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CLC number: TN253

On-line Access: 2024-08-27

Received: 2023-10-17

Revision Accepted: 2024-05-08

Crosschecked: 2014-05-04

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Citations:  Bibtex RefMan EndNote GB/T7714

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Journal of Zhejiang University SCIENCE C 2014 Vol.15 No.6 P.482-488

http://doi.org/10.1631/jzus.C1400036


Residual intensity modulation in resonator fiber optic gyros with sinusoidal wave phase modulation


Author(s):  Di-qing Ying, Qiang Li, Hui-lian Ma, Zhong-he Jin

Affiliation(s):  Micro-Satellite Research Center, Zhejiang University, Hangzhou 310027, China

Corresponding email(s):   dqying@zju.edu.cn

Key Words:  Resonator fiber optic gyro, Phase modulation, Residual intensity modulation


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Abstract: 
We present how residual intensity modulation (RIM) affects the performance of a resonator fiber optic gyro (R-FOG) through a sinusoidal wave phase modulation technique. The expression for the R-FOG system’s demodulation curve under RIM is obtained. Through numerical simulation with different RIM coefficients and modulation frequencies, we find that a zero deviation is induced by the RIM effect on the demodulation curve, and this zero deviation varies with the RIM coefficient and modulation frequency. The expression for the system error due to this zero deviation is derived. Simulation results show that the RIM-induced error varies with the RIM coefficient and modulation frequency. There also exists optimum values for the RIM coefficient and modulation frequency to totally eliminate the RIM-induced error, and the error increases as the RIM coefficient or modulation frequency deviates from its optimum value; however, in practical situations, these two parameters would not be exactly fixed but fluctuate from their respective optimum values, and a large system error is induced even if there exists a very small deviation of these two critical parameters from their optimum values. Simulation results indicate that the RIM-induced error should be considered when designing and evaluating an R-FOG system.

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