Im Rahmen dieser Arbeit werden Untersuchungen der Spinrelaxation in epitaktischen GaN-Schichten mit unterschiedlichen Donatorkonzentrationen und Versetzungsdichten mit Hilfe spin- und zeitaufgelöster differentieller Reflektanzspektroskopie präsentiert. Dabei wurden die optischen Anregungsbedingungen sehr sorgfältig gewählt. Neben der genauen Abstimmung der Anregungsenergie, unterstützt durch die Modellierung der differentiellen Reflektanz, wurden insbesondere spektral schmale Laserpulse verwendet. Diese erlauben eine selektive Anregung der untersuchten Übergänge. Es wurden Spinlebensdauern von 30 bis 170~ps bei tiefen Temperaturen für das freie A-Exziton bestimmt. In der Nähe des Metall-Isolator-Übergangs ließ sich eine langsamere Spinrelaxation als für schwächer dotierte Proben nachweisen. Die längsten beobachteten Spinrelaxationszeiten zeigen freistehende GaN-Schichten hoher Materialqualität mit sehr geringen Versetzungsdichten. In der Literatur besteht eine kategorische Unterteilung der Ergebnisse in lange elektronische Spinlebensdauern bis in den Nanosekundenbereich, erhalten mit Kerr-Messungen, und extrem kurze exzitonische Spinrelaxation in Reflektanz-Experimenten im (Sub-)Pikosenkundenbereich. Dieses Bild wird hier nicht bestätigt. Die beobachteten Spinrelaxationszeiten liegen eineinhalb bis zweieinhalb Größenordnungen über Ergebnissen, von denen bisher mit der hier verwendeten Methode berichtet wurde. Es wird gezeigt, dass die Beobachtungen extrem kurzer Spinrelaxationszeiten an anderer Stelle eine Folge der optischen Anregungsbedingungen sind. Die Verwendung sehr kurzer und damit spektral breiter Laserpulse, die eine selektive Exziton-Anregung verbieten, führt zu einem deutlich anderen zeitlichen Verhalten und stark verfälschten Ergebnissen. Diese Beobachtung löst den scheinbaren Widerspruch zwischen den beiden Ergebnisgruppen in der Literatur auf und bildet die Grundlage für weiterführende Untersuchungen. / In this work, an investigation of spin relaxation in GaN epitaxial layers with different doping concentrations and dislocation densities is presented. The measurements were carried out by the means of spin- and time-resolved differential reflectance spectroscopy. The conditions of optical excitation were chosen with special care. In particular, spectrally narrow laser pulses were used to achieve selective excitation of the examined transitions in addition to the precise adjustment of the excitation energy, supported by the modeling of the differential reflectance. The spin relaxation times obtained for the free A exciton at low temperatures are in the range of 30 to 170 ps. In the proximity of the metal insulator transition, a slower spin relaxation was observed than for lower doping concentrations. The longest spin relaxation times were found in high quality, free-standing GaN layers with very low dislocation densities. Existing results in the literature can be strictly grouped into long electronic spin lifetimes of up to a few nanoseconds, obtained with Kerr rotation, and extremely short spin relaxation in the (sub)picosecond range, measured with reflectance experiments. This picture cannot be confirmed here. The spin relaxation times observed here lie 1.5 to 2.5 orders of magnitude above the values previously reported using the same experimental method. It is shown that the instances of extremely fast spin relaxation are caused by the properties of the optical excitation. The use of ultra-short and thus spectrally broad laser pulses, which prohibits the selective excitation of excitons, leads to a significantly different temporal behavior and strongly distorted results. This finding elucidates the apparent conflict between the two groups of results and forms the basis for further investigations.

