabricated for a single Bi_{2}Te_{3} ultrathin film on the SiO_{2}/Si substrate by using electron beam lithography followed by the 5 nm/50 nm Cr/Au metal depositions with an electron beam evaporator and lift-off process. The electrical transport measurements were carried out, with the temperature ranging from 2 to 300 K and a magnetic field perpendicular to the sample plane, in a quantum design physical property measurement system under the pressure of 10 torr. The standard four-probe technique for transport measurements was adopted to eliminate the effects of contact resistance, with the two outer electrodes connected to a current source and the two inner electrodes to a voltmeter.
Results and Discussion
Size and thickness of Bi_{2}Te_{3} micro-flakes obtained from SEM and AFM observations
Size (μm) | 1–5 | 5–10 | 10–20 | 20–50 | >50 |
Thickness (nm) | 10–15 | 15–30 | 30–70 | 70–200 | >200 |
For bulk Bi_{2}Te_{3}, it is known that its crystal structure belongs to space group R‾3m (D_{3d} ^{5}). And in one unit cell, five atomic layers can be discerned, which commonly called a quintuple [21]. In Raman spectra of Bi_{2}Te_{3}, the most distinct features are E_{g} ^{2} peak (E^{2}) at ~103 cm^{−1} and A_{1g} ^{2} peak (A^{2}) at ~133 cm^{−1}. It is also reported that the intensity ratios of the E_{g} ^{2} peak to the A_{1g} ^{2} peak can be used to evaluate the thickness of Bi_{2}Te_{3} films [23]. The A_{1u} peak at ~117 cm^{−1} which is not Raman active in bulk can also emerge when the thickness of Bi_{2}Te_{3} film is less than 40 nm, and it will become more and more obvious with the decreasing of the film thickness due to crystal-symmetry breaking [21, 23].
The intensity ratios of E^{2} to A^{2} Raman peak at different film thickness
Thickness (nm) | 200 | 50 | 30 | 15 |
I (E^{2})/I (A^{2}) | 3.33 | 2.84 | 2.67 | 2.50 |
Because of the tellurium vacancies or impurities existing, Bi_{2}Te_{3} usually exhibits very good electrical conductivity. In Fig. 2, the resistance of Bi_{2}Te_{3} ultrathin film presents principally a metallic behavior, consistent with the previous works [8, 9]. It can be seen that the resistance increases with the temperature increasing at the range of 10 to 300 K, implying that conductivity is dominated by the carrier mobility. As the temperature decreases, the phonon scattering reduces, resulting in the carrier mobility increasing and the resistance decreasing. When the temperature T lowers below 10 K, the resistance is found to increase with T dropping and appears to present lnT dependence below 5 K as shown in the right inset of Fig. 2, presumably due to freezing effect of the carriers, electron-electron interactions and WAL effect [24, 25]. The low temperature less than 10 K usually brings about the absence of inelastic phonon scattering [8], and impurity scattering of the charge carriers should dominate the transport [26]. This impurity scattering substantially does not change with temperature. However, the temperature dropping causes the carrier concentration to diminish, resulting in the resistance increasing. When T drops below 5 K, electron-electron interactions as well as WAL effect probably make important contributions to conduction, at last inducing the lnT dependence of resistance [25]. In addition, the semiconductor-like resistance below 10 K shown in Fig. 2 indicates that bulk conductance of Bi_{2}Te_{3} ultrathin films is suppressed to a large extent, and surface conduction will act as a non-negligible role [24].
Here, ΔG(B) = G(B) − G(0) is the change of magneto-conductance, Ψ(x) is the digamma function, α is a coefficient indicating the type of localization, L _{ ϕ } is the phase coherent length, h is the Planck constant, and e is electronic charge. According to Fig. 3, the experimental data are fitted with the HLN equation and α = 0.47 is obtained for the Bi_{2}Te_{3} ultrathin film of 10 nm at 2 K, quite close to the theoretical value of 0.5 for WAL in a single conductive channel.
