QC 351 A7 no. 69 / The history of modern wide -field, high-speed catadioptric lenses is reviewed. One system comprising only spherical curves and representative of the current art for low-light-level systems is evaluated and used as a baseline design in a weight-reduction study. Five aspheric designs are computed and evaluated. It is found that the use of aspherics will permit weight reduction only in certain instances, i.e., if one element of an all-spherical design can be eliminated or if a fundamentally different configuration that is possible only with aspherics is substituted for the all-spherical configuration. Of these possibilities, the elimination of an element is the best replacement for the baseline design. The case of a highly constrained, purely refractive triplet is studied in some detail. Four designs are computed -from the all-spherical case to the most complex polynomial aspheric. It is found that, if only conic aspherics are employed, significant improvement can be obtained and the problems involved are sensibly the same as those in all-spherical designs. When complex aspherics are applied, the problem becomes surprisingly difficult, and there is some indication that a computer can deal with it better than can a human lens designer.

I have conducted detailed experimental and theoretical studies of the nonlinear optical properties of semiconductor materials useful for optical limiting. I have constructed optical limiters utilizing two-photon absorption along with photogenerated carrier defocusing as well as the bound electronic nonlinearity using the semiconducting material ZnSe. I have optimized the focusing geometry to achieve a large dynamic range while maintaining a low limiting energy for the device. The ZnSe monolithic optical limiter has achieved a limiting energy as low as 13 nJ (corresponding to 300W peak power) and a dynamic range as large as 105 at 532 nm using psec pulses. Theoretical analysis showed that the ZnSe device has a broad-band response covering the wavelength range from 550 nm to 800 nm. Moreover, I found that existing theoretical models (e.g. the Auston model and the band-resonant model using Boltzmann statistics) adequately describe the photo-generated carriers refractive nonlinearity in ZnSe. Material nonlinear optical parameters, such as the two-photon absorption coefficient β_2=5.5cm/GW, the refraction per unit carrier density σ_n=-0.8∗10^-21cm^3 and the bound electronic refraction n_2=-4∗10^-11esu, have been measured via time-integrated beam distortion experiments in the near field. A numerical code has been written to simulate the beam distortion in order to extract the previously mentioned material parameters. In addition, I have performed time-resolved distortion measurements that provide an intuitive picture of the carrier generation process via two-photon absorption. I also characterized the optical nonlinearities in a ZnSe Fabry-Perot thin film structure (an interference filter). I concluded that the nonlinear absorption alone in the thin film is insufficient to build an effective optical limiter, as it did not show a net change in refraction using psec pulses. An innovative numerical program was developed to simulate the nonlinear beam propagation inside the Fabry-Perot structure. For comparison, pump-probe experiments were performed using both thin film and bulk ZnSe. The results showed relatively long carrier lifetimes (>300 psec) in both samples. A numerical code was written to fit the pump-probe experimental results. The fitting yielded that carrier lifetimes (recombination through traps), radiative decay rate, two-photon absorption coefficient as well as the free carrier absorption coefficient for ZnSe bulk material.

We have conducted a detailed experimental and theoretical study of nonlinear absorption in semiconductors. Experimental measurements were made on a variety of materials at wavelengths of 1.06 and 0.53 microns using a picosecond Nd:YAG laser. Both two- and three-photon processes were investigated. Values of nonlinear absorption coefficients extracted from these measurements show excellent agreement with recent theory and scaling rules. Our theoretical investigation has been carried out for two-, three-,and n-photon absorption, for both continuous and pulsed sources. Expressions are obtained for the transmission of the sample in terms of the incident irradiance for each case. The physical interpretation of these results is discussed. We have also considered the effects of the photogenerated carriers on the measurements. Equations are developed that include linear absorption by these carriers. We have observed severe distortions on the transmitted beam, caused by changes in the refractive index of the material, due to the presence of these carriers. We present a model that accurately describes these effects in terms of the photogenerated carrier density. We have developed several novel techniques for monitoring nonlinear absorption. In particular, we have adapted the photoacoustic technique to the measurement of nonlinear absorption in semiconductors. We have also developed a technique employing irradiance modulation to greatly enhance the sensitivity to nonlinear processes and simultaneously discriminate against linear background signals. A related technique has been used to observe coherent mixing effects in semiconductors with cw, modelocked dye lasers.

