Thulium based fiber lasers represent a promising alternative for pulse energy scaling and high peak power generation with ytterbium based systems at 1µm. Advantages of thulium arise from the operation at longer wavelengths and a large gain bandwidth (1.8-2.1µm). Nonlinear effects, such as self phase modulation, stimulated Raman scattering and stimulated Brillouin scattering generally limit peak power scaling in fiber lasers. The longer wavelength of thulium fiber lasers and large mode field areas can significantly increase the nonlinear thresholds. Compared to 1µm systems, thulium fiber lasers enable single mode guidance for two times larger mode field diameter in step index fibers. Similar behavior is expected for index guiding thulium doped photonic crystal fibers. In this work a novel thulium doped rod type photonic crystal fiber design with large mode field diameter ( > 50µm) was first characterized in CW-lasing configuration and then utilized as final amplifier in a two stage master oscillator power amplifier. The system generated MW-level peak power at 6.5ns pulse duration and 1kHz repetition rate. This world record performance exemplifies the potential of thulium fiber lasers to supersede ytterbium based systems for very high peak power generation in the future. As part of this work a computer model for the transient simulation of pulsed amplification in thulium based fiber lasers was developed. The simulations are in good agreement with the experimental results. The computer model can be used for efficient optimization of future thulium based fiber amplifier designs.

The thulium fiber laser has gained interest due to its long emission wavelength, large bandwidth (~1.8 – 2.1 µm), high efficiencies (~60 %), and high output power levels both in cw as well as pulsed regimes. Applications like remote sensing, machining, medical tissue ablation, and mid-infrared generation benefit from high peak power thulium laser sources. Pulsed thulium fiber laser systems are advancing rapidly towards higher peak power levels and are becoming the preferred sources for these applications. This dissertation work describes the development of novel nanosecond pulsed thulium fiber laser systems with record high peak power levels targeting mid-infrared generation. The peak power scaling in thulium fiber lasers requires new fiber designs with larger mode field area (MFA) than commercially available step index large mode area (SI-LMA) fibers. Two different prototypes of thulium doped photonic crystal fibers (PCF) were investigated for high peak power generation. The first prototype is a flexible-PCF with MFA twice as large as SILMA fiber and the second prototype is a PCF-rod with six times larger MFA. A robust single stage master oscillator power amplifier (MOPA) source based on flexible-PCF was developed. This source provided narrow linewidth, tunable wavelength, variable pulse duration, high peak power, and high energy nanosecond pulses. The PCF-rod was implemented as a second stage power amplifier. This system generated a record level of ~1 MW peak power output with 6.4 ns pulse-duration at 1 kHz repetition rate. This thulium doped PCF based MOPA system is a state of the art laser source providing high quality nanosecond pulses. iv The single stage MOPA system was successfully implemented to pump a zinc germanium phosphide (ZGP) crystal in an optical parametric oscillator (OPO) cavity to generate 3 - 5 µm wavelengths. The MOPA source was also used to demonstrate backside machining in silicon wafer. The PCF based laser system demonstrated an order of magnitude increase in the peak power achievable in nanosecond thulium doped fiber laser systems, and further scaling appears possible. The increase in peak power will enable additional capabilities for mid-infrared generation and associated applications.