La photonique du silicium a connu un développent massif pendant les dix derniers années. Presque toutes les briques technologiques de base ont été réalisées et ont démontrées des performances remarquables. Cependant, le manque d’une source laser intégrée en silicium a conduit les chercheurs à développer de composants basés sur l’intégration entre le silicium et les matériaux III-V.Dans cette thèse je décris la conception, la fabrication et la caractérisation des lasers hybrides III-V sur silicium basés sur cette intégration. Je propose un coupleur adiabatique qui permet de transférer intégralement le mode optique du guide silicium au guide III-V. Le guide actif III-V au centre du composant fourni le gain optique et les coupleurs, des deux cotés, assurent le transfert de la lumière dans les guides silicium.Les lasers mono longueur d’onde sont des éléments fondamentaux des communications optiques. Je décris les différentes solutions permettant d’obtenir un laser mono-longueur d’onde hybride III-V sur silicium. Des lasers mono longueur d’onde ont été fabriqués et caractérisés. Ils démontrent un seuil de 21 mA, une puissance de sortie qui dépasse 10 mW et une accordabilité de 45 nm. Ces composants représentent la première démonstration d’un laser accordable hybride III-V sur silicium. / Silicon photonics knew an impressive development in the last ten years. Almost all the fundamental building blocks have been demonstrated and reveal competitive performances. However, the lack of an efficient silicon integrated laser source has led the researchers to develop heterogeneous integration of III-V materials on silicon.In this thesis I describe the design, the fabrication and the performances of these hybrid III-V on silicon lasers. I propose the use of an adiabatic coupler that totally transfers the optical mode between the III-V and the silicon waveguides. The active waveguide on III-V materials at the center of the device provides the optical gain, while, on both side, adiabatic couplers allow a loss-less transfer of the optical mode to the silicon waveguide. Single wavelength emitting lasers are fundamental elements for high bandwidth optical links. I review all the effective solutions enabling single waveguide hybrid III-V on SOI lasers. DBR, microring based, DFB and AWG laser solutions were analysed. Single wavelength operating lasers have been fabricated and characterized. A laser threshold of only 21 mA, an output power of more than 10 mW and tunability over 45 nm with a SMSR of 45 dB have been measured. These devices represent the first demonstration of a monolithically integrated hybrid III-V/Si tunable laser made by wafer bonding technique.

Single self-assembled semiconductor quantum dots (QDs) are able to emit single-photons and entangled-photons pairs. They are therefore considered as potential candidate building blocks for quantum information processing (QIP) and communication. To exploit them fully, the ability to precisely control their optical properties is needed due to several reasons. For example, the stochastic nature of their growth ends up with only little probability of finding any two or more QDs emitting indistinguishable photons. These are required for two-photon quantum interference (partial Bell-state measurement), which lies at the heart of linear optics QIP. Also, most of the as-grown QDs do not fulfil the symmetries required for generation of entangled-photon pairs. Additionally, tuning is required to establish completely new systems, for example, 87Rb atomic-vapors based hybrid semiconductoratomic (HSA) interface or QDs with significant heavy-hole (HH)-light-hole (LH) mixings. The former paves a way towards quantum memories and the latter makes the optical control of hole spins much easier required for spin- based QIP. This work focuses on the optical properties of a new type of QDs optimized for HSA experiments and their broadband tuning using strain. It was created by integrating the membranes, containing QDs, onto relaxor-ferroelectric actuators and was quantified with a spatial resolution of ~1 µm by combining measurements of the µ-photoluminescence of the regions surrounding the QDs and dedicated modeling. The emission of a neutral exciton confined in a QD usually consists of two fine-structure-split lines which are linearly polarized along orthogonal directions. In our QDs we tune the emission energies as large as ~23meV and the fine-structure-splitting by more than 90 µeV. For the first time, we demonstrate that strain is able to tune the angle between the polarization direction of these two lines up to 40° due to increased strain-induced HH-LH mixings up to ~55%. Compared to other quantum emitters, QDs can be easily integrated into optoelectronic devices, which enable, for example, the generation of non-classical light under electrical injection. A novel method to create sub-micrometer sized current-channels to efficiently feed charge carriers into single QDs is presented in this thesis. It is based on focused-laserbeam assisted thermal diffusion of manganese interstitial ions from the top GaMnAs layer into the underlying layer of resonant tunneling diode structures. The combination of the two methods investigated in this thesis may lead to new QDbased devices, where direct laser writing is employed to preselect QDs by creating localized current-channels and strain is used to fine tune their optical properties to match the demanding requirements imposed by QIP concepts.

