Handbook of Optical Fibers 2017
DOI: 10.1007/978-981-10-1477-2_7-1
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Distributed Brillouin Sensing: Time-Domain Techniques

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Cited by 18 publications
(34 citation statements)
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“…Results in Figure 6 point out that the BFS estimations obtained by polynomial fitting match very well the values obtained by nonlinear double-Gaussian fitting, especially under large applied strains (i.e., large masses), when the two BGS peaks do not highly overlap. The obtained BFS values indeed also match the expected Brillouin spectral shifts based on the applied strain and the Brillouin strain coefficient of ~0.05 MHz/με [ 1 , 2 ]. In this large strain range, the evaluated root-mean-square BFS difference is 0.18 MHz and 1.1 MHz for the first and second peaks, respectively.…”
Section: Resultssupporting
confidence: 70%
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“…Results in Figure 6 point out that the BFS estimations obtained by polynomial fitting match very well the values obtained by nonlinear double-Gaussian fitting, especially under large applied strains (i.e., large masses), when the two BGS peaks do not highly overlap. The obtained BFS values indeed also match the expected Brillouin spectral shifts based on the applied strain and the Brillouin strain coefficient of ~0.05 MHz/με [ 1 , 2 ]. In this large strain range, the evaluated root-mean-square BFS difference is 0.18 MHz and 1.1 MHz for the first and second peaks, respectively.…”
Section: Resultssupporting
confidence: 70%
“…This setup employs a 10 mW distributed feedback (DFB) laser operating at 1550 nm, whose light is split into two branches. In the upper branch (10%), an electro-optic modulator (EOM) with high extinction ratio is used to generate 20 ns optical pulses (providing 2 m spatial resolution) with about 40 dB extinction ratio, which is required to eliminate any continuous-wave Brillouin response along the sensing fiber [ 2 ]. Optical pulses are then boosted by an erbium-doped fiber amplifier (EDFA) and launched into the sensing fiber through an optical circulator with an optical power of ~100 mW (limit imposed by the onset of nonlinear effects such as modulation instability [ 14 ]).…”
Section: Methodsmentioning
confidence: 99%
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“…DOFS emerged with the development of a technique called optical time-domain reflectometer (OTDR). There are three main types of OTDR sensing mechanism, which are based on Brillouin [20][21][22][23][24], Rayleigh [25][26][27][28][29], and Raman scattering [30,31].…”
Section: Introductionmentioning
confidence: 99%