The rotational spectrum of ScO (X-2 Sigma(+)) has been measured in the gas phase in the frequency range 30-493 GHz using a combination of Fourier transform microwave/millimeter-wave (FTM/mmW) and submillimeter direct absorption methods. This work is the first pure rotational study of this radical. Both the ground vibrational and v=1 states were observed. ScO was created from the reaction of metal vapor, produced either by a laser ablation source or a Broida-type oven, and N2O, in the former case heavily diluted in argon. Extensive hyperfine structure was observed in the FTM/mmW data, although the spin-rotation splitting was found to be small (similar to 3 MHz). In the mm-wave spectra, however, the fine and hyperfine structure was blended together, resulting in broad, single lines for a given transition N + 1 <- N. The data were analyzed in a combined fit using the very accurate hyperfine measurements of Childs and Steimle (1988), employing a Hund's case b Hamiltonian, and an improved set of rotational and centrifugal distortion constants were determined. These measurements improve the accuracy of predicted frequencies for astronomical searches by 14-18 MHz, or 16-20 km/s, in the 1 mm region - a difference of half to a full linewidth for certain interstellar sources. This work also demonstrates the capabilities of the FTM/mmW spectrometer at 61 GHz.

Mémoire numérisé par la Division de la gestion de documents et des archives de l'Université de Montréal.

Après des décennies de développement, l'ablation laser est devenue une technique importante pour un grand nombre d'applications telles que le dépôt de couches minces, la synthèse de nanoparticules, le micro-usinage, l’analyse chimique, etc. Des études expérimentales ainsi que théoriques ont été menées pour comprendre les mécanismes physiques fondamentaux mis en jeu pendant l'ablation et pour déterminer l’effet de la longueur d'onde, de la durée d'impulsion, de la nature de gaz ambiant et du matériau de la cible. La présente thèse décrit et examine l'importance relative des mécanismes physiques qui influencent les caractéristiques des plasmas d’aluminium induits par laser. Le cadre général de cette recherche forme une étude approfondie de l'interaction entre la dynamique de la plume-plasma et l’atmosphère gazeuse dans laquelle elle se développe. Ceci a été réalisé par imagerie résolue temporellement et spatialement de la plume du plasma en termes d'intensité spectrale, de densité électronique et de température d'excitation dans différentes atmosphères de gaz inertes tel que l’Ar et l’He et réactifs tel que le N2 et ce à des pressions s’étendant de 10‾7 Torr (vide) jusqu’à 760 Torr (pression atmosphérique). Nos résultats montrent que l'intensité d'émission de plasma dépend généralement de la nature de gaz et qu’elle est fortement affectée par sa pression. En outre, pour un délai temporel donné par rapport à l'impulsion laser, la densité électronique ainsi que la température augmentent avec la pression de gaz, ce qui peut être attribué au confinement inertiel du plasma. De plus, on observe que la densité électronique est maximale à proximité de la surface de la cible où le laser est focalisé et qu’elle diminue en s’éloignant (axialement et radialement) de cette position. Malgré la variation axiale importante de la température le long du plasma, on trouve que sa variation radiale est négligeable. La densité électronique et la température ont été trouvées maximales lorsque le gaz est de l’argon et minimales pour l’hélium, tandis que les valeurs sont intermédiaires dans le cas de l’azote. Ceci tient surtout aux propriétés physiques et chimiques du gaz telles que la masse des espèces, leur énergie d'excitation et d'ionisation, la conductivité thermique et la réactivité chimique. L'expansion de la plume du plasma a été étudiée par imagerie résolue spatio-temporellement. Les résultats montrent que la nature de gaz n’affecte pas la dynamique de la plume pour des pressions inférieures à 20 Torr et pour un délai temporel inférieur à 200 ns. Cependant, pour des pressions supérieures à 20 Torr, l'effet de la nature du gaz devient important et la plume la plus courte est obtenue lorsque la masse des espèces du gaz est élevée et lorsque sa conductivité thermique est relativement faible. Ces résultats sont confirmés par la mesure de temps de vol de l’ion Al+ émettant à 281,6 nm. D’autre part, on trouve que la vitesse de propagation des