Abstract

The forward and backward cascaded stimulated Brillouin scattering(SBS) in the backward pumped S band distributed G652 fiber Raman amplifier have been researched, pumped by the tunable power at 1428nm fiber Raman laser and signal source is a tunable power external cavity laser (ECL) with narrow spectral bandwidth (<100MHz). The threshold power of backward Stokes the first and second stimulated Brillouin scattering SB<sub>1</sub><sup>-</sup> and SB<sub>2</sub><sup>-</sup> in the backward pumped S band distributed fiber Raman amplifier is 5mW and 67.6mW, respectively. The Stokes stimulated Brillouin scattering lines is amplified by fiber Raman amplifier and fiber Brillouin amplifier. The total G<sub>A</sub> is production of the gain of Raman G<sub>R</sub> and the gain of Brillouin amplifier G<sub>B</sub>. G<sub>A</sub>=G<sub>R</sub>×G<sub>B</sub>. In experimental work, the saturation gain of SB<sub>1</sub><sup>-</sup> and SB<sub>2</sub><sup>-</sup> is about 50dB and 65dB respectively and the saturation gain of 25km G652 backward FRA is about 25dB, so the gain of backward fiber Brillouin amplifier SB<sub>1</sub><sup>-</sup> and SB<sub>2</sub><sup>-</sup> are about 25dB and 40dB, respectively. The forward SBS does not obey the common theory that only weakening backward-SBS lines existed, according to conservation of energy and momentum and wave vector selected rule. Because the wave-guide characters weaken the wave vector rule, but the forward transmit sound wave-guide forward Brillouin scattering lines are generated and amplified in S band G652 FRA. The stimulated threshold power of the forward first Stokes SBS (SB<sub>1</sub><sup>-</sup> ) in the backward pumped FRA is 6.6mW. In experimental work, the saturation gain of SB<sub>1</sub><sup>-</sup> is about 49dB and the saturation gain of 25km G652 backward FRA is about 10dB, so the gain of SB<sub>1</sub><sup>-</sup> in the forward fiber Brillouin amplifier is about 39dB.

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