A esterificação do sec-butanol com ácido acético, submetida à catálise homogênea, apresenta poucos resultados experimentais de cinética reacional e equilíbrio químico disponíveis na literatura. A presente dissertação visa determinar os parâmetros cinéticos e de equilíbrio químico desta reação de esterificação, empregando modelo cinético de 2ª ordem baseado em atividades. Os experimentos cinéticos foram realizados em reator batelada com auxílio da metodologia Karl Fischer para análise do teor de água e determinação do perfil de frações molares ao longo da reação. A principal dificuldade na modelagem desta esterificação consistiu em representar satisfatoriamente as não-idealidades da mistura em fase líquida, em espacial nas reações cuja fração molar inicial de ácido acético foi superior a 50%. Netas condições admitiu-se a ocorrência de dissociação do ácido acético levando ao surgimento de interações iônicas. O modelo empregado para obtenção das atividades, com base em frações molares, foi o NRTL. Este modelo representou bem as interações moleculares em condição de baixa acidez, mas apresentou desvios em condições de acidez e teores de água mais elevados. O estudo também visou o desenvolvimento de modelos de calibração para um método analítico on-line visando determinar o perfil de frações molares ao longo da reação. O método empregado foi a espectroscopia de infravermelho próximo (NIR), em vista à capacidade deste método analítico em determinar quantitativamente frações molares de água, além dos demais compostos envolvidos. Outro fator determinante ao emprego do NIR é a seu crescente uso no meio industrial, e o presente trabalho visou também contribuir para o uso futuro desta técnica de monitoramento no processo industrial. Modelos de calibração multivariável com conjuntos de calibração interna por validação cruzada se mostraram adequados ao sistema estudado. Calibrações externas resultaram em modelos imprecisos, não sendo possível determinar claramente os fatores responsáveis pela imprecisão. / There is a lack of literature data on the reaction kinetics and equilibrium of the homogeneously catalyzed esterification of sec-butanol with acetic acid. This work aims at obtaining the kinetic parameters and chemical equilibrium parameters of this esterification reaction by using a second order kinetic model based on activities. The kinetic experiments were performed in a batch reactor and the Karl Fischer analytical method was used to determine the molar fraction of water along the reaction progress. The main challenge of modeling this reaction was to represent the highly non-ideal mixture in liquid phase, specially for reactions runs starting with acetic acid mole fraction higher than 50%. In these conditions, it was assumed the occurrence of acetic acid dissociation that leads to ionic interactions. The thermodynamic model used to calculate the activities was the NRTL. This model predicted well the molecular interactions on low acidity conditions but presented deviations when molar fractions of acid and water were higher. The present study also aims to develop calibration models for analytical on-line method to obtain molar fraction profiles along the reaction. Near infrared spectroscopy (NIR) was used due to the possibility of quantitatively analyze water mole fraction, besides the mole fractions of the other components. Another important reason to choose NIR was its crescent use in industry, and the present work intended to contribute towards the future use of this on line monitoring technique in industrial applications. Multivariate calibration models using internal set of calibration and cross-validation seems to be suitable for this system. External set of calibration leads to less accurate models, and the causes of this lack of accuracy were not clearly identified.

A lamotrigina (LTG) é um fármaco pertencente à classe das feniltriazinas utilizado no tratamento de crises epilépticas generalizadas e focais e no tratamento adjunto da epilepsia refratária. Devido à alta variabilidade interindividual, às interações medicamentosas e aos efeitos adversos apresentados durante a administração da LTG, a monitorização terapêutica nos pacientes que fazem uso deste fármaco é necessária para ajuste de dose individual e evitar os efeitos adversos. Assim, o objetivo deste trabalho foi a avaliação de duas técnicas de microextração: a microextração em fase líquida com fibras ocas (HF-LPME) e a microextração líquido-líquido dispersiva (DLLME) para análise da lamotrigina em amostras de plasma de pacientes epilépticos. Primeiramente foram definidas as condições eletroforéticas: foi utilizado um capilar de sílica fundida de 75 ?m de diâmetro interno e 50 cm de comprimento efetivo. O eletrólito de corrida (BGE) foi composto por ácido 2-morfolinoetanosulfônico (MES), na concentração de 130 mmol L-1 e pH 5,0. As análises foram realizadas à temperatura de 20°C e tensão de 15 kV. A amostra foi injetada hidrodinamicamente (0,5 psi por 10 s) e a detecção foi feita em 214 nm. Nestas condições a LTG e o padrão interno (PI), lidocaína, puderam ser analisados em menos de 7 minutos. A HF-LPME foi avaliada no modo de 3 fases, usando 500 ?L de plasma e 3,5 mL de solução fosfato de sódio 50 mmol L-1 pH 9,0 como fase doadora. O solvente utilizado para impregnar a fibra foi o 1-octanol. Como fase aceptora foram utilizados 60 ?L de solução de ácido clorídrico pH 4,0. Para avaliação da DLLME, foi necessária uma etapa de pré-tratamento da amostra (500 ?L de plasma) com 1 mL de acetonitrila. Após isto, 1,3 mL do sobrenadante foram adicionados a 4 mL de solução fosfato de sódio 50 mmol L-1 pH 9,0 e 120 ?L de clorofórmio (solvente extrator) foram injetados nesta amostra aquosa e 165 ?L de fase sedimentada foram recuperados. As características de desempenho analítico para ambos os métodos foram avaliadas, sendo obtida linearidade na faixa de concentração plasmática de 1-20 ?g/mL e limite inferior de quantificação (LIQ) de 1 ?g mL-1. Os ensaios de precisão e exatidão apresentaram valores de acordo com os guias oficiais. Além disso, os métodos foram seletivos, não apresentaram efeito residual e as amostras foram estáveis. Os valores de recuperação foram de 54,3 e 23% para HF-LPME e DLLME, respectivamente. Os métodos validados foram aplicados com sucesso em amostras de plasma de pacientes epilépticos em tratamento com a LTG. Além disso, as duas técnicas foram comparadas e a HF-LPME apresentou vantagens em relação à DLLME, mostrando ser uma técnica promissora para análise de matrizes complexas, com reduzido consumo de solvente orgânico e possibilidade de automação. / Lamotrigine (LTG) is an antiepileptic drug, which belongs to the class of phenyltriazine that can be used in the treatment of new-onset and refractory epilepsy. Due to its high interindividual variability, drug interactions and the adverse effects presented during the LTG administration, therapeutic drug monitoring is very important to dose adjustment and to avoid toxicity effects. Thus, the goal of this study was to develop and validate two microextraction techniques: the hollow fiber liquid-phase microextraction (HF-LPME) and the dispersive liquid-liquid microextraction (DLLME) to analyze LTG in plasma samples of epileptic patients. First of all, the eletroforetic conditions were optimized. A fused-silica uncoated capillary with 75 ?m internal diameter, and 50 cm effective length was used. The 2-(N-morpholino)ethanesulfonic acid (MES) 130 mmol L-1 pH 5.0 was chosen as background electrolyte (BGE). The temperature and the voltage were kept constant at 20°C and 15 kV respectively. For sample injection, hydrodynamic injection mode was used, with a pressure of 0.5 psi applied for 10 s. The wavelength was set at 214 nm. Under final conditions, LTG and the internal standard (IS) lidocaine were analyzed in less than 7 minutes. HF-LPME was evaluated in the three phase mode. The analyte was extracted from 4.0 mL of a basic donor phase (composed of 500 ?L of plasma and 3.5 mL of sodium phosphate solution 50 mmol L-1 pH 9.0) into an organic phase composed of 1-octanol immobilized in the pores of the hollow fiber, and further into an acidic acceptor phase (hydrochloric acid solution pH 4.0) placed in the lumen of the fiber. To evaluate DLLME, the plasma samples were pretreated to remove the proteins, and 500 ?L of plasma sample was mixed with 1 mL of acetonitrile. After that, 1,3 mL of the upper layer was added to 4 mL of sodium phosphate solution 50 mmol L-1 pH 9.0, and 120 ?L of chloroform (extracting solvent) was rapidly injected in the aqueous sample and 165 ?L of the sedimented phase was collected. Under the optimized conditions, both methods were linear over the plasmatic concentration range of 1.0-20.0 ?g mL-1 and the lower limit of quantification (LLOQ) was 1.0 ?g mL-1. Both methods showed good precision, accuracy, selectivity to LTG, with no carryover and the samples were stable under the studied conditions. The recovery were 54,3 and 23% to HF-LPME and DLLME respectively. The validated methods were successfully applied for the quantification of LTG in plasma samples of epileptic patients. The techniques were compared and HF-LPME was more advantageous for being more suitable to analysis of complex matrices using small amount of organic solvent, and also can be automated.