ions d’aluminium est bien définie juste après l’ablation et près de la surface de la cible. Toutefois, pour un délai temporel important, les ions, en traversant la plume, se thermalisent grâce aux collisions avec les espèces du plasma et du gaz. / After decades of development, laser ablation has become an important technique for a large number of applications such as thin film deposition, nanoparticle synthesis, micromachining, chemical analysis, etc. Experimental and theoretical studies have been conducted to understand the physical mechanisms of the laser ablation processes and their dependence on the laser wavelength, pulse duration, ambient gas and target material. The present dissertation describes and investigates the relative importance of the physical mechanisms influencing the characteristics of aluminum laser-induced plasmas. The general scope of this research encompasses a thorough study of the interplay between the plasma plume dynamics and the ambient gas in which they expand. This is achieved by imaging and analyzing the temporal and spatial evolution the plume in terms of spectral intensity, electron density and excitation temperature within various environments extending from vacuum (10‾7 Torr) to atmospheric pressure (760 Torr), in an inert gas like Ar and He, as well as in a chemically active gas like N2. Our results show that the plasma emission intensity generally differs with the nature of the ambient gas and it is strongly affected by its pressure. In addition, for a given time delay after the laser pulse, both electron density and plasma temperature increase with the ambient gas pressure, which is attributed to plasma confinement. Moreover, the highest electron density is observed close to the target surface, where the laser is focused and it decreases by moving away (radially and axially) from this position. In contrast with the significant axial variation of plasma temperature, there is no large variation in the radial direction. Furthermore, argon was found to produce the highest plasma density and temperature, and helium the lowest, while nitrogen yields intermediate values. This is mainly due to their physical and chemical properties such as the mass, the excitation and ionization levels, the thermal conductivity and the chemical reactivity. The expansion of the plasma plume is studied by time- and space-resolved imaging. The results show that the ambient gas does not appreciably affect plume dynamics as long as the gas pressure remains below 20 Torr and the time delay below 200 ns. However, for pressures higher than 20 Torr, the effect of the ambient gas becomes important and the shorter plasma plume length corresponds to the highest gas mass species and the lowest thermal conductivity. These results are confirmed by Time-Of-Flight (TOF) measurements of Al+ line emitted at 281.6 nm. Moreover, the velocity of aluminum ions is well defined at the earliest time and close to the target surface. However, at later times, the ions travel through the plume and become thermalized through collisions with plasma species and with surrounding ambient gas.

15 samples of gem opals were analyzed by laser ablation inductively coupled plasma mass spectrometry (LA ICP-MS) and inductively coupled plasma mass spectrometry (ICP-MS). For this study were selected the most representative samples from Slovakia, Australia, Peru, Ethiopia, Mexico, USA and the Czech Republic. These samples were obtained from private collections. The study focuses on the geochemical relationships between various forms of opal originating from igneous and sedimentary environments based on the results from LA ICP-MS and ICP-MS. The major and trace element compositions are unique for each studied opal locality and important for understanding numerous aspects of opal formation. Major element analysis shows that opals are essentially pure SiO2 (77 - 92 wt. %). Al, Fe, Ca, K, Na and Mg are the main elemental impurities. The concentrations of the trace elements vary strongly depending on the opal locality. Differences were found, e.g., in the concentrations of REE and some refractory elements, which might be indicative for determining the provenance of opals. Many studies have been published explaining the origin of luminescence, microstructures and the thermal properties of opals. However, there are very few comprehensive studies comparing gem opals from the most important historical and...

