基于FRM的干涉型光纤传感系统偏振噪声研究
详细信息    本馆镜像全文|  推荐本文 |  |   获取CNKI官网全文
摘要
法拉第旋镜FRM (Faraday Rotator Mirror)法是抑制干涉型光纤传感系统偏振诱导信号衰落的一种重要方案,它在理论上可以完全消除偏振衰落,但是由于所选FRM的旋转角度并非精确的45°,系统中会出现残余偏振诱导相位噪声(简称:偏振噪声)。当偏振噪声与目标信号频带重合时二者无法区分,在这种情况下,深入进行偏振噪声和相关抑制方法的研究有特别重要的意义。
     本文用琼斯矩阵建立了基于FRM的干涉型光纤传感系统偏振噪声的模型,分析出影响偏振噪声的三种主要因素:FRM的旋转角度偏差,入射光偏振态调制度,干涉仪两臂光纤双折射。根据这些因素提出了三种抑制偏振噪声的方法:1、尽可能选择角度偏差接近0的FRM,这种方法最直接有效;2、在传输光纤周围加一圈缓冲层以减小外界环境对光纤的直接作用,减小偏振态调制度;3、在干涉仪两臂各加一个PZT,对其施加直流调制以改变光纤双折射,从而减小偏振噪声。计算出当所选FRM为最大旋转角度偏差1°(由产品指标得到)时,系统在偏振态调制度为1.84 rad时可能出现最大偏振噪声,其幅度为0.0815 rad (-26.6 dB)。
     为了调制入射光偏振态并研究由此给干涉系统带来的偏振噪声,设计了一种M-Z型光纤偏振态调制器PSM(Polarization State Modulator),测量了PSM的稳定性,结果表明在测试时间内PSM的波动小于0.8%。搭建了基于FRM的平衡干涉型光纤传感实验系统,用PSM对入射光进行频率为1 kHz、不同调制度的偏振态调制,通过PGC外调制解调出由此产生的偏振噪声,结果表明测量值与理论值吻合较好,证明了所建偏振噪声模型的正确性.扭曲Michelson干涉仪两臂光纤,测量了干涉仪内光纤双折射对偏振噪声的影响,结果表明扭动光纤得到的偏振噪声比扭曲前减小了约12 dB ,证明了通过调整干涉仪双折射以消除或抑制偏振噪声的可行性。
     最后指出,实验中设计的偏振噪声测试系统还可用于检测传感探头的光学偏振噪声特性。用PSM对入射光施加相同的偏振态调制度,测试各探头由此产生的偏振噪声,选出偏振噪声较小的探头,从而保证各阵列的低偏振噪声特性。
The method based on Faraday Rotator Mirror(FRM) is one of the most important schemes to eliminate polarization induced fading(PIF) in interferometric fiber-optic sensing system, which in theory can completely eliminate PIF, but due to the rotation angle of the selected FRM is not exactly 45°, the system will appear in the residual polarization-induced phase noise(PIN). When the frequency bands of the residual PIN and the target signal overlap, they can not be distinguished from earch other. In this case, in-depth studies on the characteristics of residual PIN and the associated noise suppression methods seem to be especially important.
     In this dissertation, the residual PIN model of the fiber optic interferometric system based on FRM has been setup, and the three main factors affecting the PIN have been analysed : the ratation angle deviation of FRM, the state of polarization (SOP) of the input light and the birefringence of the optical fiber of the interferometer. Based on those factors three kinds of ways have been proposed to restrain the PIN:1、try the best to select FRMs with the rotation angle deviation close to 0, this approach is the most direct and effective; 2、wrap the lead-fiber with cushion materials to minish direct effect by external environment so as to decrease the degree of polariztion modulation. 3、add a PZT to each interferometer beam and drive the PZT with direct current to decrease PIN. The greatest noise with its amplitude of 0.0815 rad(-26.6 dB) possibly existing in the system when the degree of the poarizaion modulation equals to 1.84 rad is obtained.
