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Flexibly tunable multiwavelength erbium-doped fiber laser based on four-wave mixing effect in dispersion-shifted fibers

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Abstract

We experimentally demonstrate a flexibly tunable multiwavelength erbium-doped fiber laser based on degenerate four-wave mixing in a dispersion-shifted fiber. We successfully achieve the stable operation of the multiwavelength erbium-doped fiber laser at room temperature. The number of channels and wavelength spacing of the proposed multiwavelength laser can be controlled by the combination of two polarization maintaining fiber segments in the intracavity Lyot-Sagnac filter. We achieve 1.0 nm-spacing eleven channel and 0.8 nm-spacing seventeen channel lasing wavelengths at room temperature. The lasing wavelength of multiwavelength fiber laser can be also controlled by the polarization controller.

©2005 Optical Society of America

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Figures (4)

Fig.1.
Fig.1. Schematic of the proposed multiwavelength EDF laser based on degenerate four-wave mixing in the DSF. The multiwavelength operation can be achieved by the tunable PMF Lyot-Sagnac filter (dashed square). PC: Polarization controller. LD: Laser diode. EDF: Erbium-doped fiber. DSF: Dispersion-shifted fiber. PMF: Polarization-maintaining fiber. OSA: Optical spectrum analyzer.
Fig. 2.
Fig. 2. Output spectra of the tunable multiwavelength EDF laser depending on the combination of PMF segments in the Lyot-Sagnac filter. The extinction ratio was as high as ~ 50 dB. (a) Δλ = 1.0 nm, number of channels = 11. (b) Δλ = 0.8 nm, number of channels = 17.
Fig.3.
Fig.3. (a) Output spectra of the proposed tunable multiwavelength EDF laser when the polarization angle of the quarter-wave plate was 0° (solid line) and 90° (solid line), respectively, and (b) the continuous tuning of lasing wavelengths with the variation of polarization angle of the quarter-wave plate.
Fig. 4.
Fig. 4. Power fluctuation of the multiwavelength EDF laser with scanned time. The power fluctuation was less than ~0.6 dB.

Equations (2)

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Δ P i Δ P i + 1 = δ ( ω i ω i + 1 P i + 1 ω i + 1 ω i P i + 2 ( P i + 1 P i ) ) δ ( P i + 1 P i ) ,
Δ λ = λ 2 Δ n ( L 1 ± L 2 ) ,
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