ABSTRACT The focus of this work was the study possible ways to improve the efficiency of solar cells. To this end, the main aim was to investigate the deposition process of Indium Tin Oxide (ITO), Titanium Dioxide (TiO2), multi-layers ITO/TiO2 on quartz SiO2 substrates under different conditions (oxygen pressure, laser fluence and wavelength, and temperature) and later gold nanoparticles by the Reactive Pulsed Laser Ablation Deposition (RPLAD) technique. It was intended to investigate their electrical structural and optical properties under selected conditions for possible application to Dye Sensitised Solar Cells (DSSC). Under optimised conditions, maximum deposition rates of 12nm/min for ITO and 21nm/min for TiO2 thin films were achieved. Rutherford Backscattering Spectrometry (RBS) with 2MeV He+ ions was used to measure the films thickness. Uniform thicknesses over a large area were found to be about 400nm and 800nm for ITO and TiO2 films, respectively. Crystalline properties were studied via x-ray diffraction and Raman spectroscopy. X-ray Diffraction (XRD) analysis revealed that the ITO films are highly orientated nanocrystals with their a-axis normal to the glass substrate surface. The average particle size of the precipitated nanocrystals was calculated to be 10-15nm. The structure of the films was characterised via Atomic Force Microscopy (AFM) imaging of the top surface of the film. The films have a rough surface with average roughness of 26-30nm. Pores were observed with a density of 144 and 125 pores/mm2 and average size of 150 and 110nm for ITO films deposited at 200 and 400°C, respectively. TiO2 films deposited on the prepared ITO films were less crystalline. Annealing was performed at 300 and 500°C for 3 consecutive hours and the XRD results show that the transformation of TiO2 film into anatase phase was almost complete with a crystal size of ~ 6-7nm. Scanning Transmission Electron Microscopy (STEM) of the surfaces was also performed. The TiO2 films deposited onto the prepared ITO films present a relatively high pore size with an average pore diameter of ~ 40nm and excellent uniformity. It is interesting to note that the pores are randomly arranged. The random arrangement of the pores network may actually be beneficial for producing a uniform electrode. In addition, STEM cross-sectional analysis of the films showed a columnar structure but no evidence of voids in the structure. The large surface area produced suggests applications in DSSC. The electrical properties of the films were investigated and an estimation of resistivity and Hall mobility was made. Low values of resistivity and high values of mobility were observed for ITO films. The resistivity of the film increases with increasing thickness while it decreases when increasing the deposition temperature. The lowest value was found to be 1.5x10-6Ωm for ITO films deposited at 400°C. Hall mobility was found to increase with substrate temperature. In this investigation, the highest Hall mobility at room temperature was estimated to be 22.3cm2/Vs under ambient O2 pressure (PO2) of 1Pa and 52.1 and 51.3cm2/Vs for films deposited at 200 and 400°C, respectively. But the best ITO film was deposited at 200°C, since this film combines good resistivity, good Hall mobility and good transmittance. UV-VIS-IR transmission spectra were recorded on a Perkin Elmer Lambda 900. From the transmission data, the energy gap as well as the optical constant was estimated. A high transmission for ITO films in the visible (Vis) range was observed which was above 88% for films produced at room temperature and above 95% for those deposited at 200°C. The transmission for the films produced in oxygen was about 90% above 400nm, whereas it lies between 70 and 80% for films produced in rare gases. An increase in the band gap was observed by increasing the oxygen pressure and substrate temperature for ITO films. Increasing the quartz SiO2 substrate temperature from room temperature to 400 °C resulted in an increase of the transmission of TiO2 films, mostly in the Visible Near Infrared (Vis-NIR) from about 70% to 92%. After annealing at 500°C for 3 consecutive hours, the transmission of TiO2 film further sharply decreases toward shorter wavelengths. Analysis of the transmittance curve of TiO2/Au shows a decrease of about 6% of the transmission in the Ultraviolet Visible (UV-Vis) range. Optical absorption edge analysis showed that the optical density could be used to detect the film growth conditions and to correlate the film structure and the absorption edge. The TiO2 films deposited present a direct band gap at 3.51eV and 3.37eV for TiO2 as deposited and after annealing, respectively, while the indirect band gap was found to be 3.55eV and 3.26eV for TiO2 films as deposited and after annealing, respectively. There was a shift of about 0.1eV between as deposited ITO monolayer films and ITO/TiO2 bilayers deposited at 200°C. A small shift towards shorter wavelengths has been observed for multilayer ITO/TiO2/Au. In this case, the increase of Eg was ascribed to a reduction of the oxygen vacancies with increasing substrate temperature at which the ITO film was deposited. The change in the shape of the fundamental absorption edge is considered to reflect the variation of density and the short range structural modifications undetected by structural characterisations. Enlargement of band-gap energies of semiconductors may be advantageous when used in DSSC to suppress the charge recombination between the reduced electrolytes and the photo-excited holes in the valence band of TiO2 substrates and enhance the open-circuit potential of the cell. When ITO/TiO2 bilayers were annealed before depositing Au, the gap energy remained constant.

