This dissertation presents to our knowledge the first demonstration of a quantum well (QW) laser monolithically integrated with internal optical pump based on a light emitting diode (LED). The LED with high efficiency is operated in a thermoelectrophotonic (TEP) regime for which it can absorb both its own emitted light and heat. The LED optical pump can reduce internal optical loss in the QW laser, and enables monolithically integrated TEP heat pumps to the semiconductor laser. The design, growth and fabrication processes of the laser chip are discussed, and its experimental data is presented. In order to further increase the TEP laser efficiency the development of QDs as the active region for TEP edge emitting laser (EEL) is studied. The usage of QD as TEP laser's active region is significant in terms of its low threshold current density, low internal optical loss and high reliability, which are mainly due to low transparency in QD laser. The crystal growth of self-organized QDs in molecular beam epitaxial (MBE) system and characterization of QDs are mentioned. The design, growth, processing and fabrication of a QD laser structure are detailed. The characteristics of laser devices with different cavity length are reported. QD active regions with different amount of material are grown to improve the active region performance. Theoretical calculations based on material parameters and semiconductor physics indicate that with proper design, the combination of high efficiency LED in TEP regime with a QD laser can result in the integrated laser chip power conversion efficiency exceeding unity.

This dissertation explores various aspects and potential of optical pulse generation based on active, passive, and hybrid mode-locked quantum dot semiconductor lasers with target applications such as optical interconnect and high speed signal processing. Design guidelines are developed for the single mode operation with suppressed reflection from waveguide discontinuities. The device fabrication procedure is explained, followed by characteristics of FP laser, SOA, and monolithic two-section devices. Short pulse generation from an external cavity mode-locked QD two-section diode laser is studied. High quality, sub-picosecond (960 fs), high peak power (1.2 W) pulse trains are obtained. The sign and magnitude of pulse chirp were measured for the first time. The role of the self-phase modulation and the linewidth enhancement factor in QD mode-locked lasers is addressed. The noise performance of two-section mode-locked lasers and a SOA-based ring laser was investigated. Significant reduction of the timing jitter under hybrid mode-locked operation was achieved owing to more than one order of magnitude reduction of the linewidth in QD gain media. Ultralow phase noise performance (integrated timing jitter of a few fs at a 10 GHz repetition rate) was demonstrated from an actively mode-locked unidirectional ring laser. These results show that quantum dot mode-locked lasers are strong competitors to conventional semiconductor lasers in noise performance. Finally we demonstrated an opto-electronic oscillator (OEO) and coupled opto-electronic oscillators (COEO) which have the potential for both high purity microwave and low noise optical pulse generation. The phase noise of the COEO is measured by the photonic delay line frequency discriminator method. Based on this study we discuss the prospects of the COEO as a low noise optical pulse source.

This dissertation details the work has been done on a novel resonant cavity linear interferometric modulator and a direct phase detector with channel filtering capability using injection-locked semiconductor lasers for applications in RF photonics. First, examples of optical systems whose performance can be greatly enhanced by using a linear intensity modulator are presented and existing linearized modulator designs are reviewed. The novel linear interferometric optical intensity modulator based on an injection-locked laser as an arcsine phase modulator is introduced and followed by numerical simulations of the phase and amplitude response of an injection-locked semiconductor laser. The numerical model is then extended to study the effects of the injection ratio, nonlinear cavity response, depth of phase and amplitude modulation on the spur-free dynamic range of a semiconductor resonant cavity linear modulator. Experimental results of the performance of the linear modulator implemented with a multi-mode Fabry-Perot semiconductor laser as the resonant cavity are shown and compared with the theoretical model. The modulator performance using a vertical cavity surface emitting laser as the resonant cavity is investigated as well. Very low Vπ in the order of 1 mV, multi-gigahertz bandwidth (-10 dB bandwidth of 5 GHz) and a spur-free dynamic range of 120 dB.Hz2/3 were measured directly after the modulator. The performance of the modulator in an analog link is experimentally investigated and the results show no degradation of the modulator linearity after a 1 km of SMF. The focus of the work then shifts to applications of an injection-locked semiconductor laser as a direct phase detector and channel filter. This phase detection technique does not iv require a local oscillator. Experimental results showing the detection and channel filtering capability of an injection-locked semiconductor diode laser in a three channel system are shown. The detected electrical signal has a signal-to-noise ratio better than 60 dB/Hz. In chapter 4, the phase noise added by an injection-locked vertical cavity surface emitting laser is studied using a self-heterodyne technique. The results show the dependency of the added phase noise on the injection ratio and detuning frequency. The final chapter outlines the future works on the linear interferometric intensity modulator including integration of the modulator on a semiconductor chip and the design of the modulator for input pulsed light.

