A Highly Power Efficient 2×3 PIN-Diode-Based Intercoupled THz Radiating Array at 425GHz with 18.1dBm EIRP in 90nm SiGe BiCMOS

Sam Razavian, A. Babakhani
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引用次数: 4

Abstract

Efficient THz generation in silicon technologies has been of great interest over the recent years, as it enables an integrated low-cost solution for sensing, radar, communication, and spectroscopy [1]. Due to the limited $\mathrm{f}_{\mathrm{T}}/\mathrm{f}_{\max}$ of transistors, direct THz generation using a fundamental oscillator is not feasible; therefore, various approaches have been developed based on harmonic extraction and the frequency multiplication of a fundamental oscillator [2]. In these techniques, the nonlinearity of transistors is utilized to generate higher harmonics from a fundamental oscillator or frequency-multiplier cells; however, such systems have a poor efficiency and low radiated power due to device limitations. To compensate for the low generated power, a coherent array scheme is preferred to increase EI RP and radiated power. Adjusting the phase and locking the frequency of elements for coherent operation are important factors in array architectures, which can be performed through central LO distribution [3] and mutual coupling [4]. LO distribution can cause phase mismatch between elements and significantly increases the DC power consumption by adding more blocks. Mutual coupling through injection locking can maintain phase alignment. However, this type of coupling has low tuning range, which makes it challenging to synchronize elements over a broad frequency range. In this work, a technique for THz CW generation is presented, in which, instead of relying on transistor nonlinearity, a PIN diode is used in the reverse recovery mode for strong harmonic generation. A PIN diode, similar to a step recovery diode (SRD), benefits from a sharp reverse recovery and is highly nonlinear in the recovery mode, which enables efficient THz harmonic generation by upconverting the output of a mm-wave oscillator without requiring additional blocks and multipliers. The PIN-based array consists of 2x3 elements, where differential Colpitts oscillators are used as the core to push the PIN diodes into reverse recovery. Array elements are intercoupled using a collective coupling approach that enables wide tuning range and phase match between elements. The PIN-based array achieves a radiated power of 0.31 mW and 18.1dBm EIRP at 425GHz.
在90nm SiGe BiCMOS中,基于2×3引脚二极管的高效率425GHz互耦太赫兹辐射阵列,EIRP为18.1dBm
近年来,硅技术中高效的太赫兹产生引起了极大的兴趣,因为它为传感、雷达、通信和光谱学提供了一个集成的低成本解决方案[1]。由于晶体管的$\ mathm {f}_{\ mathm {T}}/\ mathm {f}_{\max}$有限,使用基频振荡器直接产生太赫兹是不可实现的;因此,基于谐波提取和基振倍频的各种方法被开发出来[2]。在这些技术中,利用晶体管的非线性从基频振荡器或倍频单元产生更高的谐波;然而,由于器件的限制,这种系统的效率较差,辐射功率较低。为了补偿低功率的产生,首选相干阵列方案来提高EI RP和辐射功率。调整相位和锁定单元频率以实现相干操作是阵列架构中的重要因素,这可以通过中心LO分布[3]和相互耦合[4]来实现。LO分布会导致元件之间的相位失配,并通过增加更多的块而显著增加直流功耗。通过注入锁定的相互耦合可以保持相位对准。然而,这种类型的耦合具有较低的调谐范围,这使得在较宽的频率范围内同步元件具有挑战性。在这项工作中,提出了一种太赫兹连续波产生技术,该技术不依赖于晶体管非线性,而是使用PIN二极管以反向恢复模式产生强谐波。PIN二极管类似于阶跃恢复二极管(SRD),受益于尖锐的反向恢复,并且在恢复模式下高度非线性,通过上变频毫米波振荡器的输出,无需额外的模块和乘数器,即可实现高效的太赫兹谐波产生。基于PIN的阵列由2x3个元件组成,其中差分Colpitts振荡器用作核心,以推动PIN二极管进入反向恢复。阵列元素使用集体耦合方法相互耦合,从而实现元素之间的宽调谐范围和相位匹配。基于pin的阵列在425GHz时的辐射功率为0.31 mW, EIRP为18.1dBm。
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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