L'objectif de ce travail porte sur la généralisation de la modélisation de la gravure du silicium dans les plasmas de fluor ou de chlore à celle de la gravure des éléments de la colonne IV et des composés III-V de structure cristalline de type diamant ou zinc-blende dans les plasmas d'halogènes, i.e. fluor, chlore, brome et iode. Dans ce contexte, les effets stériques et de diffusion en volume et/ou en surface en constituent les problématiques principales. Cette généralisation s'appuie sur le modèle de gravure de Petit et Pelletier qui, par rapport aux modèles antérieurs, prend en compte un certain nombre d'hypothèses distinctes ou additionnelles telles que les interactions répulsives entre adatomes d'halogènes proches voisins, les mécanismes de Langmuir-Hinshelwood pour la formation des produits de réaction, la nature mono-couche ou multi-couches de l'adsorption, et la diffusion des adatomes en surface. Les effets stériques relatifs à la diffusion des atomes d'halogènes à travers les surfaces (100) des structures cristallines des éléments de la colonne IV et des composés III-V définissent une première loi de similitude entre la maille du réseau cristallin et le rayon ionique de Shannon des atomes d'halogènes concernant leurs conditions de diffusion en volume. Cette loi se traduit par un diagramme prévisionnel, commun aux éléments de la colonne IV et aux composés III-V, délimitant les systèmes de gravure de types mono-couche et multi-couches. Les effets stériques relatifs aux mécanismes réactionnels de gravure sur les surfaces (100) aboutissent à des secondes lois de similitude entre la maille du réseau et le rayon covalent des adatomes d'halogènes caractérisant la nature de la gravure : gravure isotrope, gravure anisotrope, ou absence de gravure. Ces lois de similitude, distinctes pour les éléments de la colonne IV et les composés III-V (stœchiométrie différente des produits de réaction), se traduisent par deux diagrammes prévisionnels délimitant les différents domaines de gravure. Les diagrammes prévisionnels pour les éléments de la colonne IV ont pu être validés, d'une part, à partir des résultats expérimentaux antérieurs, et, d'autre part, en l'absence de données, à partir d'études expérimentales complémentaires : gravure de Si et Ge en plasma de brome et d'iode, gravure de Sn en plasma d'iode. / The objective of this work is the generalization of the modeling of the etching of silicon in fluorine or chlorine plasmas to that of the etching of the elements in column IV and of III-V compounds with diamond-like or zinc-blend crystal structure in halogen plasmas (i.e. fluorine, chlorine, bromine and iodine). In this context, steric effects and volume and/or surface diffusion are the main issues. This generalization is based on the etching model of Petit and Pelletier which, compared to previous models, takes into account a number of separate or additional assumptions such as the repulsive interactions between halogen adatoms in nearest neighbor positions, the Langmuir-Hinshelwood mechanisms for the formation of reaction products, the mono-layer or multi-layer nature of the adsorption, and the diffusion of adatoms on the surface. Steric effects related to the diffusion of halogens through the (100) surfaces of the crystal structures of the elements of column IV and III-V compounds define a first law of similarity between the crystal lattice and the Shannon ionic radius of the halogen atoms concerning their bulk diffusion conditions. This law results in a forecast diagram, common to column IV elements and III-V compounds, delimiting the mono-layer or multi-layer type of the etching systems. Steric effects related to the reaction mechanisms of etching on (100) surfaces lead to the second laws of similarity between the crystal lattice and the covalent radius of halogen adatoms characterizing the etching behavior: isotropic etching, anisotropic etching or no etching. These laws of similarity, distinct between the elements of the column IV and III-V compounds (different stoichiometry of the reaction products), result in two forecast diagrams delimiting the distinct etching domains. Forecast diagrams for column IV elements have been validated, first, from previous experimental results, and, secondly, in the absence of data, from additional experimental studies: etching of Si and Ge in bromine and iodine plasmas, and etching of Sn in iodine plasmas.

