Les rendements de fission sont des données importantes pour les applications nucléaires ainsi que pour les modèles théoriques qui cherchent à reproduire ces distributions. Les rendements des produits de fission légers pour de nombreux noyaux ont été mesurés par le passé sur le spectromètre Lohengrin. Mais la méthode expérimentale utilisée, détection par chambre à ionisation, ne permet pas la séparation des isotopes pour les produits de fission lourds. Pour valider la méthode dans cette région et compléter les bibliothèques, les rendements isobariques de l’235U(nth,f), du 239Pu(nth,f) et du 241Pu(nth,f) ont été mesurés. La mise en place d’un nouveau dispositif de détection gamma sur le spectromètre a permis de déterminer les rendements isotopiques du 239Pu(nth,f). De plus les distributions en charge ionique et en énergie cinétique des produits de fission ont été étudiées, et ont mis en évidence la présence d'isomères nanosecondes pour certains de ces noyaux. / In spite of the huge amount of fission yield data available in different libraries, more accurate values are still needed for nuclear energy applications and to improve our understanding of the fission process. Thus measurements of fission yields were performed at the mass spectrometer Lohengrin at the Institut Laue-Langevin in Grenoble, France. The mass separator Lohengrin is situated at the research reactor of the institute and permits the placement of an actinide layer in a high thermal neutron flux. It separates fragments according to their atomic mass, kinetic energy and ionic charge state by the action of magnetic and electric fields. Coupling with a high resolution ionization chamber the experiment was used to investigate the mass and isotopic yields in the light mass region. Almost all fission yields of isotopes from Th to Cf have been measured at Lohengrin with this method. It has been extended in this work to the heavy mass region for the reactions 235U(nth,f), 239Pu(nth,f) and 241Pu(nth,f). For these higher masses an isotopic separation is no longer possible. That is why a new method was undertaken with the reaction 239Pu(nth,f) to determine the isotopic yields by gamma spectrometry. During these experiments the ionic charge state and kinetic energy distributions have been measured. Nanosecond isomers have been discovered for some nuclei thanks to a non gaussian charge state distribution. The kinetic energy distributions present very interesting structures which have been also discussed.

Les travaux portent sur l’endommagement laser en régime nanoseconde aux longueurs d’onde 355 nm et 266 nm. L'objectif de cette étude est de comprendre et d'analyser les processus mis en jeu lors de l'endommagement laser en surface et en volume de matériaux optiques, massifs ou en couches minces, lors de tirs répétés. Dans ce contexte, un banc d'endommagement laser a été entièrement mis en place et automatisé. Il permet d'analyser la résistance et le vieillissement de ces composants sous irradiation UV à des fréquences de tir de 50Hz, pour un grand nombre de tirs et de relever de façon systématique les paramètres du test les plus importants (profiles spatiaux et énergies des impulsions, images du site avant et après dommage). Pour une meilleure compréhension des phénomènes physiques conduisant à la fatigue des matériaux en tirs laser répétés, un modèle a été développé afin de discriminer les effets statistiques (dus au grand nombre de tirs impliqués) de modifications du matériau sous flux UV. Ce modèle a été validé expérimentalement dans le cas de la silice synthétique étudiée en volume. En ce qui concerne les couches minces, une étude multi-paramètres de la tenue au flux UV de mixtures d'oxydes a été menée, en partenariat avec le Laser Zentrum Hannover (LZH, Allemagne). Ces matériaux ont en effet un comportement complexe et encore mal connu, en particulier en tirs répétés. Enfin, une partie du travail de thèse est consacrée à la caractérisation non-destructive de cristaux de KDP par photoluminescence pompée dans l'UV, réalisée dans le contexte du laser MégaJoule en collaboration avec le CEA Le Ripault (Monts). / The work is devoted to laser-induced damage in the nanosecond regime at the wavelengths of 266 nm and 355 nm. The goal of this study is to understand and to analyze the processes taking place during multi-pulse irradiation causing laser-damage, on the surface and in the bulk of massive or thin-films optical materials. To this end, a laser-damage experiment was entirely set up and automated. It allows analyzing the laser-damage resistance and the ageing of these components under UV irradiation at a pulse repetition rate of 50 Hz and for a high number of laser pulses and to record systematically the most important test parameters (spatial beam profiles, energies, images of the site before and after irradiation).To better understand the physical phenomena leading to fatigue effects in the materials under multiple pulse irradiation, a model was developed allowing the discrimination of statistical effects (due to the high number of shots) from material modifications under UV irradiation. This model was confirmed by testing synthetic fused silica irradiated in the bulk. Concerning thin-film coated components, oxide mixtures were studied in collaboration with the Laser Zentrum Hannover (LZH, Germany) using a multi-parameter approach. These materials show indeed a complex behavior and remain poorly known, in particular under multi-pulse irradiation. Finally, a part of the work is dedicated to the non-destructive characterization of KDP crystals by UV-pumped photoluminescence, realized in the framework of the MegaJoule project, in collaboration with CEA Le Ripault (Monts, France).