Os antidepressivos pertencem a uma importante classe de medicamentos investigados na toxicologia forense. Em casos de amostras provenientes de cadáveres, o intervalo entre o óbito e a obtenção da espécie biológica pode proporcionar a redistribuição postmortem destes fármacos. Com o objetivo de elucidar esse fenômeno, métodos analíticos foram desenvolvidos e aplicados utilizando sangue total (ST), humor vítreo (HV) e fígado. Para as amostras de ST e HV, o método de extração escolhido e validado foi a microextração em fase líquida (LPME) trifásica. Fibras ocas constituídas de polipropileno, com a extensão de 8 cm cada, foram tratadas com o solvente orgânico dodecano (fase orgânica), resultando em um membrana com permeabilidade seletiva. No lúmen destas fibras, adicionou-se ácido fórmico 0,1 mol/L (fase aceptora). Em frasco de fundo chato com 5 mL de capacidade, pipetou-se 3,5 mL de NaOH 0,1 mol/L (fase doadora) e 0,5 mL de ST ou HV. Ao término da extração, as amostras foram introduzidas no GC-MS, sem a necessidade de reações de derivatização. O estudo com ST contemplou os antidepressivos amitriptilina (AMI), nortriptilina (NTR), imipramina (IMI), desipramine (DES), clomipramina (CLO), desmetilclomipramina (DMC), fluoxetina (FLU) e norfluoxetina (NFL). Os limites de quantificação para estas substâncias ficaram inferiores aos níveis terapêuticos (20 ng/mL). As médias dos coeficientes de variação intradia e interdia foram, respectivamente, de 9,7 e 9,8%. As curvas de calibração apresentaram linearidade entre as concentrações de 20 até 1200 ng/mL. A validação do parâmetro integridade da diluição assegurou a mensuração de quantidades superiores ao limite apresentado na curva de calibração. O método foi aplicado em sete amostras reais postmortem e em apenas um caso foi observada uma diferença significativa (300%) entre os valores quantificados no ST periférico e central. Os antidepressivos tricíclicos AMI, NTR, IMI e DES foram avaliados no HV e o efeito matriz foi detectado para os dois últimos analitos. O método foi otimizado e validado utilizando solução salina adicionada de AMI e NTR. O limite de detecção igual a 5 ng/mL, foi obtido com a redução da voltagem da fonte de íons do espectrômetro de massa para 50 eV. Coeficientes de variação foram inferiores a 15%. Os procedimentos validados foram aplicados em seis amostras reais de HV. A relação encontrada entre os valores obtidos no ST periférico e HV foi de aproximadamente 0,1. A extração acelerada por solvente (ASE) e, posteriormente, a extração em fase sólida (SPE) foram as técnicas de separação dos analitos da matriz fígado. Ao término das citadas extrações, os antidepressivos foram analisados no GC-MS. Para esta matriz sólida, são necessários mais estudos, pois os valores encontrados nos ensaios analíticos estão em desacordo com as diretrizes utilizadas na validação dos métodos. / Antidepressants belong to an important class of drugs investigated in forensic toxicology. In cases of samples from corpses, the interval between death and obtaining the biological specimens can provide the postmortem redistribution of these drugs. Aiming to elucidate this phenomenon, analytical methods were developed and applied using whole blood (WB), vitreous humor (VH) and liver. For samples of WB and HV, the extraction method chosen and validated was the three-phase liquid phase microextraction (LPME). Hollow fibers consist of polypropylene, with a length of 8 cm each were treated with dodecane organic solvent (organic phase) resulting in a membrane with selective permeability. Into the lumen of these fibers was added formic acid 0.1 mol/ L (acceptor phase). In the vial containing 3.5 mL of NaOH 0.1 mol / L (donor phase) was spiked 0.5 ml of biological fluids (WB or VH). Subsequently, the samples were injected in GC-MS without derivatization reactions. The study of the ST included antidepressants amitriptyline (AMI), nortriptyline (NTR), imipramine (IMI), desipramine (DES), clomipramine (CLO), desmethylclomipramine (DMC), fluoxetine (FLU) and norfluoxetine (NFL). The quantification limits for these substances were below the therapeutic levels (20 ng / ml). The mean coefficients of variation and separate intradays were respectively 9.7 and 9.8%. The calibration curves showed linearity between concentrations of 20 to 1200 ng / mL. The validation of the integrity of the dilution parameter assured measurement higher than the limit shown in the calibration curve quantities. The method was applied to seven real postmortem samples and in one case a significant difference (300%) between the measured values in the peripheral and central ST was observed. The tricyclic antidepressants AMI, NTR, IMI and DES were evaluated in VH and the matrix effect was detected in the last two analytes. The method was optimized and validated using saline spiked AMI and NTR. The limit of detection (5 ng/ml) was obtained by reducing the voltage of the ion source of the mass spectrometer 50 eV. Coefficients of variation were below 15%. The procedures were validated in six real samples of HV. The relationship found between the values obtained in the peripheral ST and HV was approximately 0.1. Accelerated solvent extraction (ASE) and subsequently the solid phase extraction (SPE) were the techniques of separation of analytes liver matrix. At the end of the cited extractions, antidepressants were analyzed in GC-MS. To this solid tissue, further studies are needed, because the values found in the analytical tests were not in accordance with the guidelines used in the validation of the methods.