La diversification des fonctionnalités intégrées dans les systèmes micro-optoélectroniques est l'un point clé du développement de ces filières. Combiner sur une même puce des matériaux ayant des propriétés différentes doit permettre de faire émerger de nouveaux concepts de composants basés sur de nouveaux effets physiques ou sur la combinaison des propriétés physiques des matériaux intégrés. Parmi les matériaux d'intérêt, les semi-conducteurs III-V présentent des propriétés optiques exceptionnelles et sont couramment utilisés pour réaliser des composants photoniques. Les oxydes fonctionnels, quant à eux, offrent une grande variété de propriétés physiques qui en font des matériaux très prometteurs pour de nombreuses applications. Dans ce contexte, l'objectif global de cette thèse est de démontrer la possibilité d'intégrer des oxydes fonctionnels cristallins sur des hétérostructures à base de GaAs par épitaxie, et de montrer que de telles structures peuvent présenter des propriétés nouvelles pour la photonique. Plus précisément, nous avons focalisé nos efforts sur l'intégration de couches minces de PZT sur des structures à puits quantiques InGaAs/GaAs via des couches tampons de SrTiO3 (STO). Nous avons étudié et développé la croissance par épitaxie par jets moléculaires (MBE) des templates de STO sur GaAs. La forte hétérogénéité entre ces deux types de matériaux nécessite d'avoir recours à des stratégies d'ingénierie d'interface spécifiques et à un excellent contrôle des paramètres de croissance. Nous avons mis en évidence les effets bénéfiques sur la qualité structurale du STO d'une préparation de la surface de GaAs au Ti. Pour ces études, nous avons utilisé la spectroscopie de photoélectrons (XPS, in-situ ou en collaboration avec la ligne TEMPO du synchrotron SOLEIL) et microscopie électronique en transmission (TEM, en collaboration avec le LPN). Ces expériences nous ont permis de sonder structure et chimie de l'interface semi-conducteur/oxyde. Nous avons également étudié les mécanismes de croissance et de cristallisation du STO sur GaAs, en mettant notamment en œuvre des expériences d'XPS in-situ au synchrotron SOLEIL. La compréhension de ces mécanismes spécifiques nous a permis d'adapter les conditions de croissance du STO et d'obtenir des couches tampons d'excellente qualité. Nous avons étudié la croissance de couches minces de PZT sur des structures à puits quantique d'In- GaAs/GaAs via des templates de STO. Nous avons tout d'abord montré que les procédés standards de croissance de PZT (sol-gel ou ablation laser (collaboration avec l'IEF)) conduisaient à de fortes dégradations des puits quantiques du fait des réactions chimiques entre l'oxyde et le matériau III-V. Nous avons étudié les mécanismes de ces dégradations et mis en évidence une forte affinité chimique entre l'As, le Pb et le Sr. Pour pallier cette difficulté, nous avons modifié le procédé de croissance du PZT ainsi que l'hétérostructure III-V (enfouissement du puits, ajout d'AlAs ...). Ces actions combinées nous ont permis de réaliser des couches minces de PZT ferroélectriques sur des structures à puits quantiques d'InGaAs/GaAs. Nous avons ensuite défini un design d'émetteur accordable basé sur une hétérostructure PZT/GaAs/InGaAs. De tels émetteurs ont été réalisés en collaboration avec l'IEF) et mesurés leurs propriétés mécaniques et optiques en effectuant des expériences sous champ. Enfin, nous avons effectué un certain nombre d'études préliminaires visant à démontrer la possibilité d'intégrer des hétérostructures à base de GaAs sur des substrats de Si recouverts de couches tampons de STO. Nous avons pour cela envisagé