Over a wide range of applications, optical systems have utilized conventional optics in order to provide the ability to engineer the properties of incident infra-red fields in terms of the transmitted field spectral, spatial, amplitude, phase, and polarization characteristics. These micro/nano-optical elements that provide specific optical functionality can be categorized into subcategories of refractive, diffractive, multi-layer thin film dichroics, 3-D photonic crystals, and polarization gratings. The feasibility of fabrication, functionality, and level of integration which these elements can be used in an optical system differentiate which elements are more compatible with certain systems than others. With enabling technologies emerging allowing for a wider range of options when it comes to lithographic nano/micro-patterning, dielectric growth, and transfer etching capabilities, optical elements that combine functionalities of conventional optical elements can be realized. Within this one class of optical elements, it is possible to design and fabricate components capable of tailoring the spectral, spatial, amplitude, phase, and polarization characteristics of desired fields at different locations within an optical system. Optical transmission filters, polarization converting elements, and spectrally selective reflecting components have been investigated over the course of this dissertation and have been coined  MOSSE,' which is an acronym for micro-optic-spectral-spatial-elements. Each component is developed and fabricated on a wafer scale where the thin film deposition, lithographic exposure, and transfer etching stages are decoupled from each other and performed in a sequential format. This facilitates the ability to spatially vary the optical characteristics of the different MOSSE structures across the surface of the wafer itself.

Ultrafast lasers are valuable research and manufacturing tools. The ultrashort pulse duration is comparable to electron-lattice relaxation times, yielding unique interactions with matter, particularly nonlinear absorption, melting, and ablation. The field of ultrafast laser manufacturing is rapidly evolving with advances in related laser technologies. The applications of ultrashort pulse lasers in additive manufacturing aim to fill gaps left by conventional techniques especially on the nano- and micro-scale. Concurrently, uptake of ultrafast fiber lasers for micromachining has increased, and may replace the Ti:Sapphire laser as the ultrafast laser of choice. Both additive and subtractive manufacturing are accomplished with ultrafast lasers which presents the possibility of hybrid, all-in-one devices using a single laser source. As one such combination of laser techniques, ultrashort pulse surface modification of additively manufactured metals is an area of limited investigation. This thesis aims to address the ever-changing landscape of ultrafast laser manufacturing by 1) reviewing ultrafast laser additive manufacturing techniques and recent advancements 2) comparing the design, operation, and micromachining potential of a commercial ultrafast Ti:Sapphire and ultrafast fiber laser, and 3) investigating femtosecond ablation of as-printed additively manufactured Ti-6Al-4V at a range of parameters to test the feasibility of surface feature control. Ultrafast laser additive manufacturing is still in its infancy with mostly niche applications. The ultrafast fiber laser architecture is found to deliver a platform that is easier to operate and maintain and has superior micromachining throughput relative to Ti:Sapphire lasers. In our experimental work, five main surface morphologies are obtained by femtosecond ablation of a rough Ti-6Al-4V surface: laser-induced periodic surface structures (LIPSS), undulating grooves, micro-ripples, grooves, and micro-cavities. Transitions between ablation regimes and evolutions of the surface under increasing pulse energy and number of pulses are observed. These patterns allow for control over the surface geometry without the need for post-printing polishing. / Thesis / Master of Applied Science (MASc) / Ultrafast pulsed lasers of <10 picoseconds pulse duration are commonly used to modify, melt, or ablate materials. As an important research and manufacturing tool, ultrafast lasers and techniques have seen great change in the past two decades. Additive manufacturing has emerged as an area in which ultrafast lasers are becoming increasingly prevalent. To make sense of this continuously evolving landscape, this thesis 1) reviews ultrafast laser additive manufacturing techniques, applications, and advances towards industrial use and commercialisation, 2) compares the setup, operability, and characteristics for two ultrafast laser designs, and 3) investigates the surfaces produced by ultrafast laser irradiation of an additively manufactured titanium alloy part. The surface morphologies that are produced are categorised into five main patterns: laser-induced periodic surface structures, undulating grooves, micro-ripples, grooves, and micro-cavities. Each is a distinct pattern that may allow for tuning of the surface properties with respect to the wettability and biocompatibility.

