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(a) A cross sectional SEM image of the five-layer InAs/InP QDlaser core region and (b) a detailed structure for a single InAs/InP dot layer.

(a) A cross sectional SEM image of the five-layer InAs/InP QDlaser core region and (b) a detailed structure for a single InAs/InP dot layer.

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We have developed an InAs/InP quantum dot (QD) C-band coherent comb laser (CCL) module with actively stabilized absolute wavelength and power, and channel spacing of 34.462 GHz with ± 100 ppm accuracy. The total output power is up to 46 mW. The integrated average relative intensity noise (RIN) values of the lasing spectrum and a filtered single cha...

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... The most common family of devices used for the generation of wideband optical frequency combs are mode-locked lasers which emit short optical pulses by setting a fixed phase relationship between many lasing longitudinal modes [1,8]. The semiconductor laser-based frequency combs are a simple and low-cost solution with potential for use in photonic integrated circuits (PICs), exhibit a broad range of emission wavelengths, and have been demonstrated for a variety of laser technologies such as quantum well [9,10], quantum dot [11][12][13], quantum dash [14,15], and quantum cascade lasers [16]. Special attention has been drawn on quantum dot/dash combs as they promise ultrabroad gain bandwidth and ultrafast carrier dynamics, low threshold, low spontaneous emission rate, as well as large gain and saturable absorber saturation energy ratio, a critical parameter for the implementation of high-performance mode-locked lasers [17]. ...
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... An alternative method of stabilising the absolute frequency/wavelength of a comb generator [235] involves using (electrically) active wavelength locking with a stabilised narrowband optical filter (etalon) used to determine the desired optical frequency of one of the modes. ...
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... In comparison, semiconductor MLLs have the advantages of being electrically driven, while not requiring external high-power optical pumping, which makes them a great candidate for highly efficient, small-footprint, and low power consumption solutions for optical timedivision multiplexing [10] and wavelength-division multiplexing (WDM) systems [11]. In recent years, there has been significant attention paid to quantum dash (Q-dash) [12][13][14] and quantum dot (QD) MLLs [9,15,16] as flat-top comb sources, due to their properties of small linewidth enhancement factor, fast carrier dynamic-induced self-frequency modulation, and defect insensitivity, which make them an ideal platform for a reflection insensitive [17,18], temperature insensitive [19,20], and most importantly, direct-grown-on-Si light source [21][22][23][24][25][26]. ...
... For the extended time stability test that is also applied to a comb channel at 1317.69 nm, the wavelength variation is less than 1 GHz, as shown in the inset of Fig. 4(d). All the measurements are under free-running conditions, and it is believed that the combs can be further stabilized by the wavelength locker design with a feedback control loop [14]. ...
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... This work used Qdash MLL as a dual pump source for a wavelength conversion system. Next, another Qdot/Qdash MLLs were reported in [89], comprised of five layers and emitting in the C-band. By beating any consecutive modes of the comb lines of the Qdash MLLs, a high-quality beat tone of 34.46 GHz was generated. ...
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... As we will see in the next section, an important parameter for optical communication is the coherence of the comb lines. Compared to the electro-optic modulator where the linewidth RF beat note can be less than 1 Hz, the one of the quantum dot lasers has been found to range from several kHz to MHz [181]. ...
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In this work, we study the nonlinear dynamics of laser diodes optically injected with frequency combs.We first theoretically and experimentally analyze the nonlinear dynamics of edge-emitting lasers (EELs) from an optical injection of frequency combs. The injection parameters and injected comb properties are varied to unveil several locked and unlocked dynamics. For large enough injection strength and over a large detuning range, the injection locking bifurcates to a time-periodic dynamics corresponding to an optical frequency comb that extends the injected comb to a much broader optical spectrum. A bifurcation analysis reveals a cascade harmonic frequency comb dynamics leading to a significant increase in the output comb lines. We have also used the injection parameters, comb properties, and injection current to control the new comb properties. We secondly analyze the nonlinear dynamics and polarization properties in vertical-cavity surface-emitting lasers (VCSELs) subject to orthogonal optical injection with frequency combs experimentally. Most importantly, the VCSEL shows two frequency combs with orthogonal polarization from a single device for some injection parameters. We also demonstrate the possibility to control the single or two polarizations comb repetition rate through harmonic frequency combs generation. We finally present experimentally and theoretically the VCSEL injection dynamics from parallel optical frequency comb injection. We show that the two polarizations combperformance is restricted to high current injection in the case of parallel optical injection. For fixed bias current, the two polarization comb dynamics disappear when increasing the injected comb spacing.This thesis therefore demonstrates besides its interest for nonlinear laser dynamics, optical injection is a technique to harness the comb properties in laser diodes.
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