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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Di-qing Ying, Qiang Li, Hui-lian Ma, Zhong-he Jin. Residual intensity modulation in resonator fiber optic gyros with sinusoidal wave phase modulation[J]. Journal of Zhejiang University Science C, 2014, 15(6): 482-488.
@article{title="Residual intensity modulation in resonator fiber optic gyros with sinusoidal wave phase modulation",
author="Di-qing Ying, Qiang Li, Hui-lian Ma, Zhong-he Jin",
journal="Journal of Zhejiang University Science C",
volume="15",
number="6",
pages="482-488",
year="2014",
publisher="Zhejiang University Press & Springer",
doi="10.1631/jzus.C1400036"
}
%0 Journal Article
%T Residual intensity modulation in resonator fiber optic gyros with sinusoidal wave phase modulation
%A Di-qing Ying
%A Qiang Li
%A Hui-lian Ma
%A Zhong-he Jin
%J Journal of Zhejiang University SCIENCE C
%V 15
%N 6
%P 482-488
%@ 1869-1951
%D 2014
%I Zhejiang University Press & Springer
%DOI 10.1631/jzus.C1400036
TY - JOUR
T1 - Residual intensity modulation in resonator fiber optic gyros with sinusoidal wave phase modulation
A1 - Di-qing Ying
A1 - Qiang Li
A1 - Hui-lian Ma
A1 - Zhong-he Jin
J0 - Journal of Zhejiang University Science C
VL - 15
IS - 6
SP - 482
EP - 488
%@ 1869-1951
Y1 - 2014
PB - Zhejiang University Press & Springer
ER -
DOI - 10.1631/jzus.C1400036
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.
[1]Carroll, R., Coccoli, C.D., Cardarelli, D., et al., 1987. The passive resonator fiber optic gyro and comparison to the interferometer fiber gyro. Fiber Optic Gyros: 10th Anniversary Conf. Int. Society for Optics and Photonics, p.169-177.
[2]Chow, W.W., Gea-Banaciloche, J., Pedrotti, L.M., et al., 1985. The ring laser gyro. Rev. Mod. Phys., 57(1):61-103.
[3]Hotate, K., Harumoto, M., 1997. Resonator fiber optic gyro using digital serrodyne modulation. J. Lightw. Technol., 15(3):466-473.
[4]Hotate, K., Hayashi, G., 1999. Resonator fiber optic gyro using digital serrodyne modulation-method to reduce the noise induced by the backscattering and closed-loop operation using digital signal processing. SPIE, 3746:104-107.
[5]Hu, Z., 2008. Effects of residual intensity modulation of Y-waveguide modulator on interferometric fiber optic gyroscope and elimination method. Chin. J. Lasers, 35(12):1924-1929 (in Chinese).
[6]Iwatsuki, K., Hotate, K., Higashiguchi, M., 1984. Effect of Rayleigh backscattering in an optical passive ring-resonator gyro. Appl. Opt., 23(21):3916-3924.
[7]Iwatsuki, K., Hotate, K., Higashiguchi, M., 1986. Kerr effect in an optical passive ring-resonator gyro. J. Lightw. Technol., 4(6):645-651.
[8]Jaatinen, E., Hopper, D.J., Back, J., 2009. Residual amplitude modulation mechanisms in modulation transfer spectroscopy that use electro-optic modulators. Meas. Sci. Technol., 20(2):1-8.
[9]Jin, Z., Zhang, G., Mao, H., et al., 2012. Resonator micro optic gyro with double phase modulation technique using an FPGA-based digital processor. Opt. Commun., 285(5):645-649.
[10]Lefevre, H., 1993. The Fiber-Optic Gyroscope. Artech House, London, United Kingdom, p.5-26.
[11]Li, X., Ge, C., Zhang, C., 2009. The influence of residuary intensity modulation of Y waveguide on the performance of IFOG. Opto-Electron. Eng., 36(11):43-47 (in Chinese).
[12]Ma, H., Jin, Z., Ding, C., et al., 2003. Influence of spectral linewidth of laser on resonance characteristics in fiber ring resonator. Chin. J. Lasers, 30(8):731-734 (in Chinese).
[13]Ma, H., Jin, Z., Ding, C., et al., 2004. Research on signal detection method of resonator fiber optical gyro. Chin. J. Lasers, 31(8):1001-1005 (in Chinese).
[14]Ma, H., Lu, X., Yao, L., et al., 2012. Full investigation of the resonant frequency servo loop for resonator fiber-optic gyro. Appl. Opt., 51(21):5178-5185.
[15]Malvern, A., 1992. Progress toward fiber optic gyro production. Fiber Optic Gyros: 15th Anniversary Conf. Int. Society for Optics and Photonics, p.48-64.
[16]Meyer, R.E., Ezekiel, S., Stowe, D.W., et al., 1983. Passive fiber-optic ring resonator for rotation sensing. Opt. Lett., 8(12):644-646.
[17]Sathian, J., Jaatinen, E., 2012. Intensity dependent residual amplitude modulation in electro-optic phase modulators. Appl. Opt., 51(16):3684-3691.
[18]Savatinova, I., Tonchev, S., Todorov, R., et al., 1996. Electro-optic effect in proton exchanged LiNbO3 and LiTaO3 waveguides. J. Lightw. Technol., 14(3):403-409.
[19]Shupe, D.M., 1981. Fiber resonator gyroscope: sensitivity and thermal nonreciprocity. Appl. Opt., 20(2):286-289.
[20]Wang, D., Sheng, F., 2007. Residuary intensity modulation of the phase modulator in IFOG and its measurement. Opto-Electron. Eng., 34(7):26-29 (in Chinese).
[21]Wang, W., Zhang, G., 1995. The effect of residual intensity modulation of Ti: LiNbO3 phase modulator in closed-loop FOG. J. Chin. Inert. Technol., 3(1):55-58 (in Chinese).
[22]Ying, D., Ma, H., Jin, Z., 2008a. Resonator fiber optic gyro using the triangle wave phase modulation technique. Opt. Commun., 281(4):580-586.
[23]Ying, D., Ma, H., Jin, Z., 2008b. Dynamic characteristics of R-FOG based on the triangle wave phase modulation technique. Opt. Commun., 281(21):5340-5343.
[24]Ying, D., Demokan, M.S., Zhang, X., et al., 2010. Analysis of Kerr effect in resonator fiber optic gyros with triangular wave phase modulation. Appl. Opt., 49(3):529-535.
[25]Zhang, G., Wang, W., 1996. The effect of polarization crosstalk of Ti: LiNbO3 phase modulator in closed-loop fiber-optic gyro. Missil. Space Veh., 221(3):20-25 (in Chinese).
[26]Zhang, X., Ma, H., Ding, C., et al., 2005. Analysis on phase modulation spectroscopy of resonator fiber optic gyro. Chin. J. Lasers, 32(11):1529-1533 (in Chinese).
[27]Zhang, X., Ma, H., Zhou, K., et al., 2006a. Experiments in PM-spectroscopy resonator fiber optic gyro. Chin. J. Sens. Actuat., 19(3):800-803 (in Chinese).
[28]Zhang, X., Ma, H., Ding, C., et al., 2006b. Optical Kerr effect in phase modulation spectroscopy resonator fiber optic gyro. Chin. J. Lasers, 33(6):814-818 (in Chinese).
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