The nonlinear refractive index (n2) of room temperature liquid CS2 in the wavelength range of 9 to 11 micrometers is measured. A line tunable hybrid C02 TEA laser and amplifier system is used for the experiments. In these measurements the well known photoacoustic method is utilized to observe the onset of whole beam self-focusing. The photoacoustic signal in a CS2 cell, much longer than the confocal parameter, is monitored. The departure of the acoustic signal from linear growth marks the critical power for the onset of nonlinearity. It is experimentally verified that the phenomenon is power dependent as expected from self-focusing theory. The value of n2 is then calculated from the theoretical model of self focusing. Measurements of the on-axis irradiance transmitted through the nonlinear material as well as the measurements of beam distortion are used to verify the validity of the photoacoustic method. In all the measurements the on-axis intensity was smaller than the calculated threshold intensity for stimulated Brillouin scattering. The back reflection was monitored to make sure that stimulated Brillouin scattering was not playing a role in the phenomenon.

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Cette étude s'inscrit dans le cadre du développement de nouveaux matériaux pour la fabrication additive. Notre objectif est la fabrication de pièces comprenant un alliage métallique complexe (CMA) à l'aide d'un laser UV de stéréolithographie. L'alliage choisi est un alliage quasicristallin dominé par une phase icosaédrique du système AlCuFeB. Des poudres brutes d'atomisations ont été caractérisées par diffractions des rayons X et analyse thermique différentielle. Nous avons montré une bonne absorbance optique de la poudre dans le domaine UV-visible qui rend possible un début de frittage sous l'effet du laser correspondant à la formation de pontages entre les grains à une température d'environ 820°C. Concernant la fabrication à partir d'une suspension de poudres dans un liant, nous avons étudié les propriétés de mouillage des particules AlCuFeB et optimisé un mélange avec une résine époxy chargée par 20 % vol. de particules CMA. L'absorption optique de la suspension dans le domaine UV est suffisante pour fabriquer une pièce composite par stéréolithographie. La granulométrie utilisée est inférieure à 25 µm. Nous avons ainsi réussi à fabriquer des pièces de 14 mm de hauteur, en additionnant des couches de 50 µm. À partir des pièces réalisées, nous avons caractérisé la dureté et les propriétés tribologiques de ce nouveau matériau composite. La dureté des pièces ainsi fabriquées est supérieure à celle de la résine seule et atteint 88 Shore D. Nous avons également mis en évidence une amélioration de 30 % du coefficient de frottement et une diminution du volume d'usure de 40 % par rapport au matériau de la matrice époxy. Ces propriétés rendent attractif ce nouveau matériau composite pour la fabrication par stéréolithographie / This study aimed at developing new materials for additive manufacturing. We focused on producing parts containing complex metallic alloys (CMA) using a UV laser used for stereolithography. The selected intermetallic is a quasicrystalline alloy dominated by the icosahedral phase in the system AlCuFeB. The raw powders produced by gas atomization were characterized by X-ray diffraction and differential thermal analysis. The powders exhibit good optical absorption properties in the UV-visible range allowing direct laser sintering as evidenced by the formation of bridges between the grains at a temperature of about 820°C. In a second step, we have considered the manufacturing of parts made of a suspension of CMA powders in a binder. We have studied the wetting properties of the particles AlCuFeB and optimized a mixture consisting of an epoxy resin filled with 20 % vol. of CMA particles. The optical absorption of the suspension in the UV range was sufficient to produce composite parts by stereolithography. The particle size used was smaller than 25 micrometers. We have managed to make parts reaching 14 mm in height by adding layers with a thickness of 50 microns. Using test samples, we have characterized the hardness and the tribological properties of this new composite material. The hardness of the parts produced by stereolithography is larger than that of epoxy parts and reaches 88 Shore D. We have also shown a 30 % reduction of the friction coefficient as well as a 40 % reduction of wear losses compared to the epoxy matrix. These properties make attractive this new composite material for stereolithography applications