High-power fiber lasers have emerged as a cornerstone in the realm of laser technology. Characterized by their exceptional efficiency, ruggedness, and versatility, fiber lasers are experiencing widespread use in manufacturing, medical, defense, science, and in long range sensing. Unfortunately, high-power applications require strict spatial and spectral performance characteristics to be maintained, which has yet to be perfected. This dissertation discusses the power scaling of ytterbium-doped fiber laser amplifiers, presenting three significant advancements. First, a novel photonic lantern-based method is introduced for real-time monitoring of laser beam modal content and beam quality. Initial tests highlight the photonic lantern's efficiency in predicting the onset of modal instability while simultaneously measuring the laser's output beam quality, M2. Second, this work achieved 2.2 kW single-mode narrow-linewidth laser delivery through a 5-tube nested antiresonant hollow core fiber, maintaining over 95% transmission efficiency and near diffraction-limited beam quality. Lastly, this research explores active-gain fiber designs to mitigate nonlinear effects for further power scaling. One design employing confined-doping strategies, achieving a 2.4x increase in the maximum output power before the onset of stimulated Brillouin scattering. Additionally, a second experiment employing a bend-insensitive fiber design demonstrated a transverse modal instability threshold nearly 3x that of its step-index counterpart. Collectively, this work presents a novel approach to power scale, deliver, and monitor multi-kW Yb-doped fiber laser amplifiers enabling the next-generation of applications requiring the strictest spatial and spectral performance.

Alors que la science attoseconde connaît un développement fulgurant, le besoin de nouvelles sources laser adaptées à la génération d'impulsions attosecondes uniques est apparu. Grâce à ses propriétés d'accordabilité en fréquence et d'amplification de spectres ultra-larges à même de supporter des durées d'impulsions ultracourtes, conjuguées à la possibilité de stabiliser passivement la phase sous l'enveloppe (CEP) du champ électrique associé à l'impulsion laser, l'amplification paramétrique (OPA) s'est imposée comme un des outils incontournables pour la réalisation de telles sources.De plus, un intérêt croissant se manifeste pour la montée en cadence des sources d'harmoniques d'ordre élevé (HHG), en tirant parti des avancées des laser à fibre. Récemment fut démontrée la génération d'impulsions ultracourtes à très haute cadence, stabilisées en phase, dans la partie visible du spectre. Décaler la bande d'amplification vers l'infrarouge présenterait des avantages certains du point de vue de la génération d'harmoniques. En effet, travailler avec une source laser infrarouge permet d'étendre le spectre d'harmoniques et donc de réduire la durée des impulsions attosecondes générées. Jusqu'à présent, l'amplification paramétrique large bande dans l'infrarouge à haute cadence était rendue impossible par la difficulté à générer un signal à ces longueurs d'onde directement à partir d'un laser à fibre.Les travaux exposés ici décrivent la réalisation de nouvelles sources paramétriques, spécifiquement conçues en fonction des exigences de la génération d'impulsions attosecondes uniques, aussi bien en régime de forte énergie qu'à des cadences élevées.Nous présentons tout d'abord le développement d'un OPA avec stabilisation passive de la CEP, capable d'amplifier un spectre d'une largeur de 700 nm centré à 1,75 µm et délivrant une énergie de 450 µJ à la cadence de 10 Hz. Puis, nous détaillons une architecture originale d'amplification paramétrique à haute cadence pompé par un laser à fibre, qui nous a permis de générer des impulsions stabilisées en phase d'une durée inférieure à trois cycles optiques à la longueur d'onde centrale de 2,2 µm, avec une énergie de 5 µJ à la cadence de 100 kHz.Enfin, nous explorons la