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Nonlinear Fiber Optics - 4 ed. Agrawal

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9.5. Brillouin <strong>Fiber</strong> Lasers 359<br />

Figure 9.19: Schematic of a Brillouin fiber laser with two fiber loops containing optical circulators<br />

(cir2 and cir3) and acting as two mirrors of a Fabry–Perot cavity. WSC stands for a<br />

wavelength-selective coupler. (After Ref. [146]; c○2005 OSA.)<br />

60 nm was realiz<strong>ed</strong> in a 2005 experiment [146]. Figure 9.19 shows the cavity design<br />

schematically for this laser. Two fiber loops act as mirrors because of the emb<strong>ed</strong>d<strong>ed</strong><br />

optical circulators. The SBS gain is provid<strong>ed</strong> by 8.8 km of single-mode fiber (SMF-28),<br />

pump<strong>ed</strong> with an external-cavity semiconductor laser tunable from 1520 to 1620 nm.<br />

The 10-m-long EDFA is pump<strong>ed</strong> at 980 nm using another semiconductor laser. The<br />

tuning range and the number of Stokes line produc<strong>ed</strong> by such a laser vari<strong>ed</strong> with the<br />

relative power levels of two pump lasers.<br />

In an interesting configuration, the SBS pump is generat<strong>ed</strong> internally through selfse<strong>ed</strong>ing,<br />

and only one laser is ne<strong>ed</strong><strong>ed</strong> for pumping the EDFA [145]. Figure 9.20 shows<br />

the laser design schematically. The ring cavity contains a 16-m-long EDFA and 5-km<br />

of standard fiber to produce SBS gain. A Sagnac loop, built using a polarizationmaintaining<br />

fiber (PMF), is us<strong>ed</strong> as a mirror. This mirror doubles the SBS gain as light<br />

passes through the 5-km fiber twice during each round trip. The Brillouin pump is first<br />

Figure 9.20: Schematic of a self-se<strong>ed</strong><strong>ed</strong> Brillouin fiber laser: OC, PC, PMF, and OSA stand for<br />

optical circulator, polarization controller, polarization-maintaining fiber, and optical spectrum<br />

analyzer, respectively. (After Ref. [145]; c○2005 OSA.)

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