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Optica Publishing Group
  • Conference on Lasers and Electro-Optics
  • OSA Technical Digest (Optica Publishing Group, 2002),
  • paper CWH2

Effects of Dispersion in a Polarimetric fiber Laser Sensor with Highly Birefringent Fiber Grating Reflectors

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Abstract

Fiber laser sensors have found strong interest due to inherent advantages such as a frequency-encoded output, high resolution, and a compact inline design.1,2 Here, we consider a polarimetric fiber laser sensor for fluid pressure3 with highly biréfringent fiber grating reflectors and show that the grating dispersion can be employed to significantly improve the resolution into the range of a few ppm of the full scale signal. The laser consists of two identical sections of Er-doped elliptical- core fiber with a 90° offset in the angular orientation of their cores (Fig. la). The gratings are written into the birefringent fibers with equal Bragg wavelengths near 1535 nnt and a width of 320 pm (for polarized light). The reflection maxima for the two biréfringent axes are separated by Δλbiref = 60 pm. Due to the 90°-splice the reflection peaks for x and y polarized light are interchanged in wavelength at the two gratings. For both polarizations the laser oscillates on a few longitudinal modes with wavelengths in the central dip between the reflection maxima. Fluid pressure applied to one of the two fiber sections introduces a differential phase shift between the two orthogonal polarizations4 which can be observed as a change in the polarization mode beat (PMB) frequencies.3 Phase shifts in the two fiber sections caused by a common temperature change cancel each other.

© 2002 Optical Society of America

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