The primary aim of this thesis is to develop image processing algorithms to quantitatively determine the link between traumatic brain injury (TBI) severity and chronic traumatic encephalopathy (CTE) neuropathology, specifically looking into the role of blood-brain barrier disruption following TBI. In order to causally investigate the relationship between the tau protein neurodegenerative disease CTE and TBI, mouse models of blast neurotrauma (BNT) and impact neurotrauma (INT) are investigated. First, a high-speed video tracking algorithm is developed based on K-means clustering, active contours and Kalman filtering to comparatively study the head kinematics in blast and impact experiments. Then, to compare BNT and INT neuropathology, methods for quantitative analysis of macroscopic optical images and fluorescent images are described. The secondary aim of this thesis focuses on developing methods for a novel application of metallomic imaging mass spectrometry (MIMS) to biological tissue. Unlike traditional modalities used to assess neuropathology, that suffer from limited sensitivity and analytical capacity, MIMS uses a mass spectrometer -- an analytical instrument for measuring elements and isotopes with high dynamic range, sensitivity and specificity -- as the imaging sensor to generate spatial maps with spectral (vector-valued) data per pixel. Given the vector nature of MIMS data, a unique end-to-end processing pipeline is designed to support data acquisition, visualization and interpretation. A novel multi-modal and multi-channel image registration (MMMCIR) method using multi-variate mutual information as a similarity metric is developed in order to establish correspondence between two images of arbitrary modality. The MMMCIR method is then used to automatically segment MIMS images of the mouse brain and systematically evaluate the levels of relevant elements and isotopes after experimental closed-head impact injury on the impact side (ipsilateral) and opposing side (contralateral) of the brain. This method quantifiably confirms observed differences in gadolinium levels for a cohort of images. Finally, MIMS images of human lacrimal sac biopsy samples are used for preliminary clinicopathological assessments, supporting the utility of the unique insights MIMS provides by correlating areas of inflammation to areas of elevated toxic metals. The image processing methods developed in this work demonstrate the significant capabilities of MIMS and its role in enhancing our understanding of the underlying pathological mechanisms of TBI and other medical conditions. / 2019-07-09T00:00:00Z

Introdução: Na última década, desde a descrição inicial da ablação das veias pulmonares, a ablação por cateter da fibrilação atrial (FA) tem evoluído consideravelmente em eficácia e segurança, consolidando-se como opção terapêutica em pacientes selecionados com FA. No entanto, a ablação da FA é um procedimento complexo e não isento de riscos. Ainda que seja uma complicação rara, o desenvolvimento de fístulas átrio-esofágicas (FAE) é a segunda complicação responsável por morte relacionada ao procedimento e responde por 16% dos casos de morte após ablação de FA. Consensos atuais não orientam recomendações definitivas para prevenção de lesões esofágicas, consideradas lesões precursoras de FAE. O objetivo deste trabalho foi comparar a incidência de lesões esofageanas e periesofageanas por ecoendoscopia após ablação de fibrilação atrial, utilizando diferentes estratégias de proteção esofágica durante as aplicações de radiofrequência na parede posterior do átrio esquerdo. Método: No período de outubro/2012 a julho/2014, foram estudados 45 pacientes submetidos à ablação percutânea de FA, portadores de FA paroxística ou persistente há menos de um ano. Todos os pacientes foram submetidos a ablação circunferencial com isolamento elétrico das veias pulmonares, com cateter de ablação 8 mm. Antes do procedimento, os pacientes foram randomizados para uma de três estratégias de proteção esofágica durante as aplicações de radiofrequência na parede posterior do átrio esquerdo para ablação da FA: Grupo I - aplicações limite fixo e de baixa energia, 30 W; Grupo II - aplicações com energia limitada pela temperatura esofágica; GIII - aplicações com limite fixo de energia durante resfriamento esofágico contínuo. A pesquisa de lesões esofágicas/periesofágicas