<p>A detailed analysis of coupled cavity semiconductor lasers with asymmetric multiple quantum well (AMQW) active regions is presented in this thesis. The analysis involved design, fabrication, characterization, and simulation of these devices. Although the coupled cavity devices can be multi sectioned, the devices discussed in this thesis are two sectioned.</p><p> A below threshold model for an AMQW coupled cavity device is developed. Non-linear fits of the below threshold spectral data to that obtained from the model were used to extract optimized device parameters. These fits helped to create an understanding of the operation of the devices and paved the way for improved device performance. Optimized device parameters obtained from the below threshold model were later used as input parameters in the development of an above threshold model. This model verified the wavelength selection mechanism employed by coupled cavity diode lasers and predicted the longitudinal modes for sets of injection currents.</p><p> Optical coherence tomography (OCT) is an application where much interest has recently been drawn. The coupled cavity devices fabricated in this work applied with proper modulation of the injection currents and followed by subsequent time averaging have demonstrated short coherence length (-15 μm) and can be an excellent source for synthesized OCT. Rapid wavelength switching (-70 ns, the measurement was limited by detector response time) over the whole range has also been experimentally shown. Because of the high speed (relative to mechanical) wavelength switching ability, AMQW coupled cavity devices have the potential for applications requiring real time measurements including real time synthesized OCT.</p> / Thesis / Doctor of Philosophy (PhD)

In this dissertation, self-assembled InAs/InGaAs quantum dot Fabry-Perot lasers and mode-locked lasers are investigated. The mode-locked lasers investigated include monolithic and curved two-section devices, and colliding pulse mode-locked diode lasers. Ridge waveguide semiconductor lasers have been designed and fabricated by wet etching processes. Electroluminescence of the quantum dot lasers is studied. Cavity length dependent lasing via ground state and/or excited state transitions is observed from quantum dot lasers and the optical gain from both transitions is measured. Stable optical pulse trains via ground and excited state transitions are generated using a grating coupled external cavity with a curved two-section device. Large differences in the applied reverse bias voltage on the saturable absorber are observed for stable mode-locking from the excited and ground state mode-locking regimes. The optical pulses from quantum dot mode-locked lasers are investigated in terms of chirp sign and linear chirp magnitude. Upchirped pulses with large linear chirp magnitude are observed from both ground and excited states. Externally compressed pulse widths from the ground and excited states are 1.2 ps and 970 fs, respectively. Ground state optical pulses from monolithic mode-locked lasers e.g., two-section devices and colliding pulse mode-locked lasers, are also studied. Transformed limited optical pulses (~4.5 ps) are generated from a colliding pulse mode-locked semiconductor laser. The above threshold linewidth enhancement factor of quantum dot Fabry-Perot lasers is measured using the continuous wave injection locking method. A strong spectral dependence of the linewidth enhancement factor is observed around the gain peak. The measured linewidth enhancement factor is highest at the gain peak, but becomes lower 10 nm away from the gain peak. The lowest linewidth enhancement factor is observed on the anti-Stokes side. The spectral dependence of the pulse duration from quantum dot based mode-locked lasers is also observed. Shorter pulses and reduced linear chirp are observed on the anti-Stokes side and externally compressed 660 fs pulses are achieved in this spectral regime. A novel clock recovery technique using passively mode-locked quantum dot lasers is investigated. The clock signal (~4 GHz) is recovered by injecting an interband optical pulse train to the saturable absorber section. The excited state clock signal is recovered through the ground state transition and vice-versa. Asymmetry in the locking bandwidth is observed. The measured locking bandwidth is 10 times wider when the excited state clock signal is recovered from the ground state injection, as compared to recovering a ground state clock signal from excited state injection.

