2006 Optical Fiber Communication Conference and the National Fiber Optic Engineers Conference 2006
DOI: 10.1109/ofc.2006.215715
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Sub-picosecond pulse generation at 134 GHz using a quantum dash-based Fabry-Perot laser emitting at 1.56 /spl mu/m

Abstract: We report on 800 fs pulse generation, at 134 GHz, using a Fabry-Perot quantum dash laser at 1.56 Mm. A 50 kHz RF spectral linewidth at 42 GHz is also demonstrated.

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Cited by 16 publications
(23 citation statements)
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References 5 publications
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“…As discussed in section 3.2.2, a 45 GHz CW mode locking from monosection InAs/InP Qdot/Qdash laser was first demonstrated by Renaudier et al [120]. Following this report was the detailed investigation by Gosset et al [287] who demonstrated 134 GHz pulse generation from 340 µm long 6-stack InAs/InGaAsP DaWELL laser under CW operation. The 1.56 µm device exhibited deconvolved sub-picosecond pulse width of 800 fs without any pulse compression scheme and 0.46 time bandwidth product.…”
Section: Self-pulsationmentioning
confidence: 89%
See 1 more Smart Citation
“…As discussed in section 3.2.2, a 45 GHz CW mode locking from monosection InAs/InP Qdot/Qdash laser was first demonstrated by Renaudier et al [120]. Following this report was the detailed investigation by Gosset et al [287] who demonstrated 134 GHz pulse generation from 340 µm long 6-stack InAs/InGaAsP DaWELL laser under CW operation. The 1.56 µm device exhibited deconvolved sub-picosecond pulse width of 800 fs without any pulse compression scheme and 0.46 time bandwidth product.…”
Section: Self-pulsationmentioning
confidence: 89%
“…Passive mode locking employing classical two-section InAs/InGaAsP Qdash laser with one gain and one absorber section was first demonstrated by Gosset et al [287] who measured 47 kHz RF linewidth from a 6-stack Qdash laser with 940 µm gain and 180 µm absorber sections. A pulsation frequency of 43.6 GHz was measured at 169 mA CW current and with no significant effect of applied bias on the absorber section.…”
Section: Two-sectionmentioning
confidence: 99%
“…There has been extensive study of semiconductor MLLs based on quantum well (QW) and bulk active layers [4,5,11,17,18,30,31]. More recently, quantum dash (QDash) and quantum dot (QD)-based MLLs have attracted significant attention [9,16,23,40]. One of the most interesting features of QDash lasers is that passive mode-locking can be easily achieved without any saturable absorber, and that the free-running spectral linewidth (FRSL) of modebeating note in these passively locked QDash lasers is very narrow, one or two orders of magnitude narrower than those in their QW or bulk counterparts [16,23].…”
Section: Introductionmentioning
confidence: 99%
“…But unlike the MLLD that have an absorber element that locks the static phases of the longitudinal modes by periodically creating a positive net gain window when saturated by the optical field inside the laser cavity, the laser used in this, which is a single section semiconductor lasers, has other types of nonlinear processes in the gain medium, such as four wave mixing, that are able to set up a phase correlation among the modes which also become equally separated in frequency despite intra-cavity dispersion. This kind of ML mechanism has been experimentally observed for quantum-well [3,8], quantum-dash [9] and quantum-dot [10] based gain media. However, the need of external dispersion compensation in order to obtain near transform limited pulses [3,13].…”
Section: Passive Modementioning
confidence: 64%