Les détecteurs de rayon-X utilisés pour l'imagerie à haute résolution (micromètrique ou submicronique) utilisés aux synchrotrons sont pour la plupart basés sur un système de détection indirecte. Les rayons X ne sont pas directement convertis en signal électrique. Ils sont absorbés par un scintillateur qui est un matériau émettant de la lumière à la suite de l'absorption d'un rayonnement ionisant. L'image émise sous forme de lumière visible est ensuite projetée par des optiques de microscopie sur une camera 2D de type CCD ou CMOS. De nos jours, il existe différents types des scintillateurs. On distingue entre autres des scintillateurs en poudre compactée, micro structurés, céramique poly-cristalline et monocristalline. L’obtention d’une image de très bonne qualité avec une résolution spatiale au-dessous du micromètre requiert le choix d’une couche mince (1-20 µm) monocristalline. Ces types des scintillateurs peuvent être déposes sur un substrat par épitaxie en phase liquide. La très faible efficacité d’absorption dans une couche mince en fait sa faiblesse, surtout pour des énergies au-dessus de 20 keV. A l’ESRF (le synchrotron européen) des énergies jusqu'à 120 keV peuvent être exploitées pour l’imagerie. Des nouveaux scintillateurs sont donc toujours recherchés pour pouvoir améliorer le compromis entre l’efficacité d’absorption et la résolution spatiale. Dans la première partie de cet travail, un model qui décrit les détecteurs indirects pour la haute résolution, est présenté. Cet model permet de calculer la MTF (fonction de transfert de modulation) du système et peut être utilisé pour trouver la combinaison optimal de scintillateur et d’optique selon l’énergie des rayons X. Les simulations ont guidées le choix des scintillateurs à développer par épitaxie.Dans la deuxième partie, deux nouveaux types de scintillateurs développés et caractérisés dans le cadre de ce projet de thèse sont introduits : les couches minces basées sur des monocristaux de gadolinium lutétium aluminium pérovskite (GdLuAP:Eu) et d’oxyde de lutétium (Lu2O3:Eu) / X-ray detectors for high spatial resolution imaging are mainly based on indirect detection. The detector consists of a converter screen (scintillator), light microscopy optics and a CCD or CMOS camera. The screen converts part of the absorbed X-rays into visible light image, which is projected onto the camera by means of the optics. The detective quantum efficiency of the detector is strongly influenced by the properties of the converter screen (X-ray absorption, spread of energy deposition, light yield and emission wavelength). To obtain detectors with micrometer and sub-micrometer spatial resolution, thin (1-20 µm) single crystal film scintillators are required. These scintillators are grown on a substrate by liquid phase epitaxy. The critical point for these layers is their weak absorption, especially at energies exceeding 20 keV. At the European Synchrotron radiation Facility (ESRF), X-ray imaging applications can exploit energies up to 120 keV. Therefore, the development of new scintillating materials is currently investigated. The aim is to improve the contradictory compromise between absorption and spatial resolution, to increase the detection efficiency while keeping a good image contrast even at high energies.The first part of this work presents a model describing high-resolution detectors which was developed to calculate the modulation transfer function (MTF) of the system as a function of the X-ray energy. The model can be used to find the optimal combination of scintillator and visible light optics for different energy ranges, and it guided the choice of the materials to be developed as SCF scintillators. In the second part, two new kinds of scintillators for high-resolution are presented: the gadolinium-lutetium aluminum perovskite (Gd0.5Lu0.5AlO3:Eu) and the lutetium oxide (Lu2O3:Eu) SCFs

<p>Supersaturating drug delivery systems are an attractive solubility enabling formulation strategy for poorly soluble drugs due to their potential to significantly enhance solubility and hence, bioavailability. Compendial dissolution testing is commonly used a surrogate for assessing the bioavailability of enabling formulations. However, it increasingly fails to accurately predict <i>in vivo</i> performance due its closed-compartment characteristics and the lack of absorptive sink conditions. <i>In vivo</i>, drug is continually removed due to absorption across the gastrointestinal membrane, which impacts the luminal concentration profile, which in turn affects the dissolution kinetics of any undissolved material, as well as crystallization kinetics from supersaturated solutions. Thus, it is critical to develop an improved methodology that better mimics <i>in vivo</i> conditions. An enhanced approach integrates dissolution and absorption measurements. However, currently-used two-compartment absorptive apparatuses, employing a flat-sheet membrane are limited, in particular by the small membrane surface area that restricts the mass transfer, resulting in unrealistic experimental timeframes. This greatly impacts the suitability of such systems as a formulation development tool. The goal of this research is two-fold. First, to develop and test a high surface area, flow-through, absorptive dissolution testing apparatus, designed to provide <i>in vivo</i> relevant information about formulation performance in biologically relevant time frames. Second, to use this apparatus to obtain mechanistic insight into physical phenomenon occurring during formulation dissolution. Herein, the design and construction of a coupled dissolution-absorption apparatus using a hollow fiber membrane module to simulate the absorption process is described. The hollow fiber membrane offers a large membrane surface area, improving the mass transfer rates significantly. Following the development of a robust apparatus, its application as a formulation development tool was evaluated in subsequent studies. The dissolution-absorption studies were carried out for supersaturated solutions generated via anti-solvent