This paper reports the design optimization of a novel tunable dual wavelength erbium doped fiber ring laser. The effects of pump wavelength, active fiber length, and coupling ratio on threshold pump power, output power, and side mode suppression ratio (SMSR) of the lasers are investigated. Pumping a
The interaction of dual wavelength solitons in fiber laser
โ Scribed by W.C. Chen; Z.C. Luo; W.C. Xu
- Publisher
- John Wiley and Sons
- Year
- 2009
- Tongue
- English
- Weight
- 140 KB
- Volume
- 6
- Category
- Article
- ISSN
- 1612-2011
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โฆ Synopsis
The dual wavelength solitons with 41.2 nm spectral separation are achieved simultaneously via nonlinear polarization rotation technique. One is the picosecond soliton, the other is femtosecond soliton. The direct interaction of two solitons does not happen firstly for the temporal separation between them is beyond 5 times of their duration. When the continuous wave (CW), as the roles to cause the direct soliton interaction through shifting the central wavelength of the solitons, are excited to appear, the interaction of dual wavelength solitons happens. There are some dips present on the femtosecond soliton spectra, indicating the interaction between dual wavelength solitons. The power of CW affects the intensities of dips in the spectra and the pulse numbers and relative position of pulse bunches. The more the power of CW, the more the intensities of the dips at the femtosecond soliton spectra are. 5.0 dB /div -12.0 dBm -37.0 dBm -62.0 dBm 1530.0 nm 8.0 nm/div 1570.0 nm in Vac 1610.0 nm Normal (A) Threshold CutLv1: ฮปc: ฮฮป: 3.0 dB
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