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Stable room-temperature multi-wavelength lasing realization in ordinary erbium-doped fiber loop lasers

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Abstract

A suppressant effect for mode competition of multi-wavelength lasing oscillations induced by deeply saturated effect in an ordinary erbium-doped fiber ring laser (EDFRL) was observed and experimentally investigated. Results show that the effect is helpful to obtain stable multi-wavelength lasing at room temperature in the EDFRL, which offers a new and simple approach to achieve stable multi-wavelength EDF lasing. Stable two- and three- wavelength lasing oscillations were achieved based on the effect in the ordinary EDFRL for the first time to our best knowledge. The multi-wavelength lasing oscillations were so stable integrated over smaller than 1 ms that the maximum power fluctuation over more than 30 minutes of observation was less than 0.1 dB and 0.5 dB for two-wavelength lasing with a spacing of 1.28 nm and 0.76 nm, respectively.

©2006 Optical Society of America

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Figures (7)

Fig. 1.
Fig. 1. Schematic diagram of the experimental setup
Fig. 2.
Fig. 2. Transmission spectrum of the SFBG.
Fig. 3.
Fig. 3. Output spectra of the multiwavelength EDFRL with (a) dual-wavelength lasing and (b) three-wavelength lasing achieved by adjusting the VOA.
Fig. 4.
Fig. 4. Power fluctuation of the multiwavelength EDFRL during scanning: (a) for dual-wavelength lasing, the power fluctuations are less than ~0.1 dB; (b) for three-wavelength lasing, the power fluctuations are less than ~0.8 dB.
Fig. 5.
Fig. 5. Power fluctuation of the multiwavelength EDFRL during scanning without the ISO. The maximum fluctuations are 1.25 dB at 1550.96 nm and 1.52 dB at 1552.24nm, respectively.
Fig. 6.
Fig. 6. Output spectra of the dual-wavelength EDFRL obtained using the two common FBGs. with 0.76 nm wavelength spacing.
Fig. 7.
Fig. 7. Power fluctuations of the dual-wavelength EDFRL using the two FBGs with different pump power. The maximum fluctuations for 20 mW, 35mW, 70 mW and 98 mW pump powers are (1.15, 1.56) dB, (1.10, 1.18) dB, (0.41, 0.66) dB and (0.49, 0.44) dB at wavelengths of 1550.38 nm and 1551.14 nm, respectively.
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