Cette thèse comporte trois parties principales : la première concerne la synthèse et la fonctionnalisation des nanoparticules (NPs) d’or de forme sphérique et cylindrique. Les NPs d’or sont obtenues par réduction d’un sel métallique. En faisant varier certains paramètres de synthèse tels que la concentration en sels et/ou la concentration en réducteur, on peut facilement ajuster la taille de NPs sphériques. Bien qu’il existe diverses méthodes permettant de préparer des NPs cylindriques, il subsiste un problème de reproductibilité basée sur la pureté des produits de synthèse. Les différentes analyses de CTAB nous ont permis de proposer des solutions à ce problème. La fonctionnalisation de la surface des NPs d’or permet d’apporter à ces dernières de nouvelles propriétés tout en conservant leurs propriétés intrinsèques. Le but de cette fonctionnalisation est de modifier la surface des NPs en fonction des applications visées. Nous présentons ainsi différentes études de fonctionnalisation par des polyélectrolytes (PEI et PSS), des couches oxydes de SiO2, et de TiO2 et par le TDBC. La réponse optique des NPs d’or étant sensible à l’indice de réfraction du milieu environnant, il est possible de suivre et de quantifier cette fonctionnalisation par spectroscopie d’absorption. Dans une seconde partie, nous avons développé une voie de synthèse simple permettant de préparer le cœur coquille Au@TDBC sans ajout supplémentaire de sels ou de bases et à température ambiante. Etant donné qu’il est possible de moduler la taille des particules, l’optimisation du couplage fort entre les transitions électroniques du TDBC et les modes plasmon de résonances des Nps d’Au a été obtenu correspondant à une énergie de Rabi de 220 meV valeur qui n’a pas encore été obtenue avec un tel système. Dans une troisième partie, nous avons développé une nouvelle approche basée sur la méthode de Stöber pour fonctionnaliser les NPs avec des couches d’oxyde de SiO2 et de TiO2. L’utilisation des systèmes Au@TiO2 est une perspective intéressante en photocatalyse car le contact entre le métal et le semi-conducteur devrait entrainer une nette augmentation de l’efficacité photocatalytique. En effet, le métal agit comme un réservoir de photoélectrons améliorant le transfert de charges interfaciales tout en retardant la recombinaison des paires électrons-trous photo excités du semi-conducteur. / This thesis has three main parts: the first part relates to the synthesis and the functionalization of spherical gold nanoparticles (NPs) and nanorods. Gold NPs are obtained by chemical reduction of gold salt. By varying some synthesis parameters such as gold salt concentration and or reducing agent concentration, we can easily adjust the size of gold NPs. Different methods can be used to prepare gold nanorods, but there is a problem of reproducibility. This problem is based on the purity of products used to prepare gold nanorods. Different analysis of CTAB allowed us to propose solutions to this problem. Functionalization brings to gold NPs new properties. The aim of the functionalization is to modify the surface of gold NPs based on the intended applications. We present various functionalization of Au NPs by polyelectrolytes (PEI and PSS), oxides (SiO2 and TiO2) and TDBC. The optical response of Au NPs is sensitive to the refractive indexe of the surrounding medium, it is then possible to monitor and quantify this functionalization by absorption spectroscopy. In the second part of this work, we have developed a simple synthetic route for preparing Au@TDBC core shell without additional salts or bases at room temperature. Since it is possible to vary the particle size, optimization of the strong coupling between the electronic transitions of TDBC and the resonance plasmon of Au Nps obtained correspond to Rabi energy of 220 meV value which has not yet been achieved with such a system. In the third part, we have developed a new approach based on the Stöber method to functionalize the NPs with an oxide layer of SiO2 and TiO2. The use of Au@TiO2 core shell system is an interesting perspective in photocatalysis because the contact between metal and semiconductor should cause a marked increase in the photocatalytic efficiency. Indeed, the metal acts as a reservoir of photoelectrons improving the interfacial charge transfer while retarding the recombination of electron-hole pair of the semiconductor.

