掺杂GaAs/AlAs量子阱的光学和太赫兹光谱

G. Valušis, Julius Kavaliauskas, B. Čechavičius, Genė Krivaitė, D. Seliuta, Ben Sherliker, M. Halsall, P. Harrison, S. Khanna, E. Linfield
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摘要

我们提出了p型(Be)和n型(Si) &dgr掺杂GaAs/AlAs多量子阱(qw)的综合实验研究,旨在用作太赫兹(THz)范围内的选择性传感器/发射器。通过不同的光反射率、表面光电压和差分表面光电压,研究了不同设计和掺杂水平的结构。在4.300 K的温度范围内使用自由电子或光泵浦分子太赫兹激光器作为太赫兹发射源的太赫兹光电流技术。分析光反射光谱中的Franz-Keldysh振荡和差分表面光电压谱的线形,可以估计大量量子阱子带的内置电场和激子参数。将实验带间跃迁能量与考虑能带非抛物线性的包络函数近似下的计算结果进行了比较。揭示了激子线宽展宽的主要机理,并通过分析激子线宽展宽与量子阱宽度的关系,对界面粗糙度进行了评价。p型结构中的太赫兹光谱测量表明,由于束缚孔的带内吸收,在55 &mgr;m波长附近有很强的吸收,而在80 &mgr;m波长以下的结构中光电流的增加是由Be受体的光热电离引起的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Optical and terahertz spectroscopy of doped GaAs/AlAs quantum wells
We present comprehensive experimental study of p-type (Be) and n-type (Si) &dgr;-doped GaAs/AlAs multiple quantum wells (QWs) intended to be used as selective sensors/emitters in terahertz (THz) range. The structures of various designs and doping levels were studied via different optical-photoreflectance-, surface photovoltage- and differential surface photovoltage. spectroscopies and a THz photocurrent technique using as THz emission source either free electron- or optically-pumped molecular THz laser within 4.300 K range of temperatures. Analysis of Franz-Keldysh oscillations in photoreflectance spectra and line shapes of the differential surface photovoltage spectra enabled to estimate built-in electric fields and excitonic parameters for a large number of QW subbands. The experimental interband transition energies were compared with calculations performed within the envelope function approximation taking into account non-parabolicity of the energy bands. The dominant exciton line broadening mechanisms were revealed, and the interface roughness was evaluated from analysis of the dependence of exciton linewidth broadening on the QW width. Terahertz spectroscopic measurements in p-type structures have indicated strong absorption around 55 &mgr;m wavelength due to intraband absorption of the bound holes, while increase in photocurrent in the structures below 80 &mgr;m wavelength is caused by photothermal ionization of Be acceptors.
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