addition, pH-shift and by dissolution of amorphous formulations. The research demonstrates the potential of the apparatus to capture subtle differences between formulations, providing insight into the role of physical processes such as supersaturation, crystallization kinetics and liquid-liquid phase separation on the absorption kinetics. The study also explores dissolution-absorption performance of amorphous solid dispersions (ASDs) and the influence of resultant solution phase behavior on the absorption profile. Residual crystalline content in ASDs is a great concern from a physical stability and dissolution performance perspective as it can promote secondary nucleation or seed crystal growth. Therefore, the risk of drug crystallization during dissolution of ASDs containing some residual crystals was assessed using absorptive dissolution measurements and compared to outcomes observed using closed-compartment dissolution testing. Mesoporous silica-based formulations are another type of amorphous formulations that are gaining increased interest due to higher physical stability and rapid release of the amorphous drug. However, their application may be limited by incomplete drug release resulting from the adsorption tendency of the drug onto the silica surface. Thus, the performance of mesoporous silica-based formulations was also evaluated in the absorptive dissolution testing apparatus to determine the impact of physiological conditions such as gastrointestinal pH and simultaneous membrane absorption on the adsorption kinetics during formulation dissolution. Overall, the aim of this research was to demonstrate the potential of the novel <i>in vitro</i> methodology and highlight the significance of a dynamic absorptive dissolution environment to enable better assessment of complex enabling formulations. <i>In vivo</i>, there are multiple physical processes occurring in the gastrointestinal lumen and the kinetics of these processes strongly depend on the absorption kinetics and <i>vice-a-versa</i>. Thus, using this novel tool, the interplay between solution phase behavior and the likely impacts on bioavailability of supersaturating drug delivery systems can be better elucidated. This approach and apparatus is anticipated to be of great utility to the pharmaceutical industry to make informed decisions with respect to formulation optimization.</p>

In the present dissertation the formation of microstructure, the kinetics of densification and the formation of surface layers developing during liquid phase sintering of silicon carbide are studied. The focus is on the additive systems Al2O3 plus Y2O3 and AlN plus Y2O3. Phase and especially liquid phase formation in both of the systems SiC, Al2O3 , Y2O3 and AlN, Al2O3 , Y2O3 are investigated in detail examining 12 espectively 17 different compositions per system. Melting temperatures have been determined by TG/DTA, in both systems for the first time. Phase composition of samples was analysed by the combination of XRD, SEM and EDX. In the system SiC, Al2O3 , Y2O3 the formation of the phases expected from the quasibinary Al2O3 , Y2O3 could be observed thus silicon carbide has to be in equilibrium with the oxide additives. The low solubility of SiC in the oxide melt, which was suggested by Hoffmann and Nader, could be confirmed. In the system AlN, Al2O3 , Y2O3 the formation of phases as stated by Medraj was confirmed, except for the dimension of the stability region of the γ- spinel and YAG which is wider in the present work. For the first time diffusion coefficients of the species Y3+ and Al3+ in the oxide melt formed by Al2O3 and Y2O3 at temperatures above 1825 ◦ C were determined. The values are in the order of 2 · 10−6 cm2 /s which results in a diffusion length of 14.1 μm for a diffusion time of one second. This allows the fast equilibration of Y and Al deficiencies. Kinetics of densification was modeled by kinetic field, master curve and thermokinetic method, based on detailed experimental investigation of the shrinkage during liquid phase sintering of SiC. It could be proved that the first 30 − 40 % of densification are controlled by solid phase reactions which accelerate particle rearrangement without presence of a liquid phase. During the remaining 60 − 70 % of densification a liquid is present, resulting in the predominance of mechanisms of liquid phase sintering. The models deliver activation energies in the range from 608 KJ/mol to 1668 kJ/mol and allow, within the scope of validity of each method the prediction of densification during liquid phase sintering of silicon carbide. When sintering silicon carbide with Al2O3 plus Y2O3 the formation of several surface layers, depending on atmosphere, maximum temperature, dwelling time and amount and composition of additives was observed. In nitrogen atmosphere with low partial pressures a surface layer consisting of AlN is forming whilst at high partial pressures SiAlON- polytypes occur. After sintering in Argon or Ar-CO- atmosphere three main types of surface layers are present. One consists of alumina, one contains only YAG and one shows highly porous, additive depleted regions. An explanation for the formation of the several surface layers could be given by the combination of the determined diffusion coefficients with the results achieved in the thermodynamics part. The results achieved in this work can be a contribution to the knowledge based design of the production process of liquid phase sintering of silicon carbide.