possibilité d'accroître la puissance de sortie des OPA infrarouges large bande à des niveaux de plusieurs dizaines de watts, grâce à la technique de combinaison paramétrique de plusieurs faisceaux de pompe fibrés. / While attosecond science reaches new frontiers in physics, the need for innovative primary sources suited for the generation of single attosecond (as) pulses emerges. Featuring high tunability, ultra-broadband amplification bandwidth and the ability of passively stabilizing the random Carrier-Envelope Phase (CEP) of any pump laser, Optical Parametric Amplification (OPA) has proven to be one of the most effective tools to meet the stringent requirements of High-Order Harmonics (HHG) driving sources.Moreover, there is a growing interest for higher repetition rate HHG sources, pumped by Ytterbium-doped fiber lasers. High-repetition rate, CEP-stable, few cycle pulses have been successfully generated by OPAs operating in the visible part of the spectrum. Shifting the amplified bandwidth towards longer wavelengths would be clearly profitable. In fact, the shorter harmonic wavelength cut-off will allow significantly extending the harmonics spectrum and consequently shorten as pulse durations. Until know, generation of CEP-stable, few-cycle pulses in the infrared at ultra-high repetition rates was impossible due to the issue of generating a broadband infrared seed directly from a fiber laser. This thesis describes the implementation of new supercontinuum-seeded parametric sources, specifically designed for isolated attosecond pulses generation with high energy or high repetition rate.The development of a CEP-stable three-stages OPA source is reported, amplifying a 700 nm broad spectrum at a central wavelength of 1,75 µm with an energy of 450 µJ at a 10 Hz repetition rate. Then, a new architecture based on a two-stage cascaded OPA pumped by a home-made fiber laser is presented, which allowed us to generate CEP-stable 3-cycles pulses at the central wavelength of 2,2 µm, with an energy of 5 µJ at 100 kHz. Finally, we discuss the possibility of increasing the output power of parametric amplifiers to several tens of watts with broadband parametric combination of several fiber-pump beams.

[pt] Neste trabalho, desenvolvemos um laser a fibra, monomodo e de cavidades acopladas, cujo meio de ganho é uma Fibra Dopada com Érbio. As duas cavidades, C1 e C2, foram feitas no mesmo pedaço de fibra dopada, com a mesma concentração de Érbio (Er) e mesmo índice de refração. A Fibra Dopada com Érbio usada era também dopada com Germânio (Ge), que aumenta a fotossensitividade da fibra. Portanto, foi possível escrever Redes de Bragg na mesma fibra para serem usadas como os espelhos da cavidade. A configuração do laser consiste em três Redes de Bragg, escritas no mesmo núcleo da fibra, centradas em 1532nm e separadas por 30cm. As reflectividades das Redes de Bragg eram de 95 por cento, 80 por cento e 60 por cento. Com essa configuração simples de cavidades acopladas, conseguimos uma emissão laser estável e monomodo. Será apresentado também um estudo teórico para descrever o sistema. / [en] In this work, we developed a single mode coupled cavity fiber laser, in which the gain medium is an Erbium Doped Fiber. The two cavities, C1 and C2, were made in the same piece of the doped fiber, with the same concentration of Erbium (Er) and the same refraction index. The Erbium Doped Fiber used was codoped with Germanium (Ge), which increases the photosensitivity of the fiber. Therefore, it was possible to write bragg Gratings in the same fiber to be used as the cavity mirrors. The laser configuration consists of three Bragg Gratings, written in the core of the fiber, centered in 1532 nm and separated by 30cm. Ther Bragg Grating reflectivities were 95 per cent, 80 per cent and 60 per cent. With this simple configuration of coupled cavities, a stable, single mode laser emission was achieved. A theoretical study to describe the system will also be presented.