et étudié la possibilité d'utiliser des composés Zintl-Klemm d'interface susceptibles de minimiser l'énergie d'interface entre le GaAs et le STO. / Diversification of the materials and functionalities integrated on silicon is an important issue for further progression in the field of micro-optoelectronics. The monolithic heterogeneous integration of new materials on silicon, and more generally the combination on the same wafer of materials having different physical properties is a key challenge. Amongst the materials of interest, III-V semiconductors are the object of specific attention because their optoelectronic and transport properties are superior to those of silicon. Similarly, the so-called functional oxides have interesting physical properties (ferroelectricity, ferromagnetism, piezoelectricity, etc.) making them suitable for various applications (NVM, energy harvesters, MEMS . . . ). In this context, the goal of this thesis is to demonstrate the possible integration of crystalline functional oxides on GaAs-based heterostructures using epitaxy and that such structures show new properties for photonic. More precisely, we focused on integration PZT thin film on InGaAs/GaAs quantum wells structures thanks to SrTiO3 (STO) buffer layer. We first studied and developed the growth of STO on GaAs templates using molecular beam epitaxy (MBE). Because of the strong heterogeneity between the two materials, specific interface engineering strategies are required. We highlight the benefit of a Ti-based GaAs surface treatment on the structural quality of STO. For these studies we used photoelectrons spectroscopy (XPS, in-situ and collaboration with TEMPO beam line of SOLEIL synchrotron) and transmission electron spectroscopy (TEM, collaboration with LPN/C2N). Those experiments allowed us to probe both structural and chemical aspects of the semiconductor/ oxide interface. We also studied the growth mechanism of STO on GaAs through in-situ XPS experiments at SOLEIL. Thanks to the understanding of those specifics mechanisms, we could accommodate the growth conditions to obtain good quality STO buffer layers. Then we studied the growth of thin film PZT on InGaAs/GaAs quantum well structures by means of STO templates. We first showed that standard growth process (sol-gel and pulsed laser deposition at IEF/C2N) lead to strong deterioration of quantum well due to chemical reactions between the oxide and the III-V material. We studied the mechanisms involved in this deterioration and highlight the strong chemical affinity between As, Pb and Sr. To palliate this difficulty, the growth process of PZT has been modify and an AlAs “sacrificial” layers has been added in order to limit the oxygen difiusion into the substrate. Thanks to these two solutions, it has been possible to realize a PZT ferroelectric thin film on an InGaAs/GaAs quantum well heterostructure. A tunable source based on such heterostructure has been designed. In this device, the strain induced in the ferroelectric PZT by an electric field is transmitted to the substrate and the quantum well modifying its emitted wavelength. We simulated this device in order to optimize its dimensions. Then we realized this device (collaboration with IEF/C2N) and measured its mechanical and optical properties under an electric field. We also performed preliminary studies in order to demonstrate the possible integration of GaAs-based heterostructures on Si substrates in by the means of STO buffer layer. We considered the use of Zintl- Klemm compounds to minimize the interface energy between GaAs and STO allowing 2D growth of the semiconductor on the oxide.