foi feita por ecoendoscopia realizada em até 48 horas após a ablação. Resultados: As características basais foram similares nos três grupos, não sendo encontradas diferenças significativas entre as variáveis clínicas, laboratoriais, ecocardiográficas ou ecoendoscópicas prévias, com exceção da distância átrio-esofágica pré-ablação medida pela ecoendoscopia, que foi menor no Grupo III (GI = 3,9 mm +- 0,4; GII = 3,9 mm +- 0,5; GIII = 3,4 mm +- 0,4, p = 0.002). Nas ecoendoscopias pós-ablação de FA, foram encontradas 04 lesões esofágicas/periesofágicas: duas úlceras de parede esofágica e dois casos de edemas de mediastino periesofágico. Todos os casos de lesões esofágicas/periesofágicas ocorreram no grupo de resfriamento esofágico, G III (p= 0,008). A comparação das características clínicas dos pacientes que apresentaram lesões esofágicas/periesofágicas com os que não apresentaram essas alterações, pela análise bivariada, mostrou que foram similares nos dois grupos, exceto pelos valores médios de proteína C reativa (PCR) após a ablação de fibrilação atrial, que foram significativamente maiores no grupo com lesões (Grupo sem lesões: PCR = 0,82 mg/dl; Grupo com lesões: PCR = 2,12 mg/dl, p < 0,001). A comparação dos parâmetros das ablações por regiões das veias abordadas, quanto ao tempo das aplicações de radiofrequência, a potência e a temperatura do cateter de ablação, identificou que os pacientes que apresentaram lesões esofágicas/periesofágicas tiveram maiores valores de média de potência nas aplicações realizadas na parede posterior das veias pulmonares esquerdas, que os pacientes que não tiveram lesões (Grupo sem lesões esofágicas: potência média cateter = 37,7 w; Grupo com lesões esofágicas: potência média do cateter = 48,8 w, p = 0.013). A incidência de recorrência de arritmia após um único procedimento de ablação de Fibrilação Atrial, em seguimento clínico de 11 +- 5 meses, foi de 7 casos (15.6%), sem diferença significativa entre os grupos (GI = 26,7%, GII = 13,3% e GIII = 6,7%, p = 0,305). A incidência de complicações maiores relacionadas aos procedimentos de ablação realizados foi de 2,2% (um caso de congestão pulmonar no segundo dia após o procedimento, resolvido com uso de diuréticos). Conclusão: O uso da estratégia de resfriamento esofágico durante ablação de FA foi ineficaz como estratégia preventiva de lesões esofágicas/periesofágicas na população estudada, quando comparada às estratégias de aplicações de radiofrequência com baixa energia ou de energia limitada pela temperatura esofágica / Introduction: In the last decade, since the initial description of the ablation of pulmonary veins, the atrial fibrillation (AF) catheter ablation has evolved significantly in terms of efficacy and safety, consolidating itself as the therapeutic choice for AF selected patients. However, AF ablation is a complex procedure not without risks. Despite being a rare complication, the development of atrialesophageal fistulas (AEFs) ranks second in terms of procedure-related deaths, accounting for 16% of all post-AF ablation losses of life. Current consensus is not dispositive with regards to directives for the prevention of esophageal lesions, which come first and lead to AEFs. The objective of this work is to compare the incidence of esophageal and periesophageal lesions post-AF ablation, given use of different esophageal protection strategies during the radiofrequency applications on the left-atrium posterior wall. Method: From October 2012 through July 2014, 45 patients submitted to AF percutaneous ablation were studied. All of them were bearers of paroxistic or persistent AF for less than one year, and all of them were submitted to 8mm-catheter, pulmonary vein electric-shielding circumferential ablation. Before the procedure, patients were randomly assigned to one of three esophageal lesion protection strategies: Group I - 30w, low energy, fixed limited applications; Group II - energy applications limited by esophageal temperature; and Group III - fixed limit energy applications during continuous esophageal cooling. The survey for esophageal/periesophageal lesions was carried by means of esophageal endoscopy combined with radial ultrasound performed within 48 hours post ablation. Results: Baseline characteristics were even across groups; no significant differences in clinical, laboratorial, ecocardiographic