2008 International Conference on Advances in Electronics and Micro-Electronics 2008
DOI: 10.1109/enics.2008.25
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Directly Modulated Laser Intrinsic Parameters Optimization for WDM Systems

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Cited by 6 publications
(6 citation statements)
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“…The frequency chirp typically causes variations in pulse width, which combined with the fiber dispersion to degrade the digital system performance (Ahmed et al, 2014;del Río Campos et al, 2011;Hakki, 1992;Tucker, 1985;Yamamoto et al, 1987). Another serious limitation of frequency chirp is that it causes shifting in the output wavelength away from the actual laser wavelength, which is a critical issue in the directly modulated WDM systems in order to avoid channel interference (del Río Campos & Horche, 2008).…”
Section: Chirping Characteristics Of Direct Modulation Of Ldsmentioning
confidence: 99%
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“…The frequency chirp typically causes variations in pulse width, which combined with the fiber dispersion to degrade the digital system performance (Ahmed et al, 2014;del Río Campos et al, 2011;Hakki, 1992;Tucker, 1985;Yamamoto et al, 1987). Another serious limitation of frequency chirp is that it causes shifting in the output wavelength away from the actual laser wavelength, which is a critical issue in the directly modulated WDM systems in order to avoid channel interference (del Río Campos & Horche, 2008).…”
Section: Chirping Characteristics Of Direct Modulation Of Ldsmentioning
confidence: 99%
“…On the other hand, the adiabatic chirp refers to the frequency shift between the laser steady-state output powers at "1" and "0" levels (Ahmed et al, 2012). The adiabatic chirp causes a shift in the emitted wavelength, while the transient chirp causes variations in pulse width (del Río Campos & Horche, 2008). The parameters controlling frequency chirps are the linewidth enhancement factor (α-factor) (Henry, 1982;Osinski & Buus, 1987) and the gain suppression coefficient (ε) (Hangauer & Wysocki, 2015;Koch & Linke, 1986;Wang et al, 1993).…”
Section: Introductionmentioning
confidence: 99%
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