Il est possible de perméabiliser la membrane plasmique des cellules par des agents chimiques (tels que les polyéthylènes glycols ou le diméthylsulfoxyde) ou par des agents physiques (tels que les ultrasons ou les impulsions électriques). Cette perméabilisation peut être réversible ou non, ce qui signifie qu’après la perméabilisation, la membrane retrouve son intégrité et ses propriétés d’hémi-perméabilité ou pas. Ces techniques peuvent être utilisées pour faire rentrer des médicaments ou des acides nucléiques dans les cellules ou pour générer des fusions cellulaires. Une approche récente, la dynamique moléculaire, utilise des simulations numériques pour prédire les effets des agents perméabilisants sur les membranes à l’échelle moléculaire, et permet d’apporter de nouvelles données pour comprendre les mécanismes moléculaires, encore peu connus à ce jour.Les impulsions dites « classiques » en électroperméabilisation, de l’ordre de la dizaine de millisecondes à la centaine de microsecondes et d’amplitude de champ de l’ordre de 100 kV/m, perméabilisent la membrane plasmique uniquement. Cependant, récemment, des impulsions plus courtes, dites impulsions nanoseconde (quelques nanosecondes) et de plus grande amplitude de champ (de l’ordre de 10 MV/m) ont été utilisées et permettent d’affecter également les membranes des organites cellulaires. Les travaux de cette thèse portent dans un premier temps sur les effets perméabilisants d’un agent chimique (le diméthylsulfoxyde, DMSO) en comparant les modèles prédictifs de la dynamique moléculaire avec des expériences in vitro sur des cellules. Le modèle numérique prédit trois régimes d’action en fonction de la concentration du DMSO. Utilisé à faible concentration, il y a déformation de la membrane plasmique. L’utilisation d’une concentration intermédiaire entraîne la formation de pores membranaires et les fortes concentrations de DMSO ont pour conséquence la destruction de la membrane. Les expériences in vitro faites sur des cellules ont confirmé ces résultats en suivant l’entrée de marqueurs de perméabilisation. Cette étude a été comparée avec la perméabilisation par un agent physique (les impulsions électriques). Dans un deuxième temps, ces travaux traitent du développement et de l’utilisation d’un nouveau dispositif d’exposition des cellules aux impulsions nanoseconde qui permet d’appliquer des champs électriques très élevés et d’observer par microscopie leurs au niveau cellulaire. Pour finir, ce dispositif a été utilisé avec des impulsions nanoseconde pour générer des pics calciques dans de cellules souches mésenchymateuses qui présentent des oscillations calciques spontanées liées à leur état de différenciation. Ces pics induits sont dus à la libération de calcium stocké dans les organites et/ou à la perméabilisation de la membrane plasmique permettant l’établissement d’un flux de calcium intramembranaire. Il est aussi possible d’utiliser des impulsions microseconde pour générer des pics calciques dans ces cellules. Dans ce cas, les pics calciques ne sont dus qu’à la perméabilisation de la membrane plasmique. En jouant sur l’amplitude des champs électriques appliqués et sur la présence ou l’absence de calcium externe, il est possible de manipuler les concentrations calciques cytosoliques en mobilisant le calcium interne ou externe. Une des particularités de ces nouveaux outils est de pouvoir être déclenchés et arrêtés instantanément, sans réminiscence, contrairement aux molécules chimiques permettant de produire des pics calciques. Ces outils pourraient donc permettre de mieux comprendre l’implication du calcium dans des mécanismes comme la différenciation, la migration ou la fécondation. / It is possible to permeabilize the cellular plasma membrane by using chemical agents (as polyethylen glycols or diméthylsulfoxyde) or physical agents (as ulstrasounds or electric pulses). This permeabilization can be reversible or not, meaning that after the permeabilization, the membrane recovers its integrity and its hemi-permeable properties. These techniques can be used for the uptake of medicines or nucleic acids or to generate cellular fusions. A recent approach, the molecular dynamics, uses numerical simulations to predict the effects of permeabilizing agents at the molecular scale, allowed generating of new data to understand the molecular mechanisms that are not completely known yet.The pulses so called “classical” in electropermeabilization, from the range of the ten of milliseconds to the hundred of microseconds and with a field amplitude in the range of 100 kV/m, can only permeabilize the plasma membrane. However, more recently, shorter pulses, so called nanopulses (few nanosecondes) and with an higher field amplitude (in the range of 10 MV/m) have been used and allow to affect also cellular organelles membranes.This thesis is, in a first time, about the permeabilizing effects of a chemical gent (the diméthylsulfoxyde, DMSO) by comparing predictive models from molecular dynamics with experiments in vitro on cells. The numerical model predicts three regimes of action depending on the DMSO concentration. Used at low concentration, there is a plasma membrane deformation. The use of an intermediate concentration lead to membrane pores formation and higher DMSO concentrations resulted in membrane destruction. The experiments done in vitro on cells confirmed these results using the following of permeabilization markers. This study has been compared to permeabilization due to a physical agent (electric pulses).Secondly, it is about the development and the use of a new cell exposure device for nanopulses that permit to apply very high electric fields and to observe induced cellular effects simultaneously by microscopy.To finish, this device has been used with nanopulses to generate calcium peaks in mesenchymal stem cells that are presenting spontaneous calcium oscillations in correlation to their differentiation state.. These induced peaks are due to the release of the calcium stored in organelles and/or to plasma membrane permeabilization leading to a intramembrane calcium flux establishment. It is also possible to use microsecond pulses to generate calcium peaks in these cells. In this case, the calcium peaks are due to the plasma membrane permeabilization . By changing the amplitude of the applied electric fields and the presence or the absence of external calcium, it is possible to manipulate cytosolic calcium concentrations by mobilizing internal or external calcium. One feature of these new tools is to be triggered and stopped instantly without reminiscence, unlike chemical molecules permitting the production of calcium peaks. These tools could therefore lead to a better understanding of the involvement of calcium in mechanisms such as differentiation, migration or fertilization.