M.Ing. / This work comprises the implementation and comparison of five design techniques for the design of gradient-index thin film optical filters: classical rugate, inverse Fourier transform, a wavelet-based design procedure, as well as the flip-flop and the genetic optimization techniques. Designs for a high-reflectance filter, a beamsplitter, a discrete level filter, a distributed filter, and an anti-reflection coating were used to compare the various filter synthesis techniques. The optical thickness of the various examples was maintained below 30 and the refractive index excursion limits were between 1.5 and 3.2. The overall performance of a specific design was evaluated by a weighted merit function. The classical rugate filter uses a sinusoidal refractive index modulation that produces a single reflection band. More complex filters are realized by linear superposition of these elementary profiles. Sidelobe and ripple suppression are obtained by applying quintic windowing functions to the refractive index profile and adding matching layers at the edges of the filter. This filter design procedure has the best figure of merit of 3.73 for the discrete level filter, and the second best of 3.09 for the high-reflectance filter. The inverse Fourier transform links the refractive index profile and reflection spectrum of an optical filter by an approximate relation. It is self-correcting and iterative in nature. It produces filters with the highest optical density. The procedure excels in the design of the distributed filter with a figure of merit of 4.17. Mortlett's wavelet is used as the basis of the wavelet design technique. A single wavelet yields a single reflection band, similar to the classical rugate filter. Sidelobe suppression is an inherent property of the method, but matching layers are needed for passband ripple suppression. The optical density of the high reflection filter is larger for a filter designed with this method than for the equivalent classical rugate filter. The figure of merit of 1.75 for the high-reflectance filter is the best for any of the designs. Flip-flop refinement is a brute force approach to filter design. The layers of a starting design are flipped between two values of refractive index, the change in figure of merit evaluated and the best case saved. This process is repeated for a fixed number of iterations. It is computationally intensive and lacks ripple suppression characteristics. The flip-flop method does not compare well with any of the other techniques. It yields filters with the worst figures of merit for most of the design examples. However, it was applied successfully to the anti-reflection coating. The peak ripple for the anti-reflection filter in the 400 nm to 1100 nm wavelength band is 9.62 % compared to the inverse Fourier transform's 57.30 %. The genetic algorithm operates on the principle of "survival of the fittest". It is a stochastic procedure and yields quasi-random refractive index profiles. It excels with the antireflection coating. The peak ripple in the passband of the anti-reflection coating is 3.29%. The figure of merit for the anti-reflection coating designed with the genetic algorithm is 2.09.

Today’s electronic society relies on the functionality of electrical contacts. To achieve good contact properties, surface coatings are normally applied. Such coatings should ideally fulfill a combination of different properties, like high electrical conductivity, high corrosion resistance, high wear resistance and low cost. A common coating strategy is to use noble metals since these do not form insulating surface oxides. However, such coatings are expensive, have poor wear resistance and they are often applied by electroplating, which poses environmental and human health hazards. In this thesis, nanocomposite carbide-based coatings were studied and the aim was to evaluate if they could exhibit properties that were suitable for electrical contacts. Coatings in the Cr-C, Cr-C-Ag and Nb-C systems were deposited by magnetron sputtering using research-based equipment as well as industrial-based equipment designed for high-volume production. To achieve the aim, the microstructure and composition of the coatings were characterized, whereas mechanical, tribological, electrical, electrochemical and optical properties were evaluated. A method to optically measure the amount of carbon was developed. In the Cr-C system, a variety of deposition conditions were explored and amorphous carbide/amorphous carbon (a-C) nanocomposite coatings could be obtained at substrate temperatures up to 500 °C. The amount of a-C was highly dependent on the total carbon content. By co-sputtering with Ag, coatings comprising an amorphous carbide/carbon matrix, with embedded Ag nanoclusters, were obtained. Large numbers of Ag nanoparticles were also found on the surfaces. In the Nb-C system, nanocrystalline carbide/a-C coatings could be deposited. It was found that the nanocomposite coatings formed very thin passive films, consisting of both oxide and a-C. The Cr-C coatings exhibited low hardness and low-friction properties. In electrochemical experiments, the Cr-C coatings exhibited high oxidation resistance. For the Cr-C-Ag coatings, the Ag nanoparticles oxidized at much lower potentials than bulk Ag. Overall, electrical contact resistances for optimized samples were close to noble metal references at low contact load. Thus, the studied coatings were found to have properties that make them suitable for electrical contact applications.

