Abstract

A novel technique combining Brillouin phase-shift measurements with Brillouin dynamic gratings (BDGs) reflectometry in polarization-maintaining fibers is presented here for the first time. While a direct measurement of the optical phase in standard BDG setups is impractical due to non-local phase contributions, their detrimental effect is reduced by ~4 orders of magnitude through the coherent addition of Stokes and anti-Stokes reflections from two counter-propagating BDGs in the fiber. The technique advantageously combines the high-spatial-resolution of BDGs reflectometry with the increased tolerance to optical power fluctuations of phasorial measurements, to enhance the performance of fiber-optic strain sensors. We demonstrate a distributed measurement (20cm spatial-resolution) of both static and dynamic (5kHz of vibrations at a sampling rate of 1MHz) strain fields acting on the fiber, in good agreement with theory and (for the static case) with the results of commercial reflectometers.

Highlights

  • Brillouin dynamic sensing is of importance in many applications [1]

  • The SA techniques employ a tunable laser source (TLS) adjusted to the linear region of the slope of either the reflection spectrum of a fiber Bragg grating (FBG) [8] or the intrinsic Brillouin gain spectrum (BGS) [9], such that changes induced by measurand variations are translated to changes in the measured quantity

  • Problems still remain and new ones are frequently discovered, as evidenced by [13], where it was shown that the BGS linewidth broadens with increasing pump power, which affects the performance of the slope-assisted Brillouin optical time-domain analysis (SA-Brillouin Optical Time Domain Analysis (BOTDA)) techniques, indicating an additional drawback of techniques based on the direct detection of optical power

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Summary

Introduction

Recent implementations of the Brillouin Optical Time Domain Analysis (BOTDA) [2] and Brillouin Optical Correlation Domain Analysis (BOCDA) [3] techniques, have demonstrated sampling rates of the order of kilohertz's with a centimetric spatial resolution (10cm over a range of 145m for the fully distributed case of [2] and 3cm over 6m for the random access approach of [3]). Slopeassisted (SA) techniques, using a single (or at most a few) pair(s) of pump and probe frequencies can be much faster As such, they have played a key role in taking the Brillouin distributed fiber optic sensing to the fast dynamic regime [1, 4], including demonstrations of its practical utilization for monitoring the propagation of mechanical waves [5,6] (for the use of slope-assisted interrogation of a fiber-Bragg grating see [7]). Problems still remain and new ones are frequently discovered, as evidenced by [13], where it was shown that the BGS linewidth broadens with increasing pump power (with obvious ramifications on its shape and slopes), which affects the performance of the slope-assisted Brillouin optical time-domain analysis (SA-BOTDA) techniques, indicating an additional drawback of techniques based on the direct detection of optical power

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