Radio-frequency unbalanced M-Z interferometer for wavelength interrogation of fiber Bragg grating sensors.

The optical unbalanced Mach-Zehnder interferometer (UMZI) has attracted significant interests for interrogation of FBG sensors owing to its excellent advantages in sensitivity, resolution, and demodulation speed. But this method is still limited to dynamic measurements due to its poor stability and reliability when used for quasi-static detections. Here, we propose for the first time, to the best of our knowledge, a radio-frequency unbalanced M-Z interferometer (RF-UMZI) for interrogation of FBG sensors, which, owing to its operation in an incoherent rather than a coherent regime, provides an ideal solution for the existing stability problem of the conventional UMZI, with remarkable features of adjustable resolution and potentially extremely high sensitivity. A dispersion compensation fiber (DCF) and single-mode fiber (SMF) with a small length difference are served as the two unbalanced arms of the RF interferometer. The induced differential chromatic dispersion transfers the wavelength shift of the FBG to the change of the RF phase difference between the two interferometric carriers, which ultimately leads to the variation of the RF signal intensity. An interrogation of a strain-turned FBG was accomplished and a maximum sensitivity of 0.00835  a.u./με was obtained, which can easily be further improved by more than two orders of magnitude through various fiber dispersion components. Finally, the stability of the interrogation was tested.

[1]  A. Kersey,et al.  High-resolution fibre-grating based strain sensor with interferometric wavelength-shift detection , 1992 .

[2]  A. Kersey,et al.  Multiplexed fiber Bragg grating strain-sensor system with a fiber Fabry - Perot wavelength filter. , 1993, Optics letters.

[3]  Michael A. Davis,et al.  Fiber grating sensors , 1997 .

[4]  K. Hill,et al.  Fiber Bragg grating technology fundamentals and overview , 1997 .

[5]  G. Johnson,et al.  Fiber Bragg grating interrogation and multiplexing with a 3/spl times/3 coupler and a scanning filter , 2000, Journal of Lightwave Technology.

[6]  Anbo Wang,et al.  Grating-assisted demodulation of interferometric optical sensors. , 2003, Applied optics.

[7]  Sien Chi,et al.  Long-distance FBG sensor system using a linear-cavity fiber Raman laser scheme , 2004 .

[8]  A. Willner,et al.  Practical Solutions to Polarization-Mode-Dispersion Emulation and Compensation , 2006, Journal of Lightwave Technology.

[9]  José Capmany,et al.  Microwave photonics combines two worlds , 2007 .

[10]  Xinyong Dong,et al.  Intensity-modulated fiber Bragg grating sensor system based on radio-frequency signal measurement. , 2008, Optics letters.

[11]  N. Pleros,et al.  Two dimensional polymer-embedded quasi-distributed FBG pressure sensor for biomedical applications. , 2010, Optics express.

[12]  H. Xia,et al.  Ultrafast and Precise Interrogation of Fiber Bragg Grating Sensor Based on Wavelength-to-Time Mapping Incorporating Higher Order Dispersion , 2010, Journal of Lightwave Technology.

[13]  Kazuo Hotate,et al.  Reduction of polarization-fluctuation induced drift in resonator fiber optic gyro by a resonator with twin 90 degrees polarization-axis rotated splices. , 2010, Optics express.

[14]  T. Eidam,et al.  The impact of modal interference on the beam quality of high-power fiber amplifiers. , 2011, Optics express.

[15]  Lei Wang,et al.  Monitoring Thermal Effect in Femtosecond Laser Interaction With Glass by Fiber Bragg Grating , 2011, Journal of Lightwave Technology.

[16]  Tao Wei,et al.  Optical fiber sensor based on a radio frequency Mach-Zehnder interferometer. , 2012, Optics letters.

[17]  Jie Huang,et al.  Spatially continuous distributed fiber optic sensing using optical carrier based microwave interferometry. , 2014, Optics express.

[18]  Deming Liu,et al.  Wavelength interrogation of fiber Bragg grating sensors based on crossed optical Gaussian filters. , 2015, Optics letters.