太赫兹 (THz) 光谱范围在通信、非破坏性成像、光谱学和生物工程等众多领域具有相当大的应用潜力。阻碍该技术广泛商业化部署的一个主要障碍是缺乏在太赫兹范围内工作的紧凑且可批量生产的高性能半导体源。如图 1 所示,在低频侧(来自电子器件),谐振隧道二极管 (RTD) 振荡器在室温下工作。另一方面,在高频侧(来自光学装置),已报告有太赫兹量子级联激光器 (THz-QCL);然而,它们需要低温冷却。
图 1:室温半导体 THz 源(输出功率与频率)
量子级联激光器 (QCL) 是半导体发光装置(图 2(a))。该光源是通过对分子束外延或金属有机气相外延晶体生长技术生长的半导体异质结构中的电子波函数进行工程设计而创造的最知名器件之一。与基于带间跃迁的器件不同,QCL 的电学和光学特性(如光学跃迁能量和偶极矩、上下激光态寿命和电子传输)由其异质结构设计决定。工作原理如图 2(b) 所示。在过去的二十年中,QCL 已成为中红外和太赫兹区域最具吸引力的半导体源。然而,THz QCL 仍需要低温冷却才能运行。
图 2(a) 量子级联激光器器件
(b) QCL 的工作原理
从 QCL 生成 THz 的另一种方法是基于双波长中红外 QCL 中的腔内差频生成 (DFG)。这些器件称为 THz DFG-QCL,使用经过设计的中红外 QCL 有源区,可表现出巨大的子带间非线性磁化率 χ(2),从而实现高效的 THz DFG 过程(图 3)。施加偏置电流时,THz DFG-QCL 通过器件有源区中的腔内非线性混频过程产生两个中红外泵浦频率,以及对应于中红外泵浦频率差的太赫兹频率。DFG-QCL 有源区的光学非线性不需要跨 THz 跃迁的粒子数反转。因此,与 THz QCL 不同,THz DFG-QCL 可在室温下工作。THz DFG-QCL 是目前唯一可在室温下工作的电泵浦、单片、可批量生产的半导体源。
图 3:基于非线性光学效应的 THz QCL 源的工作原理概念图
在我们集团中,通过使用我们最初的概念“Anticross DAU 有源区(图 4(a))”,我们在室温下实现了 mW 级输出功率。THz 输出功率可通过室温 THz 热电探测器检测。此外,我们还基于 DAU 有源区获得了跨越一个倍频程的超宽带太赫兹发射光谱(图 4(b)),于是,我们成功地展示了使用这些太赫兹源的太赫兹成像。
图 4 (a) AnticrossDAU 结构
(b) 室温宽带太赫兹非线性 QCL 器件的典型特性
图 5 使用宽带 THz-QCL 源的光谱成像(聚乙烯、D-组氨酸、DL-组氨酸,转载自参考文献 1)
太赫兹频率范围对于许多应用都非常重要,例如成像、化学/生物传感、外差检测和光谱仪。在 ICT 领域,超宽带无线通信有望用于短距离用途,而长距离传输由于强吸水性而难以实现。
在非破坏性检测和分析领域,太赫兹频率范围辐射已用于展示光学频率下不透明物体的成像。太赫兹用途有许多,包括化学物质筛选、工业材料和历史艺术品的非破坏性成像。通过构建使用太赫兹非线性 QCL 的紧凑型成像系统,未来将对太赫兹成像技术进行大量研究。
在天文学领域,太赫兹频率信号非常重要,因为在此频率范围内可以探测到星际气体和灰尘。通过星际气体的精细结构线,可以研究恒星的形成过程。出于这些目的,天文接收器需要紧凑的本地振荡器。由于太赫兹非线性 QCL 源可以产生单频太赫兹信号,因此可以将其用作 LO 来分析来自太空的太赫兹波信号。
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