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利用交流偏置和自补偿扩展 MEMS 硅振子加速度计的偏置不稳定性。

Expanding Bias-instability of MEMS Silicon Oscillating Accelerometer Utilizing AC Polarization and Self-Compensation.

机构信息

School of Mechanical Engineering, Department of Instrument Science and Technology, Nanjing University of Science and Technology, Nanjing 210094, Jiangsu, China.

出版信息

Sensors (Basel). 2020 Mar 6;20(5):1455. doi: 10.3390/s20051455.

DOI:10.3390/s20051455
PMID:32155850
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7085690/
Abstract

This paper presents a MEMS (Micro-Electro-Mechanical System) Silicon Oscillating Accelerometer (SOA) with AC (alternating current) polarization to expand its bias-instability limited by the up-converted 1/f noise from front-end transimpedance amplifier (TIA). In contrast to the conventional DC (direct current) scheme, AC polarization breaks the trade-off between input transistor gate size and white noise floor of TIA, a relative low input loading capacitance can be implemented for low noise consideration. Besides, a self-compensation technique combining polarization source and reference in automatic-gain-control (AGC) is put forward. It cancels the 1/f noise and drift introduced by the polarization source itself, which applies to both DC and AC polarization cases. The experimental result indicates the proposed AC polarization and self-compensation strategy expand the bias-instability of studied SOA from 2.58 μg to 0.51 μg with a full scale of ± 30 g, a 155.6 dB dynamic range is realized in this work.

摘要

本文提出了一种采用交流极化的微机电系统(MEMS)硅微振动加速度计(SOA),以扩展其由前端跨阻放大器(TIA)上变频的 1/f 噪声引起的偏置不稳定性限制。与传统的直流(DC)方案相比,交流极化打破了输入晶体管栅极尺寸和 TIA 的白噪声基底之间的权衡,为了低噪声考虑,可以实现相对低的输入负载电容。此外,提出了一种结合自动增益控制(AGC)中的极化源和参考的自补偿技术。它可以消除由极化源本身引入的 1/f 噪声和漂移,适用于直流和交流极化情况。实验结果表明,所提出的交流极化和自补偿策略将研究的 SOA 的偏置不稳定性从 2.58μg扩展到 0.51μg,满量程为±30g,在这项工作中实现了 155.6dB 的动态范围。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/5291660030a1/sensors-20-01455-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/b6ee540d3238/sensors-20-01455-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/19c477ea64fe/sensors-20-01455-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/f7d95960ff3f/sensors-20-01455-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/bef1fb79365b/sensors-20-01455-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/2aa4b912323d/sensors-20-01455-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/3bcfce444456/sensors-20-01455-g006a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/c372fc8c3ba9/sensors-20-01455-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/e115e73a25b3/sensors-20-01455-g008a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/3a082c3bec63/sensors-20-01455-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/1705f713ac04/sensors-20-01455-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/5291660030a1/sensors-20-01455-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/b6ee540d3238/sensors-20-01455-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/19c477ea64fe/sensors-20-01455-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/f7d95960ff3f/sensors-20-01455-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/bef1fb79365b/sensors-20-01455-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/2aa4b912323d/sensors-20-01455-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/3bcfce444456/sensors-20-01455-g006a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/c372fc8c3ba9/sensors-20-01455-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/e115e73a25b3/sensors-20-01455-g008a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/3a082c3bec63/sensors-20-01455-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/1705f713ac04/sensors-20-01455-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/afed/7085690/5291660030a1/sensors-20-01455-g011.jpg

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