InAs/InP multiwavelength quantum dash lasers are promising solutions to rising data loads in our telecommunications systems, as one laser chip can replace many lasers operating at a single wavelength. Quantum dashes are quasi-one-dimensional nanoparticles that offer equal or increased performance as laser gain media when compared to equivalent quantum well devices. InAs/InP quantum dashes are ideal for laser devices emitting in the C-band region, centred around 1550 nm. The quantum dashes in this thesis are epitaxially grown via the self assembled Stranski-Krastanow mode. Characterizing how structure and composition of these quantum dashes affect the energy level spacing and emission wavelengths is crucial for designing better performing telecommunications lasers. In this thesis a method for determining the average heights and widths of these nanoparticles from atomic force microscopy measurements of uncapped InAs/InGaAsP/InP quantum dashes is developed. Single quantum dash simulations are built in Crosslight Photonic Integrated Circuit Simulator (PICS3D) with the lowest energy transition tuned to photoluminescence peak wavelengths provided by National Research Council Canada. These simulations are used to determine the impact of quantum dash dimensions, compositions, and heterostructure changes to the overlap integrals and emission energies. Phosphorus concentration within the quantum dash and wetting layer can modify the predicted emission wavelength by ∼200 nm, and increasing quantum dash lengths beyond 200 nm has negligible effect on emission energy and energy level spacing. The sublayer thickness is increased from 0.1 to 1 nm, and shows that emission energy will increase for GaP sublayers and decrease for GaAs sublayers by up to 30 meV. The role of the wetting layer on energy level spacing is discussed and determined to increase the emission energy by ∼15 meV when the 0.5 nm wetting layer is removed for a 2 nm quantum dash. The role of As/P intermixing is investigated in three ways: by incorporating phosphorus concentration in (1) the quantum dash and wetting layer, (2) the wetting layer, and (3) the lower portion of the quantum dash without a wetting layer. There is negligible change in the overlap integral for these three cases with all other variables held constant, and the trends between each case remain the same. Further experimental analysis of buried InAs quantum dashes is recommended for compositional information. The implementation of variable strain profiles in this model is also recommended, in addition to developing vertically coupled quantum dash simulations. Finally, performing these simulations at varying temperatures will better represent the operating conditions of quantum dash lasers.

No description available.

This thesis reports on an extensive investigation into the intrinsic frequency response of various MQW lasers as determined from parasitic-free relative intensity noise (RIN) measurements. Eleven structures were designed, grown and fabricated at Nortel Technology's Advanced Technology Laboratory in Ottawa. Five of the laser structures had active regions containing 10 QWs. The barrier layer composition for these structures was varied such that the emission wavelength corresponding to the barrier band-gap increased from 1.0 pm to 1.2 pm in 0.05 pm steps. The remaining six structures had a constant barrier layer emission wavelength of 1.1 pm but the number of quantum wells was varied from 5, 7, 8 to 14 in 2 well steps. In all structures the QWs were embedded in a graded- index-separate-confinement-heterostructure waveguiding region and were strained to 1.0 percent in compression. The devices processed from these structures were Fabry-Perot type lasers having cavity lengths ranging from 254 pm to 1016 pm. Resonance frequency and damping values as a function of injection current and single facet optical power, as well as optical spectra just below threshold, were obtained for over one hundred devices. From this data the response coefficient D, K factor, group velocity (vg), photon energy (hv), mirror loss (am), and internal absorption (aint) were characterized. Using these characterized parameters dg/dN, dg/ds, and the maximum theoretical intrinsic 3 dB bandwidth (fmax) were calculated. The effects of varying QW number, barrier height, and cavity length on all these parameters was investigated. Limitations with using the single mode rate equation model for these characterizations is discussed. As well, potential limitations with the basic design of the structures studied in this thesis as revealed by the results are explored. / Thesis / Candidate in Philosophy

