Wu Liang, Tse Wang-Kong, Brahlek M, Morris C M, Aguilar R Valdés, Koirala N, Oh S, Armitage N P
The Institute for Quantum Matter, Department of Physics and Astronomy, The Johns Hopkins University, Baltimore, Maryland 21218, USA.
Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
Phys Rev Lett. 2015 Nov 20;115(21):217602. doi: 10.1103/PhysRevLett.115.217602. Epub 2015 Nov 16.
We have utilized time-domain magnetoterahertz spectroscopy to investigate the low-frequency optical response of the topological insulator Cu_{0.02}Bi_{2}Se_{3} and Bi_{2}Se_{3} films. With both field and frequency dependence, such experiments give sufficient information to measure the mobility and carrier density of multiple conduction channels simultaneously. We observe sharp cyclotron resonances (CRs) in both materials. The small amount of Cu incorporated into the Cu_{0.02}Bi_{2}Se_{3} induces a true bulk insulator with only a single type of conduction with a total sheet carrier density of ~4.9×10^{12}/cm^{2} and mobility as high as 4000 cm^{2}/V·s. This is consistent with conduction from two virtually identical topological surface states (TSSs) on the top and bottom of the film with a chemical potential ~145 meV above the Dirac point and in the bulk gap. The CR broadens at high fields, an effect that we attribute to an electron-phonon interaction. This assignment is supported by an extended Drude model analysis of the zero-field Drude conductance. In contrast, in normal Bi_{2}Se_{3} films, two conduction channels were observed, and we developed a self-consistent analysis method to distinguish the dominant TSSs and coexisting trivial bulk or two-dimensional electron gas states. Our high-resolution Faraday rotation spectroscopy on Cu_{0.02}Bi_{2}Se_{3} paves the way for the observation of quantized Faraday rotation under experimentally achievable conditions to push the chemical potential in the lowest Landau level.
我们利用时域磁太赫兹光谱来研究拓扑绝缘体Cu_{0.02}Bi_{2}Se_{3}和Bi_{2}Se_{3}薄膜的低频光学响应。这类实验同时具有场依赖性和频率依赖性,能提供足够的信息来同时测量多个传导通道的迁移率和载流子密度。我们在这两种材料中都观察到了尖锐的回旋共振(CRs)。掺入Cu_{0.02}Bi_{2}Se_{3}中的少量铜诱导出一种真正的体绝缘体,只有单一类型的传导,总面载流子密度约为4.9×10^{12}/cm^{2},迁移率高达4000 cm^{2}/V·s。这与薄膜顶部和底部两个几乎相同的拓扑表面态(TSSs)的传导一致,其化学势比狄拉克点高约145 meV且处于体能隙中。CR在高场下变宽,我们将这种效应归因于电子 - 声子相互作用。零场德鲁德电导率的扩展德鲁德模型分析支持了这一归属。相比之下,在普通的Bi_{2}Se_{3}薄膜中,观察到了两个传导通道,我们开发了一种自洽分析方法来区分占主导的TSSs和共存的平凡体或二维电子气状态。我们对Cu_{0.02}Bi_{2}Se_{3}进行的高分辨率法拉第旋转光谱为在实验可实现的条件下观察量子化法拉第旋转铺平了道路,以便将化学势推到最低朗道能级。