The fitting parameter α is ~0.5 here, manifesting that there is only one topological surface contributing to the WAL transport for our exfoliated Bi_{2}Te_{3} films. And presumably, it is the bottom surface of the ultrathin films that dominates the conduction, due to oxidation and photolithographic contaminations existing on the top surface [10]. In Fig. 3c, d, the parameters of α and L _{ ϕ } extracted from the HLN fittings are plotted as the function of thickness and temperature, respectively. It is shown that α deviates from 0.5 to some extent with the increasing of film thickness, suggesting the bulk contribution to transport becoming larger and disturbing the signal from the surface states. A similar trend happens for α with the increasing of temperature. The phase coherent length L _{ ϕ } is also displayed to decrease with the film thickness increased, due to the effects of the surface states on conduction lowered. L _{ ϕ } can reach 188 nm for the 10-nm film. In Fig. 3d, it is noted that L _{ ϕ } can be fitted well with the T^{−1/2} dependence at the temperature ranging from 2 to 20 K, indicating again that electron-electron interactions become a significant source of dephasing [28]. The T^{−1/2} dependence of L _{ ϕ } is a typical characteristic of two-dimensional electron interference [18], and it gives evidence of the electrical transport through topological surface states existing in the 10-nm Bi_{2}Te_{3} ultrathin film.
The estimated transport parameters from SdH oscillations observed at 2 K on the Bi_{2}Te_{3} films with different thickness
t (nm) | f _{SdH} (T) | k _{F} (nm^{−1}) | m _{cyc} (m_{0}) | V _{F} (10^{5} ms^{−1}) | E _{F} (meV) | τ (10^{−13} s) | μ (cm^{2}V^{ −1} s^{−1}) |
---|---|---|---|---|---|---|---|
10 | 41.2 | 0.35 | 0.117 | 3.47 | 81 | 4.01 | 6030 |
15 | 35.3 | 0.33 | 0.107 | 3.51 | 77 | 3.61 | 5840 |
30 | 31.5 | 0.31 | 0.101 | 3.55 | 73 | 3.27 | 5680 |
For the exfoliated Bi_{2}Te_{3} ultrathin films, the Fermi level is about 80 meV above the Dirac cone, consistent with the previous work [24]. With the thickness decreasing from 30 to 10 nm, the Fermi level moves 8 meV far from the Dirac point and the bulk valence band. According to the band structures of Bi_{2}Te_{3} [6], it is testified that the Fermi level of our exfoliated Bi_{2}Te_{3} ultrathin films shifts into the bulk gap, and the electrical transport properties are dominated by topological surface states for the Bi_{2}Te_{3} films with very small thickness. Balandin et al. have explored the thickness dependence for the resistance and thermoelectric efficiency of the exfoliated Bi_{2}Se_{3} and Bi_{2}Te_{3} films [34, 35], and it is also revealed that the surface transport through the topological surface states will play more and more predominant roles with the film thickness decreased. According to Ref. [19], the mobility of Bi_{2}Te_{3} films obtained with molecular beam epitaxy (MBE) growth is 521 cm^{2}/(Vs). The mobility of our samples fabricated by means of mechanical exfoliation can reach 6030 cm^{2}/(Vs), much higher than those of the samples obtained in MBE growth [28] and chemical method [24]. Probably because the samples in the previous works have a non-insulating substrate or a surface/crystal structure not so intact as those of our exfoliated samples. In this work, the experimental mobility of carriers is found in the range of 5680 to 6030 cm^{2}/(Vs), increasing with the thickness decreased and diminishing with the bulk transport involved. It is proposed that ultra-small thickness for TIs is a good way to control and suppress the bulk contribution to the electrical transport.
Conclusions
In summary, the Bi_{2}Te_{3} ultrathin films with the thickness of several tens of nanometers have been fabricated by using mechanical exfoliation. According to the experimental results of SEM, AFM, and Raman Spectroscopy, the ultrathin films are found to possess excellent crystal quality as well as smooth surfaces, and their thickness increases with the increasing of size. The WAL effect and SdH oscillations have been observed in the magneto-transport investigations for the films with magnetic field perpendicular to the surface. It is verified that the two-dimensional transport through topological surface states plays a dominant role in conductance of the film as thin as 10 nm. The coefficient α in the HLN equation has a measurement of ~0.5 and suggests that only one surface channel contributes to the conduction. It is shown that the carrier mobility can reach ~6000 cm^{2}/(Vs) for the thinner film, almost one order of magnitude larger than the bulk mobility. Ultra-small thickness is demonstrated an effective way for TIs to control and suppress the bulk contribution to transport.
Declarations
Acknowledgements
The authors would like to acknowledge the experimental assistance and helpful suggestions from Dr. Yijun Yu and Prof. Yuanbo Zhang, Department of Physics of Fudan University. This work was supported by the National Natural Science Foundation of China under Grant No. 11374058 and the National Science Fund for Talent Training in Basic Science under Grant No. J1103204.
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Authors’ Affiliations
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