Le système ubiquitine-protéasome représente une plateforme de signalisation cellulaire chez les eucaryotes et joue un rôle majeur dans la coordination des processus cellulaires. Des progrès récents suggèrent que l’ubiquitination joue un rôle important dans les phénomènes de séparation de phase liquide-liquide (LLPS), un processus permettant la localisation d’une quantité accrue de protéines dans un compartiment subcellulaire, afin de réaliser une fonction biologique. En effet, il a été démontré que l’ubiquitination joue un rôle central dans les mécanismes qui gouvernent la LLPS durant la formation des granules de stress dans le cytoplasme ou les foci de réparation de l’ADN dans le noyau. D’autre part, chez la levure, des travaux ont montré que le protéasome est capable de s’assembler sous forme de granules dans le cytoplasme suite à un stress métabolique. Toutefois, les mécanismes par lesquels le système ubiquitine-protéasome ainsi que ses régulateurs contrôlent les processus de LLPS restent à déterminer. Dans la première étude de cette thèse, nous avons investigué le mécanisme d’action de la déubiquitinase USP16, qui a été suggérée comme un régulateur négatif de la LLPS, empêchant la formation des foci de réparations de dommages à l’ADN. Cependant, nos résultats démontrent que USP16 est majoritairement cytoplasmique et que seulement une entrée forcée de USP16 dans le noyau empêche la formation des foci de réparation des cassures double brin induites par des radiations ionisagntes et ce en favorisant la déubiquitination de l’histone H2A. De plus, aucune translocation nucléaire de USP16 n’a été observée durant le cycle cellulaire ou suite à des dommages à l’ADN. Nos travaux montrent que USP16 est activement exclue du noyau via son signal d’export nucléaire et régulerait indirectement la LLPS menant à la formation des foci de réparation de l’ADN. Dans la deuxième étude, nous décrivons le comportement dynamique des protéines du protéasome lors d’une LLPS induite par un stress métabolique. Nos résultats indiquent que le protéasome forme des foci distincts dans le noyau des cellules humaines en réponse à une privation de nutriments. Nous avons constaté que ces foci sont enrichis en ubiquitine conjuguée et nous avons démontré que le récepteur d’ubiquitine Rad23B ainsi que l’absence des acides aminés non essentiels sont des éléments clés nécessaires à l’assemblage de ces foci du iv protéasome. De plus, des expériences de survie cellulaire montrent que la présence de ces foci est associée à la mort des cellules par apoptose. En conclusion, nos travaux mettent en lumière l’importance du système ubiquitine-protéasome dans la formation et la régulation des foci cellulaires suite à une LLPS. De même, cette étude aidera également à approfondir notre compréhension sur les mécanismes qui gouvernent l’homéostasie des protéines, la survie cellulaire et le développement du cancer. / The ubiquitin-proteasome system represents a major cell-signaling platform in eukaryotes and plays a pivotal role in the coordination of cellular processes. Recent studies provided evidence that ubiquitination plays a role in liquid-liquid phase separation (LLPS), a process that results in the localization of highly increased levels of a protein in a defined subcellular compartment, in order to achieve a biological function. Indeed, ubiquitination has been shown to play a central role in the mechanisms that govern LLPS and subsequent formation of stress granules in the cytoplasm or the DNA repair foci in the nucleus. On the other hand, several studies have shown that the proteasome itself is able to form granules in the cytoplasm following metabolic stress in yeasts. However, the mechanisms by which the ubiquitin-proteasome system and its regulators control LLPS processes remain to be determined. In the first study of this thesis, we investigated the mechanism of action of USP16 deubiquitinase, which has been suggested as a negative regulator of LLPS preventing the formation of DNA damage repair foci. However, our results demonstrate that USP16 is predominantly cytoplasmic and that only enforced nuclear entry of USP16 prevents the formation of repair foci after double strand breaks induced by ionizing radiation, and this by promoting the deubiquitination of histone H2A. In addition, no nuclear translocation of USP16 was observed during cell cycle or following DNA damage. Our study shows that USP16 is actively excluded from the nucleus via its nuclear export signal and would indirectly regulate LLPS that lead to DNA repair foci. In the second study, we describe the dynamic behavior of proteasome proteins during metabolic stress, a process that involves LLPS. Our results indicate that the proteasome forms distinct foci in the nucleus of human cells in response to nutrients deprivation. We found that these foci are enriched with conjugated ubiquitin and demonstrated that the ubiquitin receptor Rad23B as well as the absence of nonessential amino acids are the key elements necessary for the assembly of these proteasome foci. In addition, cell survival experiments show that the presence of these foci is associated with cell death by apoptosis. In conclusion, our work has shed new light on the importance of the ubiquitin-proteasome system in the formation and regulation of cell foci following LLPS. Likewise, this vi study will also help deepen our understanding of the mechanisms leading to protein homeostasis, cell survival and cancer development.

Silizium basierende Technologie bestimmt den technologischen Fortschritt in der Welt und ist weiterhin ein Material für die weitere Entwicklung von Schlüsseltechnologien. Die Änderung der Silizium-Materialeigenschaft der optischen und elektronische Bandlücke durch die Reduktion der Materialdimension auf die Nanometerskala ist dabei von besonders großem Interesse. Die meisten Silizium-Nanomaterialien bestehen aus Punkt-, Kugel- oder Drahtformen. Ein relativ neues Materialsystem sind dreidimensionale, durchdringende, Nano-Komposit Netzwerke aus Silizium in einer Siliziumdioxid Matrix. Die vorliegende Arbeit untersucht die Entstehung von dreidimensionalen Silizium-Nanokomposit-Netzwerken durch Abscheidung eines siliziumreichen Siliziumoxids(SiOx, mit x<2) und anschlieÿender thermischen Behandlung. Hierbei wurden die reaktive Ionenstrahl-Sputterabscheidung (IBSD), sowie das reaktive Magnetronsputtern (RMS) verglichen. Auch wurden die Unterschiede zwischen klassischer Ofen und Millisekunden-Linienlaser Behandlung untersucht. Abgeschiedene und thermisch behandelte Dünnschichten wurden hinsichtlich der integralen Zusammensetzung, Homogenität, Morphologie und Struktur mittels