Les matériaux semi-conducteurs III-N sont à l’origine d’une véritable révolution technologique. Mais malgré l’effervescence autour de ces sources lumineuses, leurs performances dans le vert et l’UV demeurent limitées. La principale raison à cela est l’orientation cristalline (0001)III-N (dite polaire) selon laquelle ces matériaux sont généralement épitaxiés et qui induit de forts effets de polarisation. Ces effets peuvent cependant être fortement atténués par l’utilisation d’orientations de croissance dite semi-polaires. Malheureusement, les films de GaN semi-polaires hétéroépitaxiés présentent des densités de défauts très importantes, ce qui freine très fortement leur utilisation. L’enjeu de cette thèse de doctorat est de réaliser des films de GaN semi-polaire (11-22) de haute qualité cristalline sur un substrat de saphir en utilisant la technique d’épitaxie en phase vapeur aux organométalliques. La réduction de la densité de défaut étant l’objectif majeur, différentes méthodes d’ingénieries de défauts s’appuyant sur la structuration de la surface des substrats et sur la croissance sélective du GaN ont été développées. Elles ont permis d’établir l’état de l’art actuel du GaN semi-polaire hétéroépitaxié. Par la suite, dans le but d’améliorer les performances des DELs vertes, une étude dédiée à l’optimisation de leur zone active a été menée. D’autre part, le développement de substrats autosupportés de GaN semi-polaires, ainsi que la confection de cristaux 3D de grande taille dont la qualité cristalline est comparable aux cristaux de GaN massifs ont été démontrés. Ces deux approches permettant de s’approcher encore plus de la situation idéale que serait l’homoépitaxie. / Nitride based materials are the source of disruptive technologies. Despite the technological turmoil generated by these light sources, their efficiency for green or UV emission is still limited. For these applications, the main issue to address is related to strong polarization effects due to the (0001)III-N crystal growth orientation (polar orientation). Nevertheless these effects can be drastically decreased using semipolar growth orientations. Unfortunately semipolar heteroepitaxial films contain very high defect densities which hamper their adoption for the time being. The aim of this doctoral thesis is to achieve semipolar (11-22) GaN of high quality on sapphire substrate by metalorganic chemical vapor deposition. Defect reduction being the main objective, several defect engineering methods based on sapphire substrate patterning and GaN selective area growth have been developed. Thanks to refined engineering processes, the remaining defect densities have been reduced to a level that establishes the current state of the art in semipolar heteroepitaxial GaN. These results have enabled the achievement of high quality 2 inches semipolar GaN templates, thus forming an ideal platform for the growth of the forthcoming semipolar optoelectronic devices. With this in mind, to improve green LEDs, a study dedicated to the optimization of their active region has been conducted. Finally, the development of semipolar freestanding substrate has been performed, and beyond, the realization of large size crystals with a structural quality similar to that of bulk GaN has been demonstrated. These last two approaches pave the way to quasi-homoepitaxial growth of semipolar structures.

Cette thèse de doctorat traite de la mise en œuvre du procédé de soulèvement épitaxial (ou ELO pour epitaxial lift-off) à partir d'un substrat d'InP permettant le détachement des couches actives et le recyclage du substrat afin de rendre économiquement compétitive la fabrication de cellules solaires multi-jonctions pour le photovoltaïque concentré. Ce procédé, qui consiste à sous-graver sélectivement une couche sacrificielle comprise entre le substrat et les couches actives, est bien connu et maîtrisé sur un substrat de GaAs avec l'utilisation d'une couche sacrificielle d'AlAs d'épaisseur voisine de 5 nm, ce qui n'est pas possible sur un substrat d'InP en raison du fort désaccord de maille cristalline existant entre l'AlAs et l'InP. Pour l'adapter à un substrat d'InP, le développement d'une couche sacrificielle spécifique basée sur un super-réseau AlAs/InAlAs a été réalisé, ce qui permet de contourner les problématiques liées au désaccord de maille et à la croissance de matériaux contraints. Après optimisation des conditions de croissance de ce super-réseau, les épaisseurs atteintes et donc les vitesses de sous-gravure obtenues en utilisant ce type de couche sacrificielle ont satisfait aux exigences du procédé ELO. Ensuite, le report et le soulèvement de structures actives de cellules solaires InGaAs en couches minces cristallines ont été développés. Les cellules solaires ainsi fabriquées ont montré des performances semblables à celles réalisées par épitaxie standard sur un substrat d'InP, voire meilleures sous concentration en raison d'effets de confinement optique. Finalement, le recyclage du substrat d'InP réalisé avec un procédé utilisant seulement deux étapes de nettoyage par voies chimiques humides, a permis de produire des surfaces d'InP de qualité suffisante pour réaliser une reprise d'épitaxie satisfaisante. / This PhD thesis deals with the implementation of the epitaxial lift-off (ELO) process from an InP substrate allowing the detachment of active layers and the substrate recycling. The final target is to realize multi-junction solar cells in an economically competitive way for concentrated photovoltaic. The ELO process consists in the under-etching of a sacrificial layer inserted between the substrate and the active layers. It is well known and mastered on a GaAs substrate with the use of a sacrificial layer of AlAs with a thickness of about 5 nm. Such a layer is not usable on an InP substrate due to the high lattice mismatch between AlAs and InP. In order to adapt the ELO process to an InP substrate, this work aimed to develop a specific sacrificial layer based on an AlAs/InAlAs superlattice. Thus, it is possible to circumvent problems related to the lattice mismatch and to the strained layer growth. After optimization of growth conditions of this superlattice, using this type of sacrificial layer, we achieve a sufficient thickness and therefore a sufficient under-etching rate in order to meet the requirements of the ELO process. Then, the transfer and lift-off of thin crystalline film based InGaAs solar cells have been developed. This kind of solar cells showed performances similar to those obtained with a standard epitaxial growth on an InP substrate, or even better under concentration due to optical confinement effects. Finally, the recycling of the InP substrate carried out by a process using only two wet chemical cleaning steps made it possible to produce InP surfaces of sufficient quality to achieve a promising second epitaxial growth.