A influência das variáveis associadas ao laser como a fluência, o comprimento de onda, e a duração do pulso, assim como as relacionadas às propriedades das amostras, como a distribuição do tamanho das partículas e as características químicas da matriz, foram avaliadas visando à determinação quantitativa de macro- (P, K, Ca, Mg) e micronutrientes (Cu, Fe, Mn, Zn, B) em pastilhas de materiais vegetais por espectrometria de emissão óptica com plasma induzido por laser (LIBS). Os efeitos da distribuição do tamanho das partículas e da fluência do laser foram investigados a partir da análise de amostras peneiradas (150-20 µm) empregando-se um sistema LIBS, em regime temporal de nanossegundos (ns-LIBS), montado com um laser de Nd:YAG a 1064 nm (pulsos de 5 ns e 360 mJ)e um espectrômetro com óptica Echelle e detector ICCD. Observou-se um aumento na sensibilidade e na precisão das medições com a diminuição do tamanho das partículas usadas no preparo das pastilhas, e uma diminuição dos efeitos de matriz causados por diferenças no tamanho das partículas, quando pastilhas preparadas com partículas < 75 µm foram analisadas com pulsos de 50 J cm-2. Verificou-se uma melhora significativa na exatidão das medições de Mg, Fe, Mn e Zn feitas em um conjunto de pastilhas de folhas de cana-de-açúcar (partículas < 75 µm) empregando-se esta fluência. Em uma segunda etapa, observou-se que variações no comprimento de onda do laser de Nd:YAG (1064, 532, 355 e 266 nm) não influenciaram de maneira significativa a precisão e exatidão das medições em pastilhas de folhas de cana-de-açúcar, obtendo-se correlações lineares entre as intensidades dos sinais de emissão e as correspondentes frações de massa dos analitos. Variações no comprimento de onda do laser de Nd:YAG não afetaram a análise de um conjunto heterogêneo de amostras, composto por pastilhas de folhas de plantas de diferentes espécies, como soja, cana-de-açúcar, milho, citros, café, por exemplo, por ns-LIBS. No entanto, diferentemente do observado para o conjunto de pastilhas de folhas de cana-de-açúcar, observou-se, uma baixa correlação (r cal < 0,90) entre as frações de massa de Ca, Mg, P, Cu, Fe, Mn e Zn determinadas por ns-LIBS e os valores de referência, o que demonstra a baixa robustez de ns-LIBS frente às variações na composição química das matrizes. Posteriormente, analisou-se este conjunto heterogêneo de amostras com sistema LIBS, em regime temporal de femtossegundos (fs-LIBS), montado com laser de Ti:Safira (pulsos de 60 fs e 1,65 mJ) e espectrômetro com óptica Czerny-Turner e ICCD. Demonstrou-se que o uso de pulsos em regime de fs proporcionou calibrações e validação menos dependentes da composição química das matrizes. As frações de massa de Ca, Mg, P, Fe e Mn previstas por fs-LIBS foram estatisticamente concordantes com os valores de referência, independentemente do modelo de calibração usado. Além disso, o uso de calibração multivariada melhorou a capacidade preditiva de ns-LIBS, assemelhando-se à de fs-LIBS. Concluiu-se que o emprego de fs-LIBS foi a estratégia mais robusta e que ofereceu maior flexibilidade à variabilidade matricial / The influence of laser properties, such as fluence, wavelength and pulse duration, as well as sample characteristics, such as particle size distribution and chemical matrix composition, was evaluated aiming at the quantitative determination of macro- (P, K, Ca, Mg) and micronutrients (Cu, Fe, Mn, Zn, B) in pellets of plant materials by laser-induced breakdown spectroscopy (LIBS). Firstly, the effects of particle size distribution and laser fluence on the analysis of pellets (test samples) prepared with sieved samples (from 150 to 20 µm apertures) were investigated. Experiments were carried out with a nanosecond LIBS (ns-LIBS) system by using a Q-switched Nd:YAG laser at 1064 nm (5 ns; 360 mJ) and a spectrometer with Echelle optics and intensified charge-coupled device (ICCD) detector. Results indicated that smaller particles yielded to sensitivities\' enhancement and attained better measurements\' precision. Moreover, matrix effects were reduced by analyzing pellets prepared from < 75 ?m sieved fractions and pulses of 50 J cm-2. In addition, there was a significant improvement on accuracy of Mg, Fe, Mn and Zn measurements in a set of test samples of sugarcane leaves by using this fluence. In a second experiment, variations in the Nd:YAG laser wavelength (1064, 532, 355 and 266 nm) did not affect the analysis of test samples of sugarcane leaves, and provided linear correlations between emission signal intensities and corresponding analytes mass fractions. In addition, variations within Nd:YAG laser wavelength did not affect the analysis of a heterogeneous sample set composed by pellets of leaves from different crops, such as soy, sugarcane, maize, citrus and coffee by ns-LIBS. However, in