25.5 A 320GHz锁相发射机,辐射功率3.3mW, EIRP 22.5dBm,用于外差太赫兹成像系统

R. Han, Chen Jiang, A. Mostajeran, Mohammad Emadi, Hamidreza Aghasi, H. Sherry, A. Cathelin, E. Afshari
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引用次数: 56

摘要

在过去的几年中,使用固态集成电子器件的非电离太赫兹成像越来越受到关注。然而,目前有几个因素阻碍了全集成成像系统的实现。由于缺乏fmax以上的低噪声放大,硅上太赫兹像素的灵敏度无法与毫米波或光波对应的灵敏度相匹配。这与以前传感器采用的焦平面阵列结构相结合,要求光源的功率非常大。先前在硅上的工作已经证明了1mW的辐射[1,3];但实际的成像系统需要更高的功率和能源效率。此外,外差成像方案被证明是非常有效的提高检测灵敏度[4]。由于相位信息的保存,它也使数字波束形成与少量的接收器单元。然而,这需要太赫兹源和接收器LO之间的锁相,频率偏移较小(中频< 1GHz)。在[5]中,报告了一个带有探测输出的300GHz锁相环。本文提出了一种采用SiGe hbt的320GHz发射机(图25.5.1)。本作品结合16个相干辐射体,实现了3.3mW的辐射功率和0.54%的DC-RF效率,这是目前最先进的硅太赫兹辐射体中最高的,如图25.5.6的对比表所示。同时,输出光束由一个完全集成的锁相环锁相,从而实现高性能外差成像系统。
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25.5 A 320GHz phase-locked transmitter with 3.3mW radiated power and 22.5dBm EIRP for heterodyne THz imaging systems
Non-ionizing terahertz imaging using solid-state integrated electronics has been gaining increasing attention over the past few years. However, there are currently several factors that deter the implementations of fully-integrated imaging systems. Due to the lack of low-noise amplification above fmax, the sensitivity of THz pixels on silicon cannot match that of its mm-Wave or light-wave counterparts. This, combined with the focal-plane array configuration adopted by previous sensors, requires exceedingly large power for the illumination sources. Previous works on silicon have demonstrated 1mW radiation [1,3]; but higher power, as well as energy efficiency, are needed for a practical imaging system. In addition, heterodyne imaging scheme was demonstrated to be very effective in enhancing detection sensitivity [4]. Due to the preservation of phase information, it also enables digital beam forming with a small number of receiver units. This however requires phase locking between the THz source and receiver LO with a small frequency offset (IF<;1GHz). In [5], a 300GHz PLL is reported with probed output. In this paper, a 320GHz transmitter using SiGe HBTs is presented (Fig. 25.5.1). Combining 16 coherent radiators, this work achieves 3.3mW radiated power with 0.54% DC-RF efficiency, which are the highest among state-of-the-art silicon THz radiators shown in the comparison table in Fig. 25.5.6. Meanwhile, the output beam is phase-locked by a fully-integrated PLL, which enables high-performance heterodyne imaging systems.
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