Στην παρούσα εργασία μελετήθηκαν λεπτά υμένια οξειδίου του αλουμινίου (Al2O3) και οζειδίου του ζιρκονίου (ZrO2). Η ανάπτυξη των οξειδίων έγινε πάνω σε υπόστρωμα γερμανίου (Ge) με την τεχνική εναπόθεσης ατομικού στρώματος (Atomic Layer Deposition, ALD). Επίσης μελετήθηκαν υμένια οξειδίου του βολφραμίου (WO3), των οποίων η εναπόθεση έγινε με δυο διαφορετικές τεχνικές, πάνω σε υπόστρωμα P3HT:PCBM. Η μελέτη πραγματοποιήθηκε σε συνθήκες υπερυψηλού κενού (Ultra High Vacuum, UHV) με επιφανειακά ευαίσθητες τεχνικές. Κύριος στόχος αυτής της εργασίας, είναι για τα οξείδια αλουμινίου και ζιρκονίου η διερεύνηση της χημικής σύστασης και της ηλεκτρονιακής δομής ενώ θα γίνει μια εκτίμηση του πάχους των υμενίων καθώς και σύγκριση με την αναμενόμενη τιμή συμφωνα με την διαδικασία παρασκευής. Για οξείδια του βολφραμίου έγινε μελέτη τόσο της επιφανειακής χημικής σύστασης όσο και της ηλεκτρονιακής δομής της διεπιφάνειας του οξειδίου του βολφραμίου (WO3) με το υπόστρωμα P3HT:PCBM καθώς και μία σύγκριση των αποτελεσμάτων ανάμεσα στην εξάχνωση με δέσμη ηλεκτρονίων (Electron Beam Evaporation) και τη μέθοδο διαλύματος-πηκτώματος (Sol-Gel) τεχνικές οι οποίες χρησιμοποιήθηκαν για την εναπόθεση των υμενίων οξειδίου του βολφραμίου. / In the present work,studied thin films of aluminum oxide (Al2O3) and zirconium oxide (ZrO2) thin films. Atomic Layer Deposition technique (ALD) was used for the growth of oxide on the germanium (Ge) substrate. Also studied films of tungsten oxide (WO3), which were deposited with two different techniques, onto P3HT:PCBM substrate. The study was conducted under conditions of UHV (Ultra High Vacuum) using surface sensitive techniques. The main objective of this work was to investigate the chemical composition and electronic structure and make an estimate of the thickness of aluminum oxide and zirconium oxide thin films. The thickness was compared with the expected value according to the manufacturing process. For the tungsten oxides were studied the surface chemical composition and the electronic structure of the WO3/P3HT:PCBM interface as well as a comparison of results between the Electron Beam Evaporation and Sol-Gel method, techniques which were used for the deposition of thin films of tungsten oxide.

Mit Fe-Pd-Legierungen nahe der Zusammensetzung Fe70Pd30 kann man aufgrund des thermischen oder magnetischen Formgedächtniseffekts große Dehnungen erzeugen. Daher sind sie für Mikro- und Nanoaktoren sowie Sensoren von großem wissenschaftlichen und technologischen Interesse. Im Vergleich zu Massivmaterial und dünnen Schichten erwartet man für eindimensionale Geometrien wie Nanodrähte deutlich höhere Arbeitsfrequenzen und Dehnungen. Zur Herstellung von Nanodrähten eignet sich die elektrochemische Abscheidung in selbstordnende nanoporöse Membranen als effizienteste Methode gegenüber lithographischen oder physikalischen Methoden. Um den Formgedächtniseffekt auch in Fe-Pd-Nanodrähten mit ca. 30 at.% Pd zu nutzen, werden in dieser Arbeit entsprechende Herstellungsbedingungen wie Elektrolytsystem, Abscheideparameter und Nachbehandlung herausgearbeitet. Die Zusammenhänge zwischen Abscheidebedingungen und Morphologie, lokaler Mikrostruktur, Struktur sowie magnetischen Eigenschaften werden untersucht und bewertet. Es wird gezeigt, dass Fe-Pd-Nanodrähte trotz der Kombination aus edlem und unedlem Metall elektrochemisch hergestellt werden können. Ein komplexierter Fe-Pd-Elektrolyt in Kombination mit optimierten alternierenden Abscheidepotentialen führt reproduzierbar zu durchgehenden, nahezu defektfreien Nanodrähten nahe der Zusammensetzung Fe70Pd30. Mit einer nachträglichen Wärmebehandlung erreicht man eine vollständige Umwandlung der Fe-Pd-Legierung von der kubisch raumzentrierten zur kubisch flächenzentrierten Struktur. Die erfolgreiche Herstellung dieser Nanodrähte stellt eine Schlüsselposition auf dem Weg zu formgedächtnisbasierten Nanoaktoren dar. In dieser Arbeit konnten wichtige Ansatzpunkte zur Strukturkontrolle während der elektrochemischen Abscheidung und somit zur Aktivierung des Formgedächtniseffekts identifiziert werden. / Fe-Pd alloys at about 30 at.