contrast to previous findings, the univariate calibration models for ns-LIBS presented lower linearity (r cal < 0.90) for Ca, Mg, P, Cu, Fe, Mn and Zn, no matter the laser wavelength used for the analysis. These circumstances reflect the low robustness of ns-LIBS to variations within matrix chemical composition among test samples. Afterwards, test samples from different crops were analyzed by a femtosecond LIBS (fs-LIBS) by using a Ti:Sapphire laser, including a mode-locked oscillator and an ultrafast amplifier (60 fs; 1.65 mJ per pulse), and a spectrometer with Czerny-Turner optics and ICCD. Findings indicated that the pulse duration was a decisive variable for providing accurate quantification of nutrients in different plant species, which present substantial differences in terms of matrix chemical composition. Close agreement between Ca, Mg, P, Fe and Mn mass fractions predicted by fs-LIBS and those determined by ICP OES was evidenced, whatever the modeling approach used. Contrarily, for ns-LIBS analysis of test samples from different crops, only the use of multivariate partial least squares (PLS) regression appears capable for resolving the non-linear transformations of the emission intensities according to the physical mechanisms governing this temporal regime of ablation. Thus, when using multivariate modeling, the figures-of merit reflecting the predictive capabilities of ns-LIBS resemble to those achieved by fs-LIBS. Either way, fs-LIBS is a more robust approach that better offers larger flexibility to the matrix variability

Les plasmas froids d’air à pression atmosphérique sont très utiles pour un grand nombre d’applications grâce à leur chimie hors-équilibre et leur souplesse d’utilisation. Leur intérêt réside dans la production de certaines espèces réactives ou chargées avec un coût énergétique plus avantageux que la chimie à l’équilibre. L’objectif de cette thèse est de combiner les décharges nanosecondes répétitives pulsées (NRP) avec une géométrie micrométrique. Par cette combinaison, nous souhaitons palier au chauffage excessif des étincelles qui génèrent pourtant des fortes densités d’espèces. Notre étude se concentre en trois points principaux. Dans un premier temps la phase de claquage est étudiée ; c’est pendant cette étape que l’énergie est déposée et que les espèces sont produites. La combinaison des diagnostics électriques et de spectroscopie d’émission optique montrent que l’air est presque complètement dissocié et ionisé. Ensuite, nous nous intéressons à la phase de recombinaison qui conditionne la durée de vie de ces espèces. Les résultats mettent en évidence une réaction à trois corps comme mécanisme de recombinaison principal. Et enfin, le dernier point concerne le transport des espèces vers un substrat conducteur. En lui appliquant une tension, celui-ci nous permet de générer un écoulement de vent ionique provenant de la décharge. L’écoulement est étudié par vélocimétrie d’images de particules et imagerie Schlieren. Ce travail a permis de démontrer la capacité des NRP micro-plasmas dans la production contrôlée d’espèces réactives et chargées, mais aussi dans leur transport vers une surface par panache électro-aérodynamique. / Non-thermal plasmas generated in air at atmospheric pressure have numerous potential applications due to their non-equilibrium chemistry and ease of use. Their main advantages lie in the cost-efficient production of reactive and charged species compared to that of equilibrium chemistry. The aim of this thesis is to combine nanosecond repetitively pulsed discharges (NRP) with a microscale geometry. Using this combination, we seek to reduce the excessive heat release of NRP sparks, while nonetheless reaching high densities of reactive species and electrons. This work is comprised of three main parts. Our first goal is to study the breakdown phase, in which energy is deposited and charged species are produced. We employ both electrical characterization and optical emission spectroscopy in order to show that the NRP microplasma fully ionizes and dissociates the gas. The second part consists of the study of the recombination phase, in which the produced species recombine or survive. Results show that three-body recombination can explain the electron lifetime in this phase. Finally, we study the transport of plasma chemical species from the microplasma to a DC-biased conductive plate representing a substrate. By applying a voltage to this third electrode, we drive an electro-thermal plume via an ionic wind from the microplasma to the plate. This flow is investigated mainly by particle image velocimetry as well as Schlieren imaging. This work shows the capability of NRP microplasmas to produce high densities of reactive and charged species and transport them to a surface using an electrohydrodynamic plume.

