Lu Ping-Keng, Fernandez Olvera Anuar de Jesus, Turan Deniz, Seifert Tom Sebastian, Yardimci Nezih Tolga, Kampfrath Tobias, Preu Sascha, Jarrahi Mona
Electrical and Computer Engineering Department, University of California, Los Angeles, CA, USA.
Department of Electrical Engineering and Information Technology, Technical University Darmstadt, Darmstadt, Germany.
Nanophotonics. 2022 Mar 10;11(11):2661-2691. doi: 10.1515/nanoph-2021-0785. eCollection 2022 Jun.
Efficient terahertz generation and detection are a key prerequisite for high performance terahertz systems. Major advancements in realizing efficient terahertz emitters and detectors were enabled through photonics-driven semiconductor devices, thanks to the extremely wide bandwidth available at optical frequencies. Through the efficient generation and ultrafast transport of charge carriers within a photo-absorbing semiconductor material, terahertz frequency components are created from the mixing products of the optical frequency components that drive the terahertz device - a process usually referred to as photomixing. The created terahertz frequency components, which are in the physical form of oscillating carrier concentrations, can feed a terahertz antenna and get radiated in case of a terahertz emitter, or mix with an incoming terahertz wave to down-convert to DC or to a low frequency photocurrent in case of a terahertz detector. Realizing terahertz photoconductors typically relies on short-carrier-lifetime semiconductors as the photo-absorbing material, where photocarriers are quickly trapped within one picosecond or less after generation, leading to ultrafast carrier dynamics that facilitates high-frequency device operation. However, while enabling broadband operation, a sub-picosecond lifetime of the photocarriers results in a substantial loss of photoconductive gain and optical responsivity. In addition, growth of short-carrier-lifetime semiconductors in many cases relies on the use of rare elements and non-standard processes with limited accessibility. Therefore, there is a strong motivation to explore and develop alternative techniques for realizing terahertz photomixers that do not rely on these defect-introduced short-carrier-lifetime semiconductors. This review will provide an overview of several promising approaches to realize terahertz emitters and detectors without short-carrier-lifetime semiconductors. These novel approaches utilize p-i-n diode junctions, plasmonic nanostructures, ultrafast spintronics, and low-dimensional materials to offer ultrafast carrier response. These innovative directions have great potentials for extending the applicability and accessibility of the terahertz spectrum for a wide range of applications.
高效的太赫兹产生和探测是高性能太赫兹系统的关键前提。由于光频具有极宽的带宽,光子驱动的半导体器件推动了实现高效太赫兹发射器和探测器方面的重大进展。通过光吸收半导体材料中载流子的高效产生和超快传输,太赫兹频率分量由驱动太赫兹器件的光频分量的混频产物产生——这一过程通常称为光混频。产生的太赫兹频率分量以振荡载流子浓度的物理形式存在,对于太赫兹发射器而言,它可以馈入太赫兹天线并辐射出去;对于太赫兹探测器而言,它可以与入射太赫兹波混合,下变频为直流或低频光电流。实现太赫兹光电导体通常依赖于短载流子寿命的半导体作为光吸收材料,光生载流子在产生后一皮秒或更短时间内迅速被俘获,从而导致超快的载流子动力学,有利于高频器件运行。然而,虽然实现了宽带运行,但光生载流子的亚皮秒寿命导致光电导增益和光学响应率大幅损失。此外,在许多情况下,短载流子寿命半导体的生长依赖于稀有元素的使用和难以获得的非标准工艺。因此,迫切需要探索和开发替代技术来实现不依赖于这些引入缺陷的短载流子寿命半导体的太赫兹光混频器。本综述将概述几种不使用短载流子寿命半导体来实现太赫兹发射器和探测器的有前景的方法。这些新颖的方法利用p-i-n二极管结、等离子体纳米结构、超快自旋电子学和低维材料来提供超快的载流子响应。这些创新方向在扩展太赫兹光谱在广泛应用中的适用性和可及性方面具有巨大潜力。