% Pd allow obtaining high length changes or strains in the percent range due to thermal or magnetic shape memory effect. They are especially promising candidates for smart and intelligent materials in micro- and nanoactuators as well as sensors. In comparison to bulk materials and thin films the utilization of nanowires promises higher actuation frequencies and strains, which further heighten the scientific and technological interest. Electrodeposition within self-organized nanoporous templates is a very time efficient method to prepare even large arrays of Fe-Pd nanowires of different length and diameter compared to lithographic or physical methods. The aim of this work is to exhibit the preparation conditions such as electrolyte system, deposition parameter and post treatment for shape memory active Fe-Pd nanowires at about 30 at.% Pd. Correlations between morphology, local microstructure, structure and magnetic properties are investigated and evaluated. Fe-Pd nanowires are successfully prepared by electrodeposition despite the combination of noble Pd and less noble Fe metals. The usage of an electrolyte with complexed Fe and Pd ions and an optimized alternating potential deposition regime leads to continuous and almost defect free nanowires close to the composition Fe70Pd30. The complete transition from the bcc to fcc structure of the Fe-Pd alloy is achieved by an additional heat treatment. However, the successful preparation of these nanowires represents a key element towards nanoactuators based on shape memory alloys. Fundamental knowledge about electrochemical preparation of Fe-Pd nanowires is gained. Important starting points towards structure control during deposition and activation of the shape memory effect are identified.

Hocheffiziente Solarzellen beruhen auf der exzellenten Oberflächenpassivierung, die minimale Rekombinationsverluste gewährleistet. Innerhalb des letzten Jahrzehnts wurde Al2O3 in der Photovoltaikindustrie zum bevorzugten Material für p-leitendes Si. Unterschiedliche Abscheidetechnologien erreichten Passivierungen mit effektiven Minoritätsladungsträgerlebensdauern nahe der AUGER–Grenze. Die ausgezeichnete Passivierungswirkung von Al2O3wird zwei Effekten zugeschrieben: Einerseits werden Si−SiO2-grenzflächennahe Rekombinationszentren passiviert, wenn Wasserstoff, beispielsweise aus der Al2O3-Schicht, offene Bindungen absättigt. Bedingt durch die hohe Konzentration intrinsischer negativer Ladungen an der SiO2-Grenzfläche weist Al2O3 andererseits einen charakteristischen Feldeffekt auf. Das resultierende elektrische Feld hält Elektronen von Oberflächenrekombinationszentren fern. Negative Ladungen im Al2O3 werden generell als fest bezeichnet. Allerdings hat Al2O3 zusätzlich eine hohe Dichte an Haftstellen, die von Elektronen besetzt werden können. Die Dichte negativer Ladungen im Al2O3-Passivierungsschichten hängt vom elektrischen Feld und der Bestrahlungsintensität ab. Ziel dieser Arbeit ist die systematische Untersuchung dielektrischer Passivierungsschichtstapel für die Anwendung auf Si-Solarzellen. Der Qualität und Dicke der SiO2-Grenzschicht kommt in diesem Kontext eine besondere Rolle zu, da sie Ladungsträgertunneln ermöglicht. Der Elektronentransport ist eine Funktion der Oxiddicke und das Optimum zwischen Ladungseinfang und -haltung liegt bei etwa 2 nm SiO2. Vier relevante Al2O3-Abscheidetechnologien werden untersucht: Atomlagenabscheidung, Kathodenzerstäubung, Sprühpyrolyse und Rotationsbeschichtung, wobei die erstgenannte dominiert. Es werden Nanolaminate verglichen, die aus Al2O3 und TiO2, HfO2 oder SiO2 mit subnanometerdicken Zwischenschichten bestehen. Während letztgenannte die Oberflächenrekombination nicht vermindern, beeinflussen TiO2- und HfO2-Nanolaminate die Passivierungswirkung. Ein dynamisches Wachstumsmodell, das initiale und stationäre Wachstumsraten der beteiligten Metalloxide berücksichtigt, beschreibt die physikalischen Parameter. Schichtsysteme mit 0,2 % TiO2 oder 7 % HfO2 sind konventionellen Al2O3-Schichten überlegen. In beiden Fällen überwiegt die veränderte Feldeffekt- der