<p> In the past two decades, great interest in weakly ionized plasmas sustained by high voltage nanosecond pulsed plasmas at high repetition rates has emerged. For such plasmas, the electron number density does not significantly decay between pulses, unlike the electron temperature. Such conditions are favorable to reconfigurable plasma antennas where the low electron temperature may enable the reduction of the Johnson–Nyquist thermal noise if an antenna is operated in the plasma afterglow. Moreover, it may be possible to sustain such conditions with RF pulses. Doing so could enable a plasma antenna that transmits the driving frequency when the pulse is applied and receives other frequencies with low thermal noise between pulses.</p> <p>To study nanosecond pulsed plasmas, experiments were performed in a parallel-plate electrode configuration in argon and nitrogen gas at a pressure of several Torr and repetition frequencies of 30-75 kHz. To measure the time-resolved electron number density in the afterglow of each pulse, a custom 58.1 GHz homodyne microwave interferometer was constructed. The voltage and current measurements were made using a back current shunt (BCS). Initial analysis of the measured electron density in both plasmas indicated that the electron thermalization was much faster than the electron decay. In the nitrogen plasma, dissociative recombination with cluster ions was the dominant electron loss mechanism. However, the dissociative recombination rates of the electrons in the argon plasma suggested the presence of molecular impurities, such as water vapor. Therefore, to better understand the recombination mechanisms in argon plasma with trace amounts (0.1% or less by volume) of water vapor under the experimental conditions, a 0-D kinetic model was developed and fit to the experimental data. The influence of trace amounts of water on the electron temperature and density decay was studied by solving electron energy and continuity equations. It was found that in pure argon, Ar⁺ ions dominate while the electrons are very slow to thermalize and recombine. Including trace amounts of water impurities drastically reduces the time for electrons to thermalize and increases their rate of recombination. </p> <p>In addition to large quasi-steady electron number densities and low electron temperature in the plasma afterglow, plasmas sustained by nanosecond pulses use a lower power budget than those sustained by RF or DC supplies. The efficiency of the power budget can be characterized by measuring the ionization cost per electron, defined as the ratio of the energy deposited in a pulse to the total number of electrons created. This was experimentally determined in air and argon plasmas at 2-10 Torr sustained by 1-7 kV nanosecond pulses at repetition frequencies of 0.1-30 kHz. The number of electrons were determined from the measured electron density through microwave interferometry and assuming a plasma volume equivalent to the volume between electrodes. The energy deposited was calculated from voltage and current measurements using both a BCS as well as high frequency resistive voltage divider and fast current transformer (FCT). It was found that the ionization cost in all conditions was within a factor of three of Stoletov’s point (the theoretical minimum ionization cost) and two orders of magnitude less than RF plasma.</p><p> </p><p>Having shown that it is possible to generate high electron density, low electron temperature plasmas with nanosecond pulses, it was necessary to now create a plasma antenna prototype. Initially, commercial fluorescent light bulbs were used and ignited using surface wave excitation at various RF frequencies and powers. The S₁₁ of the antenna response was measured by a VNA through a novel coupling circuit, while the deposited power was measured using a bi-directional coupler. Next, a custom plasma antenna was created in which the pressure and gas composition could be varied. In addition to the S₁₁ and deposited power, the antenna gain, and the electron number density were also measured for a pure argon plasma antenna at pressures of 0.3-1 Torr. Varying the applied power shifts the antenna resonance frequency while increasing the excitation frequency caused an increase in measured electron density for the same deposited power. Initial tests using direct electrode excitation of a twin-tube integrated compact fluorescent light bulb with nanosecond pulses have successfully been achieved. Future efforts include designing the proper circuitry to time-gate out the large pulse voltage to facilitate safe antenna measurements in the plasma afterglow.<br></p>

