Polarization characteristics of terahertz wave generated by differential frequency mixing under exciton excitation condition in a semiconductor quantum well (Conference Presentation)

O. Kojima
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Abstract

As continuous wave (CW) terahertz (THz) sources, the differential-frequency-mixing (DFM) has an advantage for the frequency tunability by changing the energy separation of the two lasers. In particular, considering the inhomogeneous width in the quantum confinement systems, use of the exciton lines enables wide frequency tuning. The THz sources with the narrow bandwidth and wide frequency tunability will be applied to the high resolution THz spectroscopy. Recently, we realized the CW-THz wave generation by DFM under the exciton excitation conditions in a GaAs/AlAs multiple quantum well (MQW), which shows the wide frequency tuning range over 18 THz. Therefore, in this work, we report the polarization characteristics of a continuous THz electromagnetic wave generated by DFM due to excitation of two exciton states in the GaAs/AlAs multiple quantum well. As a sample, we used an undoped GaAs/AlAs MQW embedded in a p-i-n structure on a (001) n+-GaAs substrate. The thickness of GaAs and AlAs layer is 7.5 nm. The measurements of the THz wave were carried out at 296 K. As the laser sources, a semiconductor laser and a CW-mode Ti:sapphire laser to change the excitation energy were used. The two beams were focused on the sample surface. Comparing the polarization of the laser beams with that of the THz wave, the conversion process from the laser lights to the THz wave via the exciton states, such as the heavy hole and light hole excitons split by quantum confined effects, will be demonstrated.
半导体量子阱中激子激励下差频混合产生的太赫兹波的偏振特性(会议报告)
作为连续波(CW)太赫兹(THz)源,差频混频(DFM)通过改变两个激光器的能量间隔,具有频率可调性的优势。特别地,考虑到量子约束系统的非均匀宽度,使用激子线可以实现宽频率调谐。窄带宽、宽频率可调性的太赫兹源将应用于高分辨率太赫兹光谱。最近,我们在GaAs/AlAs多量子阱(MQW)中实现了激子激发条件下DFM产生CW-THz波,其频率调谐范围超过18 THz。因此,在这项工作中,我们报道了由于GaAs/AlAs多量子阱中两个激子态的激发,DFM产生的连续太赫兹电磁波的极化特性。作为样本,我们在(001)n+-GaAs衬底上使用了未掺杂的GaAs/AlAs MQW嵌入p-i-n结构。GaAs和AlAs层厚度为7.5 nm。太赫兹波的测量是在296 K进行的。采用半导体激光器和cw模式钛蓝宝石激光器作为激光源,改变激发能。两束光束聚焦在样品表面。将激光光束的偏振与太赫兹波的偏振进行比较,展示了激光通过量子限制效应分裂的重空穴和轻空穴激子等激子态向太赫兹波的转换过程。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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