or endoscopic variables were found, except for pre-ablation distance between posterior left atrium wall and the esophagus as measured by radial ultrasound endoscopic, smaller in Group III (GI = 3,9 mm +- 0,4; GII = 3,9 mm +- 0,5; GIII = 3,4 mm +- 0,4, p = 0.002). Post FA-ablation endoscopies revealed the existence of 4 counts of esophageal/periesophageal lesions: 2 esophageal wall ulcer and 2 periesophageal mediastin edema. All cases of esophageal/periesophageal lesions occurred in the esophageal cooling group (GIII) (p=0.008). Bivariate analysis on the clinical characteristics of patients that presented esophageal/periesophageal lesions showed no significant difference from those in the lesion-free group, except for average values for post ablation reactive-C protein (RCP), significantly greater in the lesion group (2.12 mg/dl vs. 0.82 mg/dl for the lesion-free group, p < 0.001). Ablation parameter comparison by approached vein region revealed that patients with post ablation lesions had received higher-powered applications in their posterior wall left pulmonary veins (average catheter power = 48.8 w vs. 37.7 w for lesion-free group, p=0.013). After a 11 +- 5 month clinical following, arrhythmia recurrence post a single AF ablation procedure added to 7 cases (15.6%), and no significant difference among the three different groups was found (GI = 26.7%, GII = 13.3% e GIII = 6.7%, p = 0.305). Incidence of major complications related to the ablation procedures reached 2.2% (one case of pulmonary congestion occurring in the second day post procedure, and resolved with the use of diuretics). Conclusion: The use of esophageal cooling during AF ablation was an ineffective strategy to prevent esophageal/periesophageal lesions in the studied population when compared to low-energy radiofrequency or energy limited by esophageal temperature lesion prevention strategies

Este trabalho descreve o desenvolvimento de um processo de fabricação de mini e microdispositivos fluídicos baseado na utilização de um equipamento de usinagem a laser de CO2 para criação de relevos sobre base de poli(metacrilato de metila) e na selagem térmica contra igual material. Inicialmente, o equipamento laser foi detalhadamente caracterizado, o que possibilitou elaborar métodos para a construção de microcanais de forma mais eficiente e com menores chances de defeitos. Tipicamente, os canais apresentaram seção transversal triangular em torno de 200 &#181;m de largura e 100 &#181;m de profundidade, sendo possível, no entanto, criar canais com outras características. A etapa de selagem entre a tampa e a base que apresentou melhores resultados consiste em pressurização acima de 6 kgf·cm-2 e aquecimento a 110 ºC durante 45 minutos, seguido de resfriamento por 1 h. Os microcanais selados por esta técnica, resistiram a pressões superiores a 3,5·kgf·cm-2. O processo desenvolvido se mostrou adequado para a criação de protótipos, sendo também suas principais características: (1) a facilidade de incorporação de regiões de grandes dimensões (como reservatórios) em conjunto com os microcanais, (2) número reduzido de etapas de produção e (3) boa uniformidade química da parede interna dos canais, o que é particularmente interessante para microdispositivos aplicados à Química Analítica / A microfabrication process based machining using CO2 laser on poly(methyl methacrylate) and thermal sealing is described. Initially, the laser equipment was characterized in detail, which allowed developing strategies for the construction of microchannels more efficiently and less failure-prone. Typically, the channels had a triangular cross section around 200 &#181;m in width and 100 &#181;m in depth. It is possible, however, create channels with other features. The sealing step that showed better results consists in to pressurize at 6 kgf·cm-2 and heating at 110 °C during 45 minutes, followed by natural cooling for 1 h. The microchannels sealed by using this procedure resisted pressures above 3.5 kgf·cm-2. The process proved to be adequate for prototyping and also has other main features: (1) easiness of incorporation of large regions (such as reservoirs) together with the microchannel; (2) reduced number of manufacturing steps and (3) good chemical uniformity of the inner wall of the channel, which is particularly interesting for microdevices applied to Analytical Chemistry.

