Abstract:Abstract-The authors demonstrate the drift in frequency of a static sampled-grating distributed Bragg reflector (SG DBR) laser module when it is subjected to direct modulation. The magnitude of drift and its settling time is characterized as a function of the index of modulation. Results show that when the directly modulated SG DBR is optically filtered, as in a dense wavelength-division-multiplexed system, a power penalty of 6.7 dB is incurred in comparison to the unfiltered case.
IndexTerms-Dense wavelength-… Show more
“…Nevertheless, one of the main drawbacks of this technique is the frequency fluctuation (chirp) imposed on the signal. This frequency chirp can impair the overall performance of WDM systems in two ways, either by drifting out of the receiving filter's bandwidth [2] and/or by drifting into the neighboring channel's filter bandwidth thereby causing cross channel interference. Additionally, the chirped signal would be more prone to dispersion effects in the fiber.…”
Section: Novel Frequency Chirp Compensation Scheme Formentioning
Abstract-The authors demonstrate a compensation scheme to reduce the frequency chirp associated with directly modulated sampled grating distributed Bragg reflector tunable lasers. Experimental results obtained show that the direct modulation of the laser's gain section results in a large frequency chirp of 25 GHz. However, by simultaneous modulation of the laser's phase section this large frequency chirp can be significantly reduced.Index Terms-Direct intensity modulation, frequency chirp, optical fiber communications, tunable laser (TL), wavelength-division multiplexing (WDM).
“…Nevertheless, one of the main drawbacks of this technique is the frequency fluctuation (chirp) imposed on the signal. This frequency chirp can impair the overall performance of WDM systems in two ways, either by drifting out of the receiving filter's bandwidth [2] and/or by drifting into the neighboring channel's filter bandwidth thereby causing cross channel interference. Additionally, the chirped signal would be more prone to dispersion effects in the fiber.…”
Section: Novel Frequency Chirp Compensation Scheme Formentioning
Abstract-The authors demonstrate a compensation scheme to reduce the frequency chirp associated with directly modulated sampled grating distributed Bragg reflector tunable lasers. Experimental results obtained show that the direct modulation of the laser's gain section results in a large frequency chirp of 25 GHz. However, by simultaneous modulation of the laser's phase section this large frequency chirp can be significantly reduced.Index Terms-Direct intensity modulation, frequency chirp, optical fiber communications, tunable laser (TL), wavelength-division multiplexing (WDM).
“…Furthermore, the limitations of optical and thermal properties of candidate DBR materials make it challenging to obtain large wavelength tuning range. On the other hand, more sophisticated tunable lasers with wide tuning ranges have also been developed, such as sampled grating distributed Bragg reflector (SGDBR) lasers [2,6], superstructure grating (SSG) DBR lasers [7] and high-contrast-subwavelength-grating (HCG) reflector based surface-emitting lasers [8,9]. In addition to the fabrication difficulties involving gratings and/or multiple epitaxial growths, the requirements to the reflector bandwidth and reflectivity become even more stringent.…”
This paper presents the design and experimental study of a coupled-cavity laser based on the micromachining technology for wide tuning range and improved spectral purity. The core part of this design utilizes a deep-etched movable parabolic mirror to couple two identical Fabry-Pérot chips and thus allows the active adjustment of the cavity gap so as to optimize the mode selection and to increase the tuning range as well. In experiment, the laser achieves the single longitudinal mode output over 51.3 nm and an average side-mode-suppression ratio of 22 dB when the tuning current varies from 5.7-10.8 mA. The measured wavelength tuning speed is 1.2 micros and the single mode output is stable at any wavelength when the tuning current is varied within +/- 0.06 mA. Compared with the conventional fixed cavity gap coupled-cavity lasers, such design overcomes the phase mismatching and mode instability problems while maintaining the merit of high-speed wavelength tuning using electrical current.
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