We demonstrate four experimentally simple methods for measuring very complex ultrashort light pulses. Although each method is comprised of only a few optical elements, they permit the measurement of extremely complex pulses with time-bandwidth products greater than 65,000. First, we demonstrate an extremely simple frequency-resolved-optical gating (GRENOUILLE) device for measuring the intensity and phase of pulses up to ~20ps in length. In order to achieve the required high spectral resolution and large temporal range, it uses a few-cm-thick second harmonic-generation crystal in the shape of a pentagon. This has the additional advantage of reducing the device's total number of components to three. Secondly, we introduce a variation of spectral interferometry (SI) using a virtually imaged phased array and grating spectrometer for measuring long complex ultrashort pulses up to 80 ps in length. Next, we introduce a SI technique for measuring the complete intensity and phase of relatively long and very complex ultrashort pulses. It involves making multiple measurements using SI (in its SEA TADPOLE variation) at numerous delays, measuring many temporal pulselets within the pulse, and concatenating the resulting pulselets. Its spectral resolution is the inverse delay range--many times higher than that of the spectrometer used. The waveforms were measured with ~ fs temporal resolution over a temporal range of ~ns and had time-bandwidth products exceeding 65,000, which to our knowledge is the largest time-bandwidth product ever measured with ~fs temporal resolution. Finally, we demonstrate a single-shot measurement technique that temporally interleaves hundreds of measurements with ~fs temporal resolution. It is another variation of SI for measuring the complete intensity and phase of relatively long and complex ultrashort pulses in a single shot. It uses a grating to introduce a transverse time delay into a reference pulse which gates the unknown pulse by interfering it at the image plane of an imaging spectrometer. It provided ~125 fs temporal resolution and a temporal range of 70 ps using a low-resolution spectrometer.

La fatigue du seuil d’endommagement laser dans la silice fondue a été largement étudiée au cours des dernières années, car ce phénomène est directement lié à la durée de vie des matériaux optiques utilisés dans des applications laser, le plus souvent à forte puissance. En effet, dans l’UV, on observe une décroissance du seuil d’endommagement laser quand le nombre de tirs laser augmente. Ce phénomène a été attribué pour ce couple longueur d’onde-matériau à des modifications laser-induites dans le matériau. Sous irradiation laser multiple à 266 nm, en utilisant des impulsions nanosecondes de densité d’énergie constante, nous avons observé que le signal de photoluminescence est modifié jusqu’à l’endommagement. A partir de cela, nous proposons une nouvelle représentation des données expérimentales qui permet de prédire l’apparition d’un endommagement dans le matériau. Cette prédiction réalisée à partir du signal de fluorescence et non de la statistique d’endommagement utilisée jusque-là, permet une économie significative de surface de composant et du temps d’expérience. Afin d’étendre l’intérêt de l’étude à un plus grand nombre d’applications, une extension des résultats à la longueur d’onde de 355 nm est proposée. Nous proposons un modèle où l’endommagement dans la silice fondue sous irradiation multiple à 266 nm est causé par une accumulation de modifications laser-induites induisant de l’autofocalisation non-linéaire. Afin d’essayer de généraliser la méthode de diagnostic de la fatigue par fluorescence, nous avons aussi réalisé des tests préliminaires sur des cristaux optiques non-linéaires bien connus comme le LBO ou le KDP. / Fatigue effects in fused silica have been largely studied in the past years, as this phenomenon is directly linked to the lifetime of high power photonic materials. Indeed, in the UV regime, we observe a decrease of the LIDT (Laser-Induced Damage Threshold) when the number of laser shots increases and this has been attributed for this couple wavelength/material to laser-induced material modifications. Under 266 nm laser irradiation, with nanosecond pulses of constant fluence, we observed that the photoluminescence is modified until damage occurs. Based on this observation, we propose a new representation of the experimental S-on-1 breakdown data which allows predicting the occurrence of material breakdown. This prediction, based on fluorescence signal and not damage statistics (presently widely used) allows consuming fewer sample surface and saving time. To extend the interest of the study to many more applications, we propose an extension of the results at 355 nm. We suppose that damage is caused in our fused silica samples by accumulation of laser-induced modifications under multiple-pulse UV irradiation inducing catastrophic non-linear self-focusing. In order to try to extend the fatigue diagnostic method by fluorescence, we have also realized preliminary tests in well-known non-linear crystals like LBO and KDP.