The deterministic generation and manipulation of quantum states has attracted much interest ever since the rise of quantum mechanics. Large-scale, distributed quantum states are the basis for novel applications such as quantum communication, quantum remote sensing, distributed quantum computing or quantum voting protocols. The necessary infrastructure will be provided by distributed quantum networks, allowing for quantum bit processing and storage at single nodes. Quantum states of light then allow for inter-node transmission of quantum information. Transmission losses in optical fibers may be overcome by quantum repeaters, the quantum equivalent of classical signal amplifiers. The fragility of quantum superposition states makes building such networks very challenging. Hybrid solutions combine the strengths of different physical systems: Efficient quantum memories can be realized using alkali atoms such as rubidium. Leading in the deterministic generation of single photons and polarization entangled photon pairs are semiconductor InAs/GaAs quantum dots grown by the Stranski-Krastanov method. Despite remarkable progress in the last twenty years, complex quantum optical protocols could not be realized due to low degree of entanglement, low brightness and broad wavelength distribution. In this work, an emerging family of epitaxially grown GaAs/AlGaAs quantum dots obtained by droplet etching and nanohole infilling is studied. Under pulsed resonant two-photon excitation, they emit single pairs of entangled photons with high purity and unprecedented degree of entanglement. Entanglement fidelities up to f = 0.94 are observed, which are only limited by the optical setup or a residual exciton fine structure. The samples exhibit a very narrow wavelength distribution at rubidium memory transitions. Strain tuning is applied via piezoelectric actuators to allow for reversible fine-tuning of the emission frequency. In a next step, active feedback is employed to stabilize the frequency of single photons emitted by two separate quantum dots to an atomic rubidium standard. The transmission of a rubidium-based Faraday filter serves as the error signal for frequency stabilization. A residual frequency deviation of < 30MHz is achieved, which is less than 1.5% of the quantum dot linewidth. Long-term stability is demonstrated by Hong-Ou-Mandel interference between photons from the two quantum dots. Their internal dephasing limits the expected visibility to V = 40%. For frequency-stabilized dots, V = (41 ± 5)% is observed as opposed to V = (31 ± 7)% for free-running emission. This technique reaches the maximally expected visibility for the given system and therefore facilitates quantum networks with indistinguishable photons from distributed sources. Based on the presented techniques and improved emission quality, pivotal quantum communication protocols can now be implemented with quantum dots, such as transferring entanglement between photon pairs. Embedding quantum dots in a dielectric antenna ensures a bright emission. For the first time, entanglement swapping between two pairs of photons emitted by a single quantum dot is realized. A joint Bell measurement heralds the successful generation of the Bell state Ψ+ with a fidelity of up to (0.81 ± 0.04). The state's nonlocal nature is confirmed by violating the CHSH-Bell inequality with S = (2.28 ± 0.13). The photon source is tuned into resonance with rubidium transitions, facilitating implementation of hybrid quantum repeaters. This work thus represents a major step forward for the application of semiconductor based entangled photon sources in real-world scenarios.

