Comparison of THz (far-infrared) time domain spectroscopy and FTS methods

D. Grischkowsky
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Abstract

This paper will first describe the optoelectronic generation and detection of freely-propagating fsec pulses of THz electromagnetic radiation, and then applications of the THz beam system to THz time-domain spectroscopy (TDS) will be presented. Via optoelectronic excitation, a transient point source of THz radiation is generated at the focus of a dielectric collimating lens, followed by an additional paraboloidal focusing and collimating mirror. This source produces well collimated beams of fsec pulses of THz radiation. Matched to an identical receiver, the resulting system has extremely high collection efficiency (1). With a demonstrated signal-to-noise ratio of 1000, a time resolution of less than 150 fsec and a frequency range from 0.2 THz to more than 5 THz, (1 THz = 33.3 cm-1 = 4.1 meV), the performance of this optoelectronic THz system is limited by the intrinsic response time of the semiconductor (2).
太赫兹(远红外)时域光谱与FTS方法的比较
本文首先介绍了太赫兹电磁辐射自由传播fsec脉冲的光电产生和探测,然后介绍了太赫兹波束系统在太赫兹时域波谱(TDS)中的应用。通过光电激发,在介质准直透镜的焦点处产生一个瞬态太赫兹辐射点源,随后是一个额外的抛物面聚焦和准直镜。该源产生准直的fsec太赫兹辐射脉冲光束。与相同的接收器相匹配,所得到的系统具有极高的收集效率(1)。所演示的信噪比为1000,时间分辨率小于150 fsec,频率范围从0.2 THz到超过5 THz, (1 THz = 33.3 cm-1 = 4.1 meV),该光电太赫兹系统的性能受到半导体固有响应时间的限制(2)。
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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