Dans un premier temps, nous avons optimisé des structures laser VECSEL dans le but de maximiser la puissance émise par une gestion thermique adéquate. Les structures conçues et fabriquées contiennent une zone active à base d’InP pour l’émission à 1.55 µm. Un miroir hybride métal- semiconducteur à base d’un miroir de Bragg GaAs/AlAs est intégré à la zone active. La structure semiconductrice est intégrée avec différents substrats hôtes de bonne conductivité thermique sur la base de simulations numériques, et les performances des dispositifs fabriqués sont évaluées expérimentalement sous pompage optique Les VECSELs intégrés sur substrat diamant CVD présentent les puissances de sortie les plus élevées, et sont de bons candidats pour l’émission de puissance (> 500 mW) à 1.55 µm et pour les expériences de blocage de modes. D’un autre côté nous montrons que l’intégration d’un substrat de cuivre par voie électrochimique représente une approche flexible et faible-coût, pour atteindre une puissance de sortie de plusieurs dizaines de mW jusqu’à ~ 200 mW.Dans un second temps, nous avons développé des SESAMs à 1.55 µm. La région active est formée de puits quantiques InGaAsN/GaAs, couplés par effet tunnel à des plans GaAsN à recombinaison rapide. Des temps caractéristiques de recouvrement de l’absorption de quelques picosecondes à la dizaine de picoseconde sont ainsi mesurés.La résonance de la microcavité SESAM est ajustée de manière contrôlée grâce à des couches de phase spécifques épitaxiées en surface de la structure. La gravure sélective couche par couche des couches de phase permet d’accorder la profondeur de modulation et la dispersion de vitesse de groupe (GDD) de la structure SESAM.Finalement nous avons assemblé les structures SESAM et VECSEL dans une cavité à quatre miroirs pour obtenir un fonctionnement laser en régime de blocage de modes passif. Nous observons que la durée de l’impulsion de blocage de modes peut être réduite de plusieurs picosecondes (~ 10 ps), jusqu’à moins de la picoseconde (0.9 ps) en accordant la GDD de la structurre SESAM. / In a first step, we have developed and implemented VECSEL structures, aiming at maximizing the laser output power through a proper thermal management. The fabricated VECSEL chips contain an InP-based active region for emission at 1.55 µm. A hybrid metal-GaAs/AlAs Bragg mirror is used to achieve efficient dissipation of the heat generated in the active region. The semiconductor structure is integrated to various host substrates and the VECSEL performances are investigated numerically and experimentally. VECSELs with CVD diamond substrates have the best overall performance and are promising for large output power (> 500 mW), while electroplated copper substrate is demonstrated to be a flexible and cost-effective approach for thermal management in 1.55 µm OP-VECSEL in order to achieve output power of several tens of mW to ~ 200 mW. The second part of the work is devoted to the development of SESAM structures at 1.55 µm. The structures include an active region consisting of InGaAsN / GaAs quantum wells surrounding by GaAsN planes, allowing to achieve absorption relaxation time of few picoseconds. The SESAM microcavity resonance was adjusted via a selective etching of phase layers specifically designed to control the magnitude of both the modulation depth and the intra cavity group delay dispersion of the device.Finally, assembling VECSEL and SESAM chips in a cavity, we observe experimentally that the mode-locked pulse duration could be reduced from several picoseconds to less than one picosecond when the resonance and group delay dispersion of the SESAM microcavity are tuned.

L’objectif de la thèse concerne le développement de lasers à semi-conducteur à blocage de modes qui présentent un grand intérêt pour les systèmes de télécommunications optiques à très haut débit (WDM, OTDM, radio sur fibre…).Les nanostructures à base de boites quantiques (BQs) possèdent des propriétés remarquables grâce au confinement 0D des porteurs de charge. Leur utilisation dans les lasers à blocage de modes a donné lieu à des avancées importantes en terme de génération d’impulsions très courtes à haute fréquence et avec un très faible niveau de bruit.Durant la thèse, une optimisation de la croissance des structures lasers à BQs InAs sur substrat InP(113)B a été menée afin d’accroître le nombre de plans de BQs tout en assurant une forte densité pour maximiser le gain modal. Le travail a également porté sur l’utilisation de substrats InP(001) désorienté et l’obtention d’empilement de plans de BQs de faible anisotropie. Une optimisation de la technologie des lasers monomode de type « shallow-ridge » a été réalisée sur substrat conventionnel InP (001). Nous avons confirmé l’intérêt des BQs pour améliorer l’efficacité d’injection grâce à une réduction de la diffusion latérale des porteurs. Le blocage de modes a été obtenue sur des lasers à mono-section et double sections à base de BQs InAs élaborés sur InP (001) désorienté et InP(113))B, à des fréquences de répétitions allant de 20 jusqu’à 83 GHz. Les spectres RF présentent des pics de faibles largeurs (jusqu’à 20 kHz) qui indique un faible bruit de phase. Enfin, une étude a été menée sur le comportement en température des lasers à blocage de modes passif à double sections à base de BQs ou de BatQs InAs/InP. / Semiconductor mode-locked lasers (MLLs) are at the centre of interest for a large range of photonic applications (WDM, OTDM, radio over fiber ...). Because of their outstanding performance coming from the 0D carrier confinement, the use of quantum dots (QDs) nanostructures as active material for MLLs has led to the generation of ultra-short and high frequency pulses with low noise. For the present thesis studies were carried out on InAs based QDs laser growth on InP (113)B in order to increase the number of stacked QDs layers while maintaining a high density of QDs to maximize modal gain. Work has also been focused on layers stacking and obtaining real QDs using misoriented (001) InP substrate. Structural qualities have been confirmed using AFM, polarized photoluminescence and broad laser characterization. A shallow ridge waveguide optimization technology has been realized on conventional (001) InP substrate. We have confirmed the improved injection efficiency of QDs due to lower lateral carrier diffusion. Mode-locking was obtained on single and two sections InAs based QDs lasers elaborated on (001) InP misoriented substrate and (113)B InP substrate, from 20 to 83 GHz. The RF linewidth at -3 dB is as low as 20 kHz indicating a ML regime with a low phase noise. Finally, we have studied the temperature effect on the QDs and QDashes InAs/InP multi-section MLLs.