Les travaux de recherche, rapportés dans ce manuscrit, portent sur l’étude d’un laser à fibre en forme de huit et le développement de sources à 1.6 µm. En premier temps, nous avons étudié la dynamique impulsionnelle d’un laser à fibre micro-structurée en forme de huit. L’objectif est de montrer l’impact des propriétés de la fibre micro-structurée sur le comportement impulsionnel du laser. Nous avons également étudié le phénomène d’hystérésis dans cette cavité. Nos résultats numériques ont permis de démontrer l’universalité de ce phénomène dans les cavités lasers. Autrement, il est indépendant de la technique de verrouillage de modes. En second lieu, nous avons développé une source laser émettant à 1.6 µm à partir d’un amplificateur fonctionnant dans la bande C. La méthode que nous avons explorée est basée sur la gestion des pertes linéaires. L’émission, en continu et en verrouillage de modes, a été démontrée dans deux configurations différentes. Enfin et en se basant sur ce concept, nous avons rapporté des sources accordables sur une large fenêtre spectrale. Nous avons également étudié différentes formes des régimes harmoniques autour de 1.6 µm. / During our research, we are interested in studying of the figure of eight fiber laser based on the microstructured optical fiber and developing a 1.61 µm mode locked fiber laser from a C-band double-clad Er : Yb doped fiber amplifier. In the first step and based on a theoretical model, we have investigated the multi-pulse emission of a microstructured figure-of eight fiber laser operating in passive mode-locking. The proposed laser is mode locked by the nonlinear amplifying loop mirror (NALM). We further study the hysteresis dependence and the number of pulses in steady state as a function of both the small signal gain and the nonlinear coefficient of microstructured fiber. Our results demonstrate that the nonlinear coefficient of microstructured fiber plays a key role in the formation of multi-soliton. In the second step and based on the control of the linear losses of the cavity, we demonstrate the possibility to achieve filter less laser emission above 1.6 μm, from a C-band double-clad Er: Yb doped fiber amplifier, using a figure-of-eight geometry and a unidirectional ring cavity. We also reported a widely tunable mode locked fiber laser and harmonic mode locking of twin and third pulse around 1.61 µm.

Materiais compósitos são projetados e fabricados para várias aplicações de alto desempenho, incluindo componentes para os segmentos automobilístico, aeroespacial, aeronáutico, naval, de defesa, de óleo e gás, energia eólica e até equipamentos esportivos. Porém, a união por soldagem de Compósitos de Matriz Metálica de Alumínio (Al-CMM) ainda é um grande obstáculo para a maior disseminação desta classe de materiais estruturais. As mudanças microestruturais decorrentes do ciclo de soldagem e/ou do tratamento térmico afetam sensivelmente as propriedades mecânicas e físico-químicas finais da junta e do metal base nas proximidades de mesma, daí a importância de se estudar a evolução microestrutural que prospera nestas etapas. O presente trabalho caracterizou a microestrutura do compósito liga-A356/SiCp soldado por laser de fibra de Itérbio, empregando-se nessa tarefa técnicas de microscopia óptica, radiografia e microscopia eletrônica de varredura, assim como difração de raios-X e de elétrons retroespalhados, ensaio instrumentado de dureza e microtomografia computadorizada. O foco das análises realizadas restringiu-se à geometria dos cordões de solda, à expulsão de SiC particulado da zona soldada, à volatilização de elementos químicos da poça de soldagem, à formação de precipitados fragilizantes de Al4SiC4 em formato de agulhas no cordão de solda e à determinação das regiões com concentração de poros, todos estes fenômenos tendo efeitos nocivos, em maior ou menor extensão, no desempenho global da junta do Al-CMM soldada a laser, notadamente em suas propriedades mecânicas e eletroquímicas. / Microstructural materials composites are designed and manufactured for various high performance applications, including components for different industries like automobile, aerospace, aeronautical, naval, defense, oil and gas, wind energy and even sports equipment. However, the junction by welding of Aluminum Metal Matrix Composite (Al-MMC) is still a major obstacle to the further spread of this class of structural materials. The microstructural changes resulting from the welding cycle and / or post-weld heat treatment significantly affect the final mechanical and physicochemical properties of the joint and the base metal near it, hence the importance of studying the microstructural evolution that thrives in these steps. This study aims to characterize the microstructure of the composite alloy-A356 / SiCp welding by Ytterbium fiber laser, using optical microscopy, X-ray, scanning electron microscopy, X-ray diffraction, electron backscatter diffraction, instrumented test hardness and computed microtomography. The focus of the analyzes was restricted to the geometry of the weld bead, the particulate SiC expulsion of the welded zone, volatilization of chemical elements from the welding zone, formation of precipitates embrittlement of Al4SiC4 in needle shape in the weld bead and determining the concentration of regions with pores, all these phenomena have harmful effects to a greater or lesser extent, the overall performance of the joining Al-CMM laser welded, mainly in their mechanical and electrochemical properties.