O desenvolvimento de sistemas laser com pulsos ultracurtos trouxe a possibilidade de usinagem de estruturas muito pequenas em praticamente qualquer tipo de material. Neste trabalho foi dada continuidade a estudos já iniciados no Centro de Lasers e Aplicações (CLA) com os materiais dielétricos, introduzindo a largura temporal dos pulsos laser como mais uma variável e utilizando os conhecimentos adquiridos para a determinação de limiares de ablação e parâmetros de incubação em alguns metais como: aço AISI 1045, aço inoxidável VI138, cobre eletrolítico e molibdênio. A ausência de calor no processo de ablação dos metais torna-se muito difícil, pois a criação de uma camada de íons é muito prejudicada pela mobilidade eletrônica ao seu redor. Assim a ablação de metais com pulsos ultracurtos, tem como principal mecanismo a explosão de fase associada a outros processos que também contribuem na ablação, porém em menor escala, como a explosão coulombiana e a fusão ultrarrápida. Além disso, propriedades como a constante de acoplamento elétron-fônon e a condutividade térmica assumem um papel importante e devem ser levadas em conta na investigação do processo de ablação dos metais. Este trabalho possibilitou a obtenção de parâmetros de operação nos quais o calor transferido para a rede é minimizado, possibilitando a microusinagem de precisão e alterações controladas na morfologia da superfície de diversos metais. Os resultados propiciaram assim condições para novos desenvolvimentos e aplicações práticas de usinagem com pulsos ultracurtos. / The development of laser systems with ultrashort pulses brought the possibility of machining very small structures in virtually any type of material. In this work was continued the studies already started in Lasers and Applications Center (CLA), with dielectric materials, introducing temporal width of the laser pulses as another variable, and using the knowledge acquired to determine ablation threshold and incubation parameters of some metals such as AISI 1045 steel, VI 138 stainless steel, electrolytic copper and molybdenum. The absence of heat in the ablation process of metals is much more difficult since the creation of a layer of ions is greatly impaired by electronic mobility in its vicinity. Hence, the ablation process for metals with ultrashort pulses, has, as main mechanism, the phase explosion associated with other processes that also contribute in the process, but on a smaller scale, such as Coulomb explosion and ultrafast fusion. Moreover, properties such as electron-phonon coupling constant and thermal conductivity play an important role and should be taken into account in investigating the process of ablation of metals. This study made it possible to obtain operation parameter where the heat transferred to the lattice is minimized, enabling precision micromachining and controlled changes in the morphology of the surface of metals. The results provided conditions for new developments and real machining applications with ultrashort pulses.

A Gerência de Rejeitos Radioativos do IPEN já se utiliza da técnica de ablação por laser para descontaminação de peças superficialmente contaminadas por material radioativo. Esta tecnologia, porém, demonstrou grande potencial para caracterização destes rejeitos com o objetivo de levantar o Inventário Radioisotópico de peças. As técnicas atuais para levantar este inventário (esfregaço e modelagem físico-matemática) sofrem de grandes limitações de implementação e de precisão. O objetivo deste trabalho é desenvolver o projeto de uma sonda de ablação por laser acoplada a um módulo de sucção e captura por filtro do particulado ejetado na ablação, permitindo envio do filtro para análise de emissões radioativas para classificação de radioisótopos. / The department Gerência de Rejeitos Radioativos (Radioactive Waste Management) from IPEN has already used the laser ablation technique for superficial decontamination of parts. This technique has also shown great potential for characterization of this waste with the purpose of rising data for the Radioisotopic Inventory of parts. The current techniques for this purpose (wipe sampling and physical modeling) lack the accuracy and practicality. The objective of this study is to develop the project of an instrument of laser ablation engaged with a module for sucking and capturing (by filter) the particulate ejected from the ablation, allowing the filter to be analyzed in laboratory for radioisotopic classification through radioactive emission.