2017
DOI: 10.1364/oe.25.016059
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Temperature-strain discrimination in distributed optical fiber sensing using phase-sensitive optical time-domain reflectometry

Abstract: A method based on coherent Rayleigh scattering distinctly evaluating temperature and strain is proposed and experimentally demonstrated for distributed optical fiber sensing. Combining conventional phase-sensitive optical time-domain domain reflectometry (ϕOTDR) and ϕOTDR-based birefringence measurements, independent distributed temperature and strain profiles are obtained along a polarization-maintaining fiber. A theoretical analysis, supported by experimental data, indicates that the proposed system for temp… Show more

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Cited by 76 publications
(42 citation statements)
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References 29 publications
(74 reference statements)
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“…The two tones were amplified by an erbium-doped fiber amplifier (EDFA), and then amplitude- The magnitude of Rayleigh back-scatter of coherent optical fields is extremely noisy [34,35].…”
Section: Experimental Setup and Proceduresmentioning
confidence: 99%
“…The two tones were amplified by an erbium-doped fiber amplifier (EDFA), and then amplitude- The magnitude of Rayleigh back-scatter of coherent optical fields is extremely noisy [34,35].…”
Section: Experimental Setup and Proceduresmentioning
confidence: 99%
“…The polarization handling devices based on PCFs filled with material, such as polarization splitters (PS) [20][21][22] and polarization rotators (PR) [23,24], have important applications in optical fiber sensing [25,26]. The PS could be divided into two fundamental modes (HE x 11 and HE y 11 ) and propagate them in different directions.…”
Section: Of 12mentioning
confidence: 99%
“…DOFS can provide physical information continuously all along the entire optical fiber length. The DOFS for short range and high resolution strain monitoring include optical time domain reflectometry (OTDR) [5], [6] and optical frequency domain reflectometry (φOFDR) [7], based on Rayleigh scattering induced by the refractive index inhomogeneity in optical fiber, and the measured position distance L to the detector is deduced by the travelling time of back scattered pulses τ in the optical fiber, τ=2nL/c, where n is the refractive index of the fiber and c is the light velocity in vacuum [8]. Table 1 shows a rough comparison of various parameters of the different DOFS.…”
Section: Principle and Experimentsmentioning
confidence: 99%