학술논문
SEBAT-Based Readout for FET THz Detectors With Intrinsic Power-to-Frequency Conversion
Document Type
Periodical
Author
Source
IEEE Sensors Journal IEEE Sensors J. Sensors Journal, IEEE. 22(8):7763-7771 Apr, 2022
Subject
Language
ISSN
1530-437X
1558-1748
2379-9153
1558-1748
2379-9153
Abstract
TeraHertz (THz) detection with Field-Effect Transistor-based (FET-based) detectors requires low-noise amplification, which typically involves trade-offs in terms of complexity, power, and area, resulting in severe scalability constraints for pixel integration into imaging arrays. The purpose of this paper is to describe a novel approach, from design to experimental validation, that enables active device-level amplification of the signal generated by a FET detector and converts it to a frequency suitable for digital processing. This has been done by exploiting a Single-Electron Bipolar Avalanche Transistor (SEBAT) to build a low-noise compact front-end circuit. The FET output is connected to the SEBAT forming a circuit element that here is defined as a TeraHertz Single-Electron Transistor (THzSET). The FET generates a detection current when it senses the THz signal; this current is then injected into the SEBAT, which generates an avalanche current pulse for each single electron, achieving a device-level amplification. The avalanche pulse rate is then evaluated from the signal measured at the SEBAT collector, and performing an FFT of the counts-per-second curve over time it is possible to measure the modulated THz signal applied to the device. The obtained Responsivity $\text {R}_{\text {F}}$ and the Noise Equivalent Power NEP are respectively $\frac {\text {4.61Gcps}}{\text {W}}$ and $\frac {\text {88nW}}{\sqrt {\text {Hz}}} $ at 330GHz illumination frequency. This is achieved with sub- $\mu \text{W}$ power consumption and minimal area overhead: indeed, the pixel and the interface have a total area of 0.146mm 2 , where the antenna area is ${455} \times {320}\mu \text{m}^{{2}}$ and the SEBAT area is ${27} \times {22}\mu \text{m}^{{2}}$ .