A influência das variáveis associadas ao laser como a fluência, o comprimento de onda, e a duração do pulso, assim como as relacionadas às propriedades das amostras, como a distribuição do tamanho das partículas e as características químicas da matriz, foram avaliadas visando à determinação quantitativa de macro- (P, K, Ca, Mg) e micronutrientes (Cu, Fe, Mn, Zn, B) em pastilhas de materiais vegetais por espectrometria de emissão óptica com plasma induzido por laser (LIBS). Os efeitos da distribuição do tamanho das partículas e da fluência do laser foram investigados a partir da análise de amostras peneiradas (150-20 µm) empregando-se um sistema LIBS, em regime temporal de nanossegundos (ns-LIBS), montado com um laser de Nd:YAG a 1064 nm (pulsos de 5 ns e 360 mJ)e um espectrômetro com óptica Echelle e detector ICCD. Observou-se um aumento na sensibilidade e na precisão das medições com a diminuição do tamanho das partículas usadas no preparo das pastilhas, e uma diminuição dos efeitos de matriz causados por diferenças no tamanho das partículas, quando pastilhas preparadas com partículas < 75 µm foram analisadas com pulsos de 50 J cm-2. Verificou-se uma melhora significativa na exatidão das medições de Mg, Fe, Mn e Zn feitas em um conjunto de pastilhas de folhas de cana-de-açúcar (partículas < 75 µm) empregando-se esta fluência. Em uma segunda etapa, observou-se que variações no comprimento de onda do laser de Nd:YAG (1064, 532, 355 e 266 nm) não influenciaram de maneira significativa a precisão e exatidão das medições em pastilhas de folhas de cana-de-açúcar, obtendo-se correlações lineares entre as intensidades dos sinais de emissão e as correspondentes frações de massa dos analitos. Variações no comprimento de onda do laser de Nd:YAG não afetaram a análise de um conjunto heterogêneo de amostras, composto por pastilhas de folhas de plantas de diferentes espécies, como soja, cana-de-açúcar, milho, citros, café, por exemplo, por ns-LIBS. No entanto, diferentemente do observado para o conjunto de pastilhas de folhas de cana-de-açúcar, observou-se, uma baixa correlação (r cal < 0,90) entre as frações de massa de Ca, Mg, P, Cu, Fe, Mn e Zn determinadas por ns-LIBS e os valores de referência, o que demonstra a baixa robustez de ns-LIBS frente às variações na composição química das matrizes. Posteriormente, analisou-se este conjunto heterogêneo de amostras com sistema LIBS, em regime temporal de femtossegundos (fs-LIBS), montado com laser de Ti:Safira (pulsos de 60 fs e 1,65 mJ) e espectrômetro com óptica Czerny-Turner e ICCD. Demonstrou-se que o uso de pulsos em regime de fs proporcionou calibrações e validação menos dependentes da composição química das matrizes. As frações de massa de Ca, Mg, P, Fe e Mn previstas por fs-LIBS foram estatisticamente concordantes com os valores de referência, independentemente do modelo de calibração usado. Além disso, o uso de calibração multivariada melhorou a capacidade preditiva de ns-LIBS, assemelhando-se à de fs-LIBS. Concluiu-se que o emprego de fs-LIBS foi a estratégia mais robusta e que ofereceu maior flexibilidade à variabilidade matricial / The influence of laser properties, such as fluence, wavelength and pulse duration, as well as sample characteristics, such as particle size distribution and chemical matrix composition, was evaluated aiming at the quantitative determination of macro- (P, K, Ca, Mg) and micronutrients (Cu, Fe, Mn, Zn, B) in pellets of plant materials by laser-induced breakdown spectroscopy (LIBS). Firstly, the effects of particle size distribution and laser fluence on the analysis of pellets (test samples) prepared with sieved samples (from 150 to 20 µm apertures) were investigated. Experiments were carried out with a nanosecond LIBS (ns-LIBS) system by using a Q-switched Nd:YAG laser at 1064 nm (5 ns; 360 mJ) and a spectrometer with Echelle optics and intensified charge-coupled device (ICCD) detector. Results indicated that smaller particles yielded to sensitivities\' enhancement and attained better measurements\' precision. Moreover, matrix effects were reduced by analyzing pellets prepared from < 75 ?m sieved fractions and pulses of 50 J cm-2. In addition, there was a significant improvement on accuracy of Mg, Fe, Mn and Zn measurements in a set of test samples of sugarcane leaves by using this fluence. In a second experiment, variations in the Nd:YAG laser wavelength (1064, 532, 355 and 266 nm) did not affect the analysis of test samples of sugarcane leaves, and provided linear correlations between emission signal intensities and corresponding analytes mass fractions. In addition, variations within Nd:YAG laser wavelength did not affect the analysis of a heterogeneous sample set composed by pellets of leaves from different crops, such as soy, sugarcane, maize, citrus and coffee by ns-LIBS. However, in contrast to previous findings, the univariate calibration models for ns-LIBS presented lower linearity (r cal < 0.90) for Ca, Mg, P, Cu, Fe, Mn and Zn, no matter the laser wavelength used for the analysis. These circumstances reflect the low robustness of ns-LIBS to variations within matrix chemical composition among test samples. Afterwards, test samples from different crops were analyzed by a femtosecond LIBS (fs-LIBS) by using a Ti:Sapphire laser, including a mode-locked oscillator and an ultrafast amplifier (60 fs; 1.65 mJ per pulse), and a spectrometer with Czerny-Turner optics and