chemischen Passivierung, die mit einer Grenzflächenzustandsdichte von maximal 5·1010 eV−1·cm−2 unverändert auf hohem Niveau verbleibt. Die Ladungsdichte beider Schichtsysteme wird entweder über die Änderung ihrer Polarität der festen Ladungen oder der Fähigkeit zum Ladungseinfang bestimmt. Das Tunneln von Elektronen wird durch ein mathematisches Modell erklärt, dass eine bewegliche Ladungsfront innerhalb der Oxidschicht beschreibt. / High-efficiency solar cells rely on excellent passivation of the surface to ensure minimal recombination losses. In the last decade, Al2O3 became the material of choice for p-type Si in the photovoltaic industry. A remarkable surface passivation with effective minority carrier lifetimes close to the AUGER–limit was demonstrated with different deposition techniques. The excellent passivation effect of Al2O3 is attributed to two effects: Firstly, recombination centers at the Si−SiO2 interface get chemically passivated when hydrogen, for instance from the Al2O3 layer, saturates dangling bonds. Secondly, Al2O3 presents an outstanding level of field effect passivation due to its high concentration of intrinsic negative charges close to the SiO2 interface. The generated electrical field effectively repels electrons from surface recombination centers. Negative charges in Al2O3 are generally termed fixed charges. However, Al2O3 incorporates a high density of trap sites, too, that can be occupied by electrons. It was shown that the negative charge density in Al2O3 passivation layers depends on the electrical field and on the illumination intensity. The goal of this work is to systematically investigate dielectric passivation layer stacks for application on Si solar cells. The SiO2 interface quality and thickness plays a major role in this context, enabling or inhibiting carrier tunneling. Since the electron transport is a function of the oxide thickness, the balance between charge trapping and retention is achieved with approximately 2 nm of SiO2. Additionally, four relevant Al2O3 deposition techniques are compared: atomic layer deposition, sputtering, spray pyrolysis and spin–on coating, whereas the former is predominant. Using its flexibility, laminates comprising of Al2O3 and TiO2, HfO2 or SiO2 with subnanometer layers are compared. Although the latter do not show decreased surface recombination, nanolaminates with TiO2 and HfO2 contribute to the passivation. Their physical properties are described with a dynamic growth model that considers initial and steady–state growth rates for the involved metal oxides. Thin films with 0.2 % TiO2 or 7 % HfO2 are superior to conventional Al2O3 layers. In both cases, the modification of the field effect prevails the chemical effect, that is, however, virtually unchanged on a very high level with a density of interface traps of 5·1010 eV−1·cm−2 and below. The density of charges in both systems is changed via modifying either the polarity of intrinsic fixed charges or the ability of trapping charges within the layers. The observations of electron tunneling are explained by means of a mathematical model, describing a charging front, which moves through the dielectric layer.

Die vorliegende Arbeit behandelt die Synthese und die Eigenschaften von fluordotierten Aluminium(hydr)oxiden. Dazu wurde zunächst ein Syntheseprotokoll erarbeitet, das die kontrollierte und reproduzierbare Sol-Gel Synthese von F-Al(OH)3-Phasen ermöglichte. Auf Grundlage dieser Syntheseroute konnten Parameter wie der Fluorgehalt der Phasen kontrolliert und der Einfluss auf strukturelle Eigenschaften systematisch untersucht werden. Die Charakterisierung der amorphen Phasen wurde hauptsächlich über MAS NMR spektroskopische Methoden vorgenommen. Herausragendes Strukturmerkmal der Proben ist die Anwesenheit von AlV- und AlIV-Sites, die charakteristisch für das hohe Maß an struktureller Störung in den Proben sind. Über die Untersuchung der thermischen Eigenschaften konnte gezeigt werden, dass es schon bei Temperaturen von unterhalb 80 °C zur anteiligen Dehydroxylierung der Phasen kommt und mit einem starken Anstