Conference on Lasers and Electro-Optics 2017
DOI: 10.1364/cleo_at.2017.jtu5a.85
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Detrimental Effects in Brillouin Distributed Sensors Caused By EDFA Transient

Abstract: We investigate the deleterious effect and the error in Brillouin optical time-domain analyzers induced by the combination of a low extinction ratio pulse generation with the transient behavior of erbium-doped fiber amplifiers.

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Cited by 9 publications
(6 citation statements)
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“…In a well-designed BOTDA, a high extinction ratio (ER) pump pulse wave is employed. Therefore, the SBS-interaction between the probe and pump pedestal can be neglected [ 45 , 46 ]. As a result, the noise outside the time domain trace consists of classical noise only.…”
Section: Resultsmentioning
confidence: 99%
“…In a well-designed BOTDA, a high extinction ratio (ER) pump pulse wave is employed. Therefore, the SBS-interaction between the probe and pump pedestal can be neglected [ 45 , 46 ]. As a result, the noise outside the time domain trace consists of classical noise only.…”
Section: Resultsmentioning
confidence: 99%
“…However, this amplification is not useful for sensing. In case of a strong probe wave, not only the pulse but also the pedestals (especially the trailing pedestal) will deplete, which lead to severe distortions on the BOTDA traces (see Figure 13(b)) [75,76].…”
Section: Higher Pulse Extinction Ratiomentioning
confidence: 99%
“…For a conventional MZM, the ER is only 20 dB but can be enhanced up to 30 dB with special designs. Higher ERs of more than 40 dB can be achieved with switching type semiconductor optical amplifiers (SOA) and a 60 dB ER with RF switches [75,76].…”
Section: Higher Pulse Extinction Ratiomentioning
confidence: 99%
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“…The imaginary part of Equation (1) is the Brillouin phase spectrum and the real part represents the BGS which is approximated by a Lorentzian shape [24]. Provided that the pump depletion is negligible and the extinction ratio (ER) of the pump pulse is infinitely high so that no pump leakage-probe interaction is considered [29,30,31], the local Brillouin gain gB that will be experienced by the probe wave at position z is given by gB(ω,z)=prefixexp[GB(ω)Leff]·prefixexp[2αz] where α is the linear loss coefficient of the fiber, Leff=[1exp(αL)]/α represents the effective length, L=vcT/2 has the same expression as the spatial resolution, where vc is the speed of light in the fiber and T is the pulse width.…”
Section: Simulationmentioning
confidence: 99%