Single self-assembled semiconductor quantum dots (QDs) are able to emit single-photons and entangled-photons pairs. They are therefore considered as potential candidate building blocks for quantum information processing (QIP) and communication. To exploit them fully, the ability to precisely control their optical properties is needed due to several reasons. For example, the stochastic nature of their growth ends up with only little probability of finding any two or more QDs emitting indistinguishable photons. These are required for two-photon quantum interference (partial Bell-state measurement), which lies at the heart of linear optics QIP. Also, most of the as-grown QDs do not fulfil the symmetries required for generation of entangled-photon pairs. Additionally, tuning is required to establish completely new systems, for example, 87Rb atomic-vapors based hybrid semiconductoratomic (HSA) interface or QDs with significant heavy-hole (HH)-light-hole (LH) mixings. The former paves a way towards quantum memories and the latter makes the optical control of hole spins much easier required for spin- based QIP. This work focuses on the optical properties of a new type of QDs optimized for HSA experiments and their broadband tuning using strain. It was created by integrating the membranes, containing QDs, onto relaxor-ferroelectric actuators and was quantified with a spatial resolution of ~1 µm by combining measurements of the µ-photoluminescence of the regions surrounding the QDs and dedicated modeling. The emission of a neutral exciton confined in a QD usually consists of two fine-structure-split lines which are linearly polarized along orthogonal directions. In our QDs we tune the emission energies as large as ~23meV and the fine-structure-splitting by more than 90 µeV. For the first time, we demonstrate that strain is able to tune the angle between the polarization direction of these two lines up to 40° due to increased strain-induced HH-LH mixings up to ~55%. Compared to other quantum emitters, QDs can be easily integrated into optoelectronic devices, which enable, for example, the generation of non-classical light under electrical injection. A novel method to create sub-micrometer sized current-channels to efficiently feed charge carriers into single QDs is presented in this thesis. It is based on focused-laserbeam assisted thermal diffusion of manganese interstitial ions from the top GaMnAs layer into the underlying layer of resonant tunneling diode structures. The combination of the two methods investigated in this thesis may lead to new QDbased devices, where direct laser writing is employed to preselect QDs by creating localized current-channels and strain is used to fine tune their optical properties to match the demanding requirements imposed by QIP concepts.

The incorporation of Gallium Nitride (GaN) Power Amplifiers (PAs) into future high power aperture radar systems is certain; however, the introduction of this technology into multifunction radar systems will present new challenges to radar engineers. This dissertation describes a broad investigation into amplitude and phase transients produced by GaN PAs when they are excited with multifunction radar waveforms. These transients are the result of self-heating electrothermal memory effects and are manifested as interpulse instabilities that can negatively impact the coherent processing of multiple pulses. A behavioral model based on a Foster network topology has been developed to replicate the measured amplitude and phase transients accurately. This model has been used to develop a digital predistortion technique that successfully mitigates the impact of the transients. The Moving Target Indicator (MTI) Improvement Factor and the Root Mean Square (RMS) Pulse-to-Pulse Stability are used as metrics to assess the impact of the transients on radar system performance and to test the effectiveness of a novel digital predistortion concept. / Ph. D. / The incorporation of Gallium Nitride (GaN) Power Amplifiers (PAs) into future radar systems is certain, and will present new challenges to radar engineers. This dissertation describes a broad investigation into signal transients produced by GaN PAs when they are excited with a wide variety of RF pulsed waveforms. These waveforms are representative of those used by a radar system to conduct multiple functions or missions. The transients are primarily the result of changes in the GaN PA gain due to self-heating, and are manifested as differences in consecutive pulses. These pulse-to-pulse differences negatively affect the ability of a radar system to extract information from a received echo. A behavioral model based on a Foster network topology has been developed to replicate the measured signal transients accurately. This model has been used to develop a digital predistortion technique that successfully counteracts the transients mitigating the impact of the transients. The Moving Target Indicator (MTI) Improvement Factor and the Root Mean Square (RMS) Pulse-to-Pulse Stability are used as performance metrics to quantify the effect of the transients on radar system performance and to test the effectiveness of a novel digital predistortion concept.