ICCD. Findings indicated that the pulse duration was a decisive variable for providing accurate quantification of nutrients in different plant species, which present substantial differences in terms of matrix chemical composition. Close agreement between Ca, Mg, P, Fe and Mn mass fractions predicted by fs-LIBS and those determined by ICP OES was evidenced, whatever the modeling approach used. Contrarily, for ns-LIBS analysis of test samples from different crops, only the use of multivariate partial least squares (PLS) regression appears capable for resolving the non-linear transformations of the emission intensities according to the physical mechanisms governing this temporal regime of ablation. Thus, when using multivariate modeling, the figures-of merit reflecting the predictive capabilities of ns-LIBS resemble to those achieved by fs-LIBS. Either way, fs-LIBS is a more robust approach that better offers larger flexibility to the matrix variability

Les impulsions de champ électrique nanoseconde de forte intensité (nsPEF) ont été proposées pour le traitement du cancer avec des effets secondaires minimes et peu susceptibles de conduire à une résistance de la tumeur au traitement. Le glioblastome multiforme (GBM) est un cancer du cerveau incurable montrant une résistance aux traitements actuels tels que la chirurgie, la radiothérapie et la chimiothérapie. Dans cette thèse, l'imagerie des cellules vivantes est utilisée pour étudier in vitro les effets de nsPEF sur une lignée de cellules de glioblastome humain (U87-MG), et pour évaluer la pertinence de l'utilisation des nsPEF en tant que nouveau traitement pour le GBM. En accord avec les résultats publiés précédemment, nous montrons que les cellules U87-MG répondent aux nsPEF avec une poration de la membrane plasmique, une augmentation rapide du calcium intracellulaire et une perte progressive du potentiel de membrane mitochondriale. De nouveaux résultats montrent que 100 impulsions de 10 ns délivrées à 44 kV/cm perturbent la dynamique de croissance des microtubules indépendamment du calcium et du gonflement, ces derniers étant connus pour provoquer la dépolymérisation des microtubules. La microscopie à super-résolution nous a permis de visualiser les flexions et ruptures de microtubules après l'application nsPEF suggérant un effet plus direct des impulsions. L'étude des nsPEF sur le calcium a également été menée via des indicateurs de calcium génétiquement encodés (GECIs) qui permettent une comparaison entre les GECIs et les indicateurs chimiques couramment utilisés. En utilisant le GECI GCaMP, le potentiel d'expression des GECIs dans des endroits subcellulaires spécifiques a permis de mettre en évidence une onde de calcium induite par l'application des nsPEF, grâce à une forme de GCaMP fixée à la membrane plasmatique. Ce phénomène, qui n'est pas habituel avec des indicateurs chimiques cytosoliques classiques en raison de la diffusion, permet de confirmer l'origine extracellulaire des pics de calcium post nsPEF. Cette thèse démontre que les nsPEF appliqués à des cellules U87-MG induisent plusieurs effets cellulaires majeurs et potentiellement destructeurs. La perturbation du réseau de microtubules par les nsPEF pourrait éventuellement être exploitée comme un antimitotique, administré localement, pour le traitement de GBM, avec des effets secondaires systémiques réduits et une faible résistance au traitement. / High powered, nanosecond duration pulsed electric fields (nsPEF) have been proposed as a minimal side-effect, electrical cancer therapy that is unlikely to result in tumour resistance. Glioblastoma multiforme (GBM) is an incurable brain cancer showing resistance to current treatments such as surgery, radiotherapy and chemotherapy. This thesis uses live-cell imaging to look in vitro at the effects of nsPEF on a human glioblastoma cell line (U87-MG) in a first step towards assessing its suitability as a novel treatment for GBM. In agreement with previously published results we show that U87-MG cells respond to nsPEF with plasma membrane poration, a rapid increase in intracellular calcium and a gradual loss of mitochondrial membrane potential. We present novel results showing that 100, 10 ns pulses delivered at 44 kV/cm disrupt microtubule growth dynamics in a way that is independent of calcium and swelling, both of which are known to cause microtubule depolymerisation. Super-resolution microscopy allowed us to visualise microtubules bending and breaking following nsPEF application suggesting a more direct effect of the pulse. We look also at the application of genetically encoded calcium indicators (GECIs) to nsPEF calcium studies making a comparison between GECIs and commonly used chemical indicators. Using the GECI GCaMP, we show the advantages of being able to express GECIs in specific subcellular locations by visualising an nsPEF induced calcium wave with a plasma membrane bound form of GCaMP. This event, which is not evident with classic cytosolic chemical indicators due to diffusion, helps confirm the extracellular origin of the post-nsPEF calcium spike. The work in this thesis demonstrates that nsPEF causes several major, and possibly destructive, cellular events when applied to U87-MG cells. The disruption of the microtubule network by nsPEF could potentially be exploited as a locally administered antimitotic, for GBM treatment, with reduced systemic side effects and lower occurrences of resistance.