학술논문

SEBAT-Based Readout for FET THz Detectors With Intrinsic Power-to-Frequency Conversion
Document Type
Periodical
Source
IEEE Sensors Journal IEEE Sensors J. Sensors Journal, IEEE. 22(8):7763-7771 Apr, 2022
Subject
Signal Processing and Analysis
Communication, Networking and Broadcast Technologies
Components, Circuits, Devices and Systems
Robotics and Control Systems
Detectors
Field effect transistors
Sensors
Antennas
Junctions
Performance evaluation
Metals
Terahertz
FET detector
CMOS sensors
SEBAT
avalanche diode
THzSET
Language
ISSN
1530-437X
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 ${27} \times {22}\mu \text{m}^{{2}}$ .