학술논문

A Temperature-Drift Suppression Phase-Locked-Loop With Tunable Locked Range and Frequency Division for MEMS Resonant Accelerometers
Document Type
Periodical
Source
IEEE Sensors Journal IEEE Sensors J. Sensors Journal, IEEE. 24(5):5885-5894 Mar, 2024
Subject
Signal Processing and Analysis
Communication, Networking and Broadcast Technologies
Components, Circuits, Devices and Systems
Robotics and Control Systems
Resonant frequency
Micromechanical devices
Temperature measurement
Optical resonators
Voltage-controlled oscillators
Phase locked loops
Temperature sensors
Microelectromechanical system (MEMS)
resonate accelerometer
temperature compensation
Language
ISSN
1530-437X
1558-1748
2379-9153
Abstract
Microelectromechanical system (MEMS) resonant accelerometers have attracted attention because of their high resolution and quasi-digital output, but their performances are seriously damaged by external temperature fluctuations. Our previous work proposed a temperature-drift suppression phase-locked loop (TDS-PLL) featuring a temperature-sensitive resonator (TSR) as a voltage-controlled oscillator (VCO) to monitor the frequency variations of the acceleration-sensitive resonator (ASR). To solve the problem of mismatched temperature coefficients (TCFs) between the TSR and ASR, the frequency synthesis unit is introduced in this article. The temperature drift of the two resonators can offset each other by adjusting the division factor so that the acceleration drift caused by temperature can be mitigated. Additionally, the proposed self-adaptive frequency regulation (SAFR algorithm) automatically adjusts the locked range of the PLL, thereby expanding the full-scale range of the accelerometer. The effectiveness of the system is further validated through theoretical analysis and simulations. Experimental results indicate that the bias-instability is 3.7 $\mu \text{g}$ and the noise floor is 1.24 $\mu \text{g}/\surd $ Hz with ±2 g full-scale range at room temperature. The temperature drift is 54 mg within a temperature range of 10 °C–60 °C, which is reduced by 95% compared to the uncompressed MRA (1.23 g).