     In order to modulate the SOP of input light and investigate the PIN induced by it, a M-Z type optic fiber polarization state modulator(PSM) is put forward and its stability is measured with the result that its fluctuation is lower than 0.8%. Experimental sensing system of balance fiber optic interferomter based on FRM has been set up, and the PIN induced by the input light with different SOP demodulated by PSM at 1 kHz is measured through PGC, results indicate that experiment values are in good accordance with the ones of theory, which demonstrates the correctness of the PIN model. The PINs are measured as well by twisting the optic fiber of the interferometer, which directly changes the birefringence of the fiber, and results show that a decrease by about 12 dB on PIN is obtained by twisting the optic fiber, and the feasibility to eliminate or suppress the residual PIN by adjudting the birefringence of the optic fiber is proved.
     In the end, it is pointed that the system testing PIN can also be used to check the characteristics of optical PIN of the sensor. Modulate the SOP of the input light by the same degree, and test the PIN for every sensor to be used in big scale system, then select the ones with low PIN to ensure low-PIN characteristics of the whole system.
引文
[1]廖延彪,黎敏.光纤传感器的今日与发展[J].传感世界,专家论坛,2004:6~12.
    [2]张学亮,用于拖曳阵阵形测量的光纤磁场传感研究,国防科技大学博士论文,2007.
    [3]王泽锋,罗洪,熊水东等.基于光频调节的干涉型光纤水听器相位补偿检测方法[J].光学学报,2007,27(4):654~658.
    [4]倪明,张仁和,胡永明等.关于光纤水听器灵敏度的讨论[J].应用声学,2002,12(6):18~17.
    [5] Clay K Kirkendall, Anthony Dandridge. Overview of high performance fibre-optic sensing[J]. Applied Physics, 2004, 37: 197 R~216R.
    [6]翼邦杰,李碧丽.光纤传感器应用于水声的试验研究[J].舰船科学技术,2007,29(2):76~78.
    [7]余瑞兰,刘勇,王安.光纤Michelson干涉仪干涉条纹对比度的研究[J].大气与环境光学学报,2007,2(3):231~235.
    [8]戎华北.光纤传感器的应用与发展[J].厦门科技知识长廊,2005:34~36.
    [9]沈洪,罗晖.光纤水听器传感技术及应用[J].技术与应用,2007,27~29.
    [10]倪行洁,赵勇,杨剑等.光纤水声传感技术[J].测量与设备,2006,12:33~38.
    [11]王泽锋,罗洪,胡永明.干涉型光纤传感及其信号检测技术的研究[J].应用光学,2007,86~91.
    [12]张楠,大规模光纤水听器阵列光学外差及时分复用技术研究,国防科技大学硕士论文,2007.
    [13]梁迅,光纤水听器系统噪声分析及抑制技术研究,国防科技大学博士论文,2008.
    [14]倪明,光纤水听器关键技术研究,中国科学院博士论文,2003.
    [15] S.-T.Shih, M.-H.Chen, W.-W.Lin. Analysis of fibre optic Michelson inerferometric sensor distortion caused by the imperfect properties of its 3×3 coupler[J]. Proc.-Optoelectron, 1997,144(6):377~382.
    [16]崔杰,刘亭亭,肖灵等.一种确定光纤传感器中3×3耦合器输出信号相位差的新算法[J].应用声学,2006,27(1):36~41.
    [17]张诚,王金海,陈才和等.非对称3×3干涉型传感器解调系统设计[J].光电工程,2007,34(11):135~140.
    [18]曹家年,于晓之,朱雪峰等.干涉型光纤传感器PGC检测中的AGC[J].哈尔滨工程大学学报,2007,28(8):930~934.
    [19]岳士举,丁昕,曹家年.干涉型光纤水听器PGC解调方案的研究[J].应用科技,2006,33(6):110~114.
    [20]刘鹰,李玉深,徐大伟等.迈克尔逊干涉型光纤水听器研究与实现[J].传感器技术,2005,24(11):30~32.
    [21]曹家年,张立昆.双光束干涉型光纤传感器抗偏振消衰落技术[J].光纤与电缆及其应用技术,1999,4:22~27.
    [22]胡永明,陈哲,孟洲等.全保偏光纤迈克尔逊干涉仪[J].中国激光,1997,24(10):891~894.