Aim: To validate a method for the synthesis of a ZTA composite (Al2O3-80%/ Zr2O- 20%) and to characterize the experimental materials topography, optical, and mechanical properties in the as-sintered condition and after a simulated low temperature degradation (LTD) aging protocol compared to a translucent Y-TZP (ZPEX). Material and methods: Experimental ZTA (ZTA ZPEX 80/20) and translucent Y-TZP (ZPEX) green-state disc-shaped specimens were obtained by uniaxial/isostatic ceramic powder pressing technique. Discs were sintered according to a preestablished protocol. After sintering, two-sided polishing was performed with diamond discs and diamond suspensions to 1 m. Thirty specimens of each group underwent an aging protocol in autoclave (20h, 134ºC and 2.2 bar). The specimens were subjected to the following characterization tests, in the as-sintered condition and aged: 1) nanoindentation testing to acquire the materials elastic modulus (E) and hardness (H); 2) interferometry was utilized to characterize topographical parameters (Sa/Sq); 3) X-ray Diffraction (XRD) to assess the tetragonal-monoclinic phase transformation; 4) scanning electron microscopy (SEM) to evaluate the homogeneity of surfaces and distribution of grains; 5) reflectance tests on white and black background to determine the Contrast Ratio (CR) and the Translucency Parameter (TP) by color difference (E) and 6) biaxial flexural strength testing according to ISO 6872:2015. Apparent density was measured using Archimedes principle. Weibull 2-p was used to calculate characteristic stress, Weibull modulus, and probability of survival (reliability) at 300, 500 and 800 MPa. Data were statistically evaluated through Repeated Measures ANOVA following post-hoc comparisons by Tukey test (p<0.05). Results and Conclusion: The proposed method was able to successfully synthetize an aging resistant ZTA ZPEX 80/20 composite, with the elastic modulus being the only decreased property after aging. For such composite, the surface roughness parameters, hardness, optical and mechanical properties were not affected by simulated LTD aging. In contrast, the translucent Y-TZP zirconia presented a significant extent of tetragonal to monoclinic phase transformation compared to ZTA composite after aging, along with significant alterations in all evaluated parameters, except for surface roughness. / Objetivos: Validar um método para a síntese de um compósito ZTA (Al2O3-80%/ Zr2O- 20%) e caracterizar a topografia do material experimental e suas propriedades ópticas e mecânicas, antes e após um protocolo de envelhecimento simulando uma degradação em baixa temperatura (DBT), comparado a uma zircônia Y-TZP translúcida (ZPEX). Material e métodos: Os espécimes experimentais ZTA (ZTA ZPEX 80/20) e Y-TZP translúcido (ZPEX) em forma de disco foram obtidos por técnica de prensagem uniaxial / isostática do pó cerâmico. Os discos foram sinterizados de acordo com um protocolo pré-estabelecido. Após a sinterização, um polimento bilateral foi realizado com discos de diamante e suspensões de diamante de até 1 m. Trinta espécimes de cada grupo foram submetidos a um protocolo de envelhecimento em autoclave (20h, 134ºC e 2,2 bar). Os espécimes foram submetidos aos seguintes testes de caracterização, antes e após envelhecimento: 1) ensaios de nanoindentação para obtenção do módulo de elasticidade dos materiais (E) e dureza (H); 2) a interferometria foi utilizada para caracterizar os parâmetros topográficos (Sa / Sq); 3) difração de raios X (XRD) para avaliar a transformação da fase monoclínica para tetragonal; 4) microscopia eletrônica de varredura (MEV) para avaliar a homogeneidade da superfícies e distribuição dos grãos; 5) testes de refletância em fundo branco e preto para determinar a Relação de Contraste (RC) e o Parâmetro de Translucidez (PT) por diferença de cor (E) e 6) teste de flexão biaxial (TFB), de acordo com a ISO 6872: 2015 . A densidade aparente foi medida usando o princípio de Arquimedes. Weibull 2- p foi utilizada para calcular a resistência característica, módulo de Weibull e a probabilidade de sobrevida (confiabilidade) a 300, 500 e 800 MPa. Os dados foram submetidos à análise de variância medidas repetidas, seguida de comparações múltiplas pelo teste de Tukey (p <0,05). Resultados e Conclusão: O método proposto foi capaz de sintetizar com sucesso um compósito ZTA ZPEX 80/20 resistente ao envelhecimento, sendo o módulo de elasticidade a única propriedade que diminuiu após o envelhecimento. Para tal compósito, os parâmetros de rugosidade superficial, propriedade nanomecânica de dureza, propriedades ópticas e mecânicas não foram afetadas pelo envelhecimento simulado de DBT. Em contraste, a zircônia translúcida Y-TZP apresentou uma extensão significativa da transformação da fase tetragonal para monoclínica em comparação ao composto ZTA após o envelhecimento, juntamente com alterações significativas em todos os parâmetros avaliados, exceto a rugosidade superficial.