La fusion sélective par laser est un procédé de la technologie de fabrication rapide de plus en plus utilisé dans l’industrie automobile, aéronautique, médicale, etc. Selon le principe de la fabrication rapide, la pièce est fabriquée couche par couche en fusionnant et soudant les particules fines par laser. Actuellement, les principaux matériaux utilisés sont les métaux métalliques ou les polymères. Le faible ou modeste point de fusion de ces matériaux conduit à une mise en œuvre par laser relativement facile. Cependant, en raison de leur point de fusion élevé, de la forte résistance à haute température et de la faible conductivité thermique, l’utilisation de matériaux céramiques est limitée dans la technologie de fusion laser sélective. Cette étude explore la fusion laser sélective de zircone stabilisée par yttrine avec un laser à fibre de longueur d’onde d’environ 1 µm. L’influence de différentes puissances de laser et de différentes vitesses de balayage sur la microstructure et la déformation de l’échantillon a été étudiée, et la densité relative et la microdureté ont été mesurées. Notamment, l’effet de différentes températures de préchauffage sur la microstructure sera étudié. En même temps, la structure cristalline céramique et la transformation des phases pendant le procédé de prototypage rapide ont été analysées. Les résultats expérimentaux montrent qu’il est possible de fondre complètement de la poudre YSZ avec un laser à fibre NIR, et avec l’optimisation des paramètres de fabrication, la densité relative de l’échantillon peut atteindre 91 %. Il est inévitable de voir se former des fissures et des pores dans les pièces fabriquées du fait de l’hétérogénéité de la distribution de l’énergie du laser. Cette distribution de l’énergie peut être améliorée grâce à l’optimisation des paramètres ; les longueurs de fissure peuvent être contrôlées et maîtrisées par un préchauffage du lit de poudre. Notamment, à haute température (1500°C, 2000°C et 2500°C) de préchauffage, la fissure verticale continue devient désordonnée et courte. Une transformation de la structure monoclinique et cubique en structure tétragonale s’est produite pendant le processus de fabrication. / Selective laser melting is a rapid manufacturing process coming from the rapid prototyping technology, which is widely used in the automotive, aeronautical, medical industry etc. According to the principle of rapid manufacturing, the piece is manufactured layer by layer through the laser sintering or melting the fine powder. Currently, the main powder materials used are metal or polymer materials. The low melting point of these materials facilitates the melting process. However, duo to the high melting point, strong strength at high temperature and low thermal conductivity the application of ceramic materials is limited in the technology of selective laser melting. In this study, selective laser melting of the ceramic yttria stabilized zirconia by a 1μm wavelength fiber laser was explored. The influence of different laser powers and different scanning velocities on the microstructure and the deformation were analyzed, then the micro-hardness and relative density were measured. In particular, the effect of different preheat temperatures on microstructure was investigated. At the same time, the crystal structure and phase transformation during the fabrication were analyzed. Experimental results show that YSZ powder can be completely melted by the near IR fiber laser. With the optimization of the manufacturing parameters, the relative density of sample could reach 91 %. The forming of cracks and pores in the manufactured parts is rarely avoid due to the heterogeneity of distribution of energy. The energy distribution could be improved by optimizing the parameters and the crack lengths can be controlled by preheating the powder bed. In particular, the high temperature (1500 ℃, 2000 ℃ and 2500 ℃) lead the continuous vertical crack becomes messy and short. The transformation of monoclinic and cubic crystal to tetragonal crystal can be observed during the fabrication.