Rutherford-Rückstreuspektroskopie, Ramanspektroskopie, Röntgenbeugung, spektroskopische Ellipsometrie, Photospektrometrie und (Energie gefilterter) Transmissionselektronenmikroskopie untersucht. Abhängig von der Abscheidemethode und des thermischen Ausheilprozesses wurden unterschiedliche Strukturgrößen und Kristallisationsgrade erzeugt. Insbesondere wurde gezeigt, dass während der 13 ms langen Laserbearbeitung (Ofen: 90 min) wesentlich größere Strukturen (laser:~50 nm; oven:~10 nm) mit einer deutlich höheren Kristallinität (laser:~92-99%; oven:~35-80%) entstehen. Darüber hinaus erhält sich die abscheidebedingte Morphologie nach der Ofenbehandlung, verschwindet jedoch nach der Laserprozessierung. Erklärt wurde dies mit einem Prozess über die flüssige Phase während der Laserbearbeitung, im Gegensatz zu einem Festphasenprozess bei der Ofenbehandlung. Abschließend wurde gezeigt, dass absichtlich eingebrachte vertikale und horizontale Schwankungen der Zusammensetzung genutzt werden können, um definierte Silizium Nanonetzwerke mit einer dreidimensionalen quadratischen Netzstruktur herzustellen.:1 Introduction 2 Fundamentals 2.1 The silicon - silicon oxide system 2.1.1 The Si-O phase diagram 2.1.2 Chemical reaction consideration 2.2 Phase separation of binary systems 2.2.1 Phase separation regimes 2.2.2 Diffusion in solids 2.3 Different types of silicon nanostructures 2.3.1 0D - Silicon nanoparticles 2.3.2 1D - Silicon nanowires 2.3.3 3D - Silicon nanonetworks 3 Experimental methods 3.1 SiOx thin film deposition 3.1.1 SiOx thin films by ion beam sputter deposition 3.1.2 SiOx thin films by reactive magnetron sputter deposition 3.1.3 Comparison of ion beam and magnetron sputter deposition 3.2 Thermal processing of as-deposited SiOx thin films 3.2.1 Oven treatment 3.2.2 Laser treatment 3.3 Thin-film characterization 3.3.1 Rutherford backscattering 3.3.2 Spectroscopic ellipsometry and photospectrometry 3.3.3 Raman spectroscopy 3.3.4 X-ray diffraction 3.3.5 Transmission electron microscopy 4 Results 4.1 Accessible SiOx compositions as a function of deposition and annealing method 4.2 Structure and properties of ion beam sputter deposited SiOx thin films before and after thermal processing 4.2.1 Phase- and microstructure of SiO0:6 thin films deposited by ion beam sputter deposition at 450°C 4.2.2 Phase- and microstructure of SiO0.6 thin films deposited by ion beam sputter deposition at room temperature 4.3 Structure and properties of reactive magnetron sputter deposited SiOx thin films before and after thermal processing 4.4 Multilayer SiOx films for the generation of defined squared mesh structures 5 Discussion 5.1 Compositional homogeneity of SiO0:6 thin films before and after thermal treatment 5.2 Phase structure of as-deposited SiOx thin films 5.3 Influence of the thermal treatment on the structural properties of percolated Si:SiO2 nanostructures 5.3.1 Observed structural properties 5.3.2 Origin of different structure sizes - liquid vs. solid state crystallization 5.4 Influence of the deposition temperature during ion beam sputtering on the structural properties of percolated Si:SiO2 nanostructures before and after thermal processing 5.5 Influence of the deposition method on the structural properties of percolated Si:SiO2 nanostructures 5.6 Formation of interface layers and electrical characterization 6 Summary and outlook 6.1 Summary 6.2 Outlook A EFTEM imaging / Silicon-based technology determines the technological progress in the world significantly and is still a material of choice for further development of key technologies. In particular the reduction of silicon structure sizes to a nanometer scale are of great interest. Most silicon nano structures are based on spherical, dot-like or cylindrical, wire-like geometries. A relatively new material system are three dimensional percolated nanocomposite networks of silicon within a silica matrix. To form any of these nano structures fast, room temperature processes are desired which also offer the possibility of structure modification by different process management. The present work studies the formation of three-dimensional silicon nanocomposite networks by the deposition of a silicon rich silicon oxide (SiO x , with x < 2) and subsequent thermal treatment. Thereby, reactive ion beam sputter deposition (IBSD) as well as reactive magnetron sputtering (RMS) was compared. As well, the differences between a conventional oven and a millisecond line-focused diode laser were studied. As-deposited and thermally treated thin films were characterized with regard to the overall mean composition, homogeneity, morphology and structure by Rutherford backscattering, Raman spectroscopy, X-ray diffraction, spectroscopic ellipsometry, photospectrometry as well as cross-sectional and energy-filtered transmission electron microscopy. Depending on the deposition method as well as the thermal treatment process different structure sizes and degrees of crystallization were achieved. Most notably it was found, that during 13 ms laser processing (oven: min. 90 min), much bigger structures (laser: ≈ 50 nm; oven: ≈ 10 nm) with a notably higher degree of crystallization (laser: ≈ 92-99%; oven: ≈ 35-80%) evolve. Moreover, the structure morphology after deposition is preserved during oven treatment but diminishes following laser processing. This was explained by a process via the liquid phase for laser processing in contrast to a solid state process during oven treatment. Finally it was shown, that intentional introduced vertical and horizontal composition fluctuations can be used to form well-defined silicon nano-networks with a three dimensional square mesh structure.:1 Introduction 2 Fundamentals 2.1 The silicon - silicon oxide system 2.1.1 The Si-O phase diagram 2.1.2 Chemical reaction consideration 2.2 Phase separation of binary systems 2.2.1 Phase separation regimes 2.2.2 Diffusion in solids 2.3 Different types of silicon nanostructures 2.3.1 0D - Silicon nanoparticles 2.3.2 1D - Silicon nanowires 2.3.3 3D - Silicon nanonetworks 3 Experimental methods 3.1 SiOx thin film deposition 3.1.1 SiOx thin