    [23] G.A.Cranch, R.Crickmore, C.K.Kirkendall et al.. Acoustic performance of a large-aperture, seabed , fiber-optic hydrophone array[J]. Acoustical Societyof America, 2004,115(6):2848~2858.
    [24] Ni Ming, Yang Huayong Xiong Shuidong et al.. Investigation of polarization induced fading in fiber-optic interferometers with polarization based polarization diversity receivers[J]. Applied Optics, 2006, 45(11):1~4.
    [25] A.D.Kersey, M.J.Marrone, Optimization and Stabilization of Visibilitu in Interferometric Fiber-Optic Sensors Using Input-Polarization Control[J]. Lightwave Technology, 1988,6(10): 1599~1609.
    [26]李东,张晓晖,黄俊斌.光纤干涉仪输入光偏振态反馈控制理论分析[J].激光技术,2006,30(2):126~129.
    [27] M.J.Marrone, A.D.Kersey, A.Dandridge. Input Polarization Control Scheme for Addressing Polarization Induced Fading in Multiplexed Interferometric Sensor Arrays[J]. Distributed and Multiplexed Fiber Optic Sensors, 1991,1586:194~202 .
    [28] Y.S Boger, M.Tur. Polarization-Induced visibility Limits in Interferometric Fibre-Optic Sensor Arrays[J]. Electronics Letters,1991,27(8):622~623.
    [29]苑克娥,梅海平,饶瑞中.光纤干涉系统光学湍流测量原理及其偏振噪声问题的分析[J].量子电子学报,2007,24(3): 347~350.
    [30]李东,张晓晖,黄俊斌等.非平衡光纤Mach-Zehnder干涉仪偏振衰落及相位噪声分析[J].激光与红外,2005,30(2):126~129.
    [31]吴悦峰,肖浩,张松伟等.基于法拉第旋转镜的Michelson干涉仪偏振相位噪声研究[J].光电子·激光,2008,19(11):1446~1449.
    [32]李东,黄卫东,曾文锋等.输入光偏振态对光纤干涉仪条文可视度的影响[J].激光与红外,2006,36(8):703~706.
    [33] J.I Arce-Diego, J.Echevarria et al..Temperature dependence on the visibility limits in fibre-optic Michelson interferometric sensors with birefringence compensation[J].
    [34]熊水东,光纤矢量水听器研究,国防科技大学博士论文,2003.
    [35]宋微微,降低干涉型光纤传感器本底噪声方案的研究,哈尔滨工程大学硕士论文,2007.
    [36] L.A.Ferreira, J.L.Santos, F.Farahi. Polarization-Induced noise in a fiber-optic Michelson interferometer with Faraday rotator mirror elements[J]. Applied Optics, 1995, 34(28): 6399~6402.
    [37]石顺祥,张海星,刘劲松,物理光学与应用光学,陕西:西安电子科技大学出版社,2003.
    [38]叶玉堂,饶建珍,肖峻,光学教程,北京:清华大学出版社,2005.
    [39]张雪原,法拉第镜式光学电流互感器的理论研究,哈尔滨工程大学硕士论文,2004.
    [40]齐龙舟,肖浩,李芳等.光纤激光水听器消偏振衰落技术研究[J].传感与微系统,2008,27:21~23.
    [41]王光辉,吴福全,徐世昌.法拉第旋转角测量的同向检测法[J].光电子.激光,2004,15(12):1477~1478.
    [42] Boyain A R, Martinez-Leon Cruz J L. Low-frequency and high-frequency all-fiber modulators based on birefringence modulation [J]. App Opt, 1999, 38(30) :6278~6283.
    [43] Kersey, Marrone, Dandridge. Analysis of Input-Polarization-Induced Phase Noise in Interferometric Fiber-Optic Sensors and Its Reduction using Polarization Scrambling[J]. Lightwave Technology, 1990, 8(6): 838~845.
    [44]张海良,光学消偏器原理与研究,国防科技大学硕士论文,2003.
    [45]季家镕,高等光学教程,北京:科学出版社,2007.

© 2004-2018 中国地质图书馆版权所有 京ICP备05064691号 京公网安备11010802017129号

地址:北京市海淀区学院路29号 邮编:100083

电话:办公室:(+86 10)66554848;文献借阅、咨询服务、科技查新:66554700