Modulation induced transient chirping in single frequency lasers

Wavelength excursions with magnitudes as large as 6 A are seen to occur in single frequency lasers (both C3and DFB) during a transition from one power level to another. The wavelength shifts briefly toward shorter wavelengths and then back to the equilibrium value during turn-on and toward longer wavelengths and back during turn-off. These excursions, which are well explained by a model in which the carrier density is temporarily driven out of equilibrium by a change in injection current, last for hundreds of picoseconds or about one half of the relaxation resonance period. This time dependent behavior gives rise to a dramatic degradation of lightwave system performance with increasing bit rate. Laser structures which heavily damp the relaxation resonance peak are seen to exhibit the least chirp and to perform best in high speed transmission systems.

[1]  High-speed 1.55 μm single-longitudinal-mode ridge waveguide C3 laser , 1983 .

[2]  N. A. Olsson,et al.  High‐speed direct single‐frequency modulation with large tuning rate and frequency excursion in cleaved‐coupled‐cavity semiconductor lasers , 1983 .

[3]  J. P. van der Ziel,et al.  Spectral broadening of pulsating AlxGa1-xAs double heterostructure lasers , 1979 .

[4]  Ivan P. Kaminow,et al.  120 km lightwave transmission experiment at 1 Gbit/s using a new long-wavelength avalanche photodetector , 1984 .

[5]  P. P. Smyth,et al.  1.2 Gbit/s optical fibre transmission experiment over 113.7 km using a 1.528 μm distributed-feedback ridge-waveguide laser , 1984 .

[6]  Richard A. Linke,et al.  130 KM TRANSMISSION EXPERIMENT AT 2 GB/S USING SILICA-CORE FIBER AND A VAPOR PHASE TRANSPORTED DFB LASER. , 1984 .

[7]  J. E. Midwinter A study of intersymbol interference and transmission medium instability for an optical fibre system , 1977 .

[8]  C. A. Burrus,et al.  Picosecond frequency chirping and dynamic line broadening in InGaAsP injection lasers under fast excitation , 1983 .

[9]  R. A. Linke,et al.  Transient chirping in single-frequency lasers: lightwave systems consequences , 1984 .

[10]  K. Kishino,et al.  Wavelength variation of 1.6 µm wavelength buried heterostructure GaInAsP/InP lasers due to direct modulation , 1982, IEEE Journal of Quantum Electronics.

[11]  K. Nakagawa,et al.  Chirp pulse transmission through a single-mode fibre , 1982 .

[12]  Richard A. Linke,et al.  High Speed Laser Driving Circuit And Gigabit Modulation Of Injection Lasers , 1983, Optics & Photonics.

[13]  H. Toba,et al.  Injection-locking technique applied to a 170 km transmission experiment at 445•8 Mbit/s , 1984 .

[14]  Dynamic linewidth of amplitude-modulated single-longitudinal-mode semiconductor lasers operating at 1.5 μm wavelength , 1984 .

[15]  K. Ogawa,et al.  Very-high-speed back-illuminated InGaAs/InP PIN punch-through photodiodes , 1981 .

[16]  Ivan P. Kaminow,et al.  High-frequency characteristics of directly modulated InGaAsP ridge waveguide and buried heterostructure lasers , 1984 .

[17]  R. Linke Direct gigabit modulation of injection lasers - Structure-dependent speed limitations , 1984, Journal of Lightwave Technology.

[18]  T. Koch,et al.  Nature of wavelength chirping in directly modulated semiconductor lasers , 1984 .

[19]  G. Thompson,et al.  A theory for filamentation in semiconductor lasers including the dependence of dielectric constant on injected carrier density , 1972 .