films by ion beam sputter deposition 3.1.2 SiOx thin films by reactive magnetron sputter deposition 3.1.3 Comparison of ion beam and magnetron sputter deposition 3.2 Thermal processing of as-deposited SiOx thin films 3.2.1 Oven treatment 3.2.2 Laser treatment 3.3 Thin-film characterization 3.3.1 Rutherford backscattering 3.3.2 Spectroscopic ellipsometry and photospectrometry 3.3.3 Raman spectroscopy 3.3.4 X-ray diffraction 3.3.5 Transmission electron microscopy 4 Results 4.1 Accessible SiOx compositions as a function of deposition and annealing method 4.2 Structure and properties of ion beam sputter deposited SiOx thin films before and after thermal processing 4.2.1 Phase- and microstructure of SiO0:6 thin films deposited by ion beam sputter deposition at 450°C 4.2.2 Phase- and microstructure of SiO0.6 thin films deposited by ion beam sputter deposition at room temperature 4.3 Structure and properties of reactive magnetron sputter deposited SiOx thin films before and after thermal processing 4.4 Multilayer SiOx films for the generation of defined squared mesh structures 5 Discussion 5.1 Compositional homogeneity of SiO0:6 thin films before and after thermal treatment 5.2 Phase structure of as-deposited SiOx thin films 5.3 Influence of the thermal treatment on the structural properties of percolated Si:SiO2 nanostructures 5.3.1 Observed structural properties 5.3.2 Origin of different structure sizes - liquid vs. solid state crystallization 5.4 Influence of the deposition temperature during ion beam sputtering on the structural properties of percolated Si:SiO2 nanostructures before and after thermal processing 5.5 Influence of the deposition method on the structural properties of percolated Si:SiO2 nanostructures 5.6 Formation of interface layers and electrical characterization 6 Summary and outlook 6.1 Summary 6.2 Outlook A EFTEM imaging

Thin transparent conductive layers containing ATO nanoparticles are a modern material that has found use in a wide range of optoelectronic applications. For liquid phase deposition there were designed and prepared compositions using a „brick and mortar“ approach combined templating agents. A sol-gel solution formed of inorganic precursors of tin chloride and antimony trichloride in the presence of ATO nanoparticles was mixed with a surfactant to improve the structure and wettability of applied films. Polyethylene glycol, polyoxyethylene (20)cetylether, sodium dioctylsulfosuccinate and polyvinylpyrrolidone were used as templating agents. Thin layers of these compositions were applied by the spin-coating method. Characterized parameters were resistivity, thickness and turbidity. A resul compositions showed relatively good electrical properties and high transparency and a potencial to be used for material printing.

In thisproject, solubility of butyl paraben in 7 puresolvents and 5 ethanol aqueous solvents has been determined at from 1 ℃to 50 ℃. Thermodynamic properties of butyl paraben have been measured by DifferentialScanning Calorimetey. Relationship between molar solubility of butyl paraben in6 pure solvents and thermodynamic properties has been analyzed. Thisrelationship suggests a method of estimating activity of solute at equilibrium fromcombining solubility data with DSC measurements. Then, activity coefficient accordingto the solubility at different temperatures can be estimated. Duringthe solubility measurements in ethanol aqueous solvents, it is found that whenbutyl paraben is added into aqueous solutions with certain proportion ethanol,solutions separates into two immiscible liquid layers in equilibrium. Water andethanol are primary in top layer, while the butyl paraben is primary in bottomlayer, but the solution turns to cloudy when two layers of solution are mixed. Theaim of this work was to present the phase behaviour of liquid-liquid-phaseseparation for (butyl paraben + water + ethanol) ternary system from 1 ℃ to 50 ℃at atmospheric pressure. Thearea of liquid-liquid-phase separation region in the ternary phase diagram increaseswith the increasing temperature from 10 ℃to 50 ℃. In thisstudy, more than several hundreds of nucleation experiments of butyl paraben havebeen investigated in ethyl acetate, propanol, acetone and 90% ethanol aqueoussolution. Induction time of butyl paraben has been determined at 3 differentsupersaturation levels in these solvents, respectively. Free energy ofnucleation, solid-liquid interfacial energy, and nuclei critical radius havebeen determined according to the classical nucleation theory. Statistical analysis ofinduction time reveals that the nucleation is a stochastic process with widevariation even at the same experiment condition. Butyl paraben nucleates most difficultlyin 90 % ethanol than in other 3 solvents, and most easily in acetone. The interfacialenergy of butyl paraben in these solvents tends to increasing with decreasemole fraction solubility in these solvents. Coolingcrystallizations with different proportions of butyl paraben, water and ethanolhave been observed by Focused Beam Reflectance Method, Parallel VirtualMachine, and On-line Infrared. The FBRM, IR curves and the PVM photos show someof the solutions appeared liquid-liquid phase separation during coolingcrystallization process. The results suggest that if solutions went throughliquid-liquid phase separation region during the cooling crystallizationprocess the distribution of crystals crystal was poor. Droplets from solutions withsame proportion butyl paraben but different proportions of water and ethanolhave been observed under microscope. Induction time of the droplets has been determinedunder the room temperature. Droplets from top layer or bottom layer of solutionwith liquid-liquid phase separation on small glass or plastic plates were alsoobserved under microscope. The microscope photos show that the opposite flows ofcloudy solution on the glass and the plastic plate before nucleation. The resultsof the cooling and evaporation crystallization experiments both revealed thatnucleation would be prevented by the liquid-liquid phase separation. / QC 20110630