Power Thresholds and Pump Depletion in Brillouin Fiber Amplifiers

The Brillouin fiber amplifier (BFA) has been used in Brillouin optical time (frequency) domain analyzer based sensors. The performance of this sensor depends on pump depletion which occurs when the threshold is reached and when the Brillouin gain is saturated. Although threshold definitions are common for Brillouin fiber generators (BFG), there is no explicit threshold definition for BFA. More importantly we find the maximum gain point corresponds to the optimized distributed sensing system where the depletion effect remains small to moderate. We find that only the method based on the determination of the power for which the pump becomes depleted, and hence, the Stokes gain saturated (i.e. inflexion method), remains valid for BFA. We also derive an analytical relation accounting for the various sensor key parameters such as fiber type and length as well as input Stokes power. The thresholds obtained with the analytical relation are within 10% of experimental and numerical values, which is maximum power that can be launched for a given optimum sensing configuration.

[1]  X. Bao,et al.  Theoretical study of the effect of slow light on BOTDA spatial resolution. , 2006, Optics express.

[2]  Luc Thévenaz,et al.  Gain-assisted pulse advancement using single and double Brillouin gain peaks in optical fibers. , 2005, Optics express.

[3]  Iñigo Salinas,et al.  Stimulated Brillouin scattering gain profile characterization by interaction between two narrow-linewidth optical sources. , 2005, Optics express.

[4]  A. Schweinsberg,et al.  Tunable all-optical delays via Brillouin slow light in an optical fiber , 2005, (CLEO). Conference on Lasers and Electro-Optics, 2005..

[5]  Luc Thévenaz,et al.  Observation of pulse delaying and advancement in optical fibers using stimulated Brillouin scattering. , 2005, Optics express.

[6]  M. V. Deventer,et al.  Polarization properties of stimulated Brillouin scattering in single-mode fibers , 1994 .

[7]  Boyd,et al.  Noise initiation of stimulated Brillouin scattering. , 1990, Physical review. A, Atomic, molecular, and optical physics.

[8]  Polina Bayvel,et al.  Solutions of the SBS equations in single mode optical fibres and implications for fibre transmission systems , 1990 .

[9]  D. Jackson,et al.  Potential of stimulated Brillouin scattering as sensing mechanism for distributed temperature sensors , 1989 .

[10]  R. M. Derosier,et al.  Performance of a WDM network based on stimulated Brillouin scattering , 1989, IEEE Photonics Technology Letters.

[11]  T. Horiguchi,et al.  Tensile strain dependence of Brillouin frequency shift in silica optical fibers , 1989, IEEE Photonics Technology Letters.

[12]  N. A. Olsson,et al.  Cancellation of fiber loss by semiconductor laser pumped Brillouin amplification at 1.5 μm , 1986 .

[13]  D. Cotter Observation of stimulated Brillouin scattering in low-loss silica fibre at 1.3 μm , 1982 .

[14]  R. Smith Optical power handling capacity of low loss optical fibers as determined by stimulated Raman and brillouin scattering. , 1972, Applied optics.

[15]  SERIES G: TRANSMISSION SYSTEMS AND MEDIA, DIGITAL SYSTEMS AND , 2020 .

[16]  Mario F. S. Ferreira,et al.  Analysis of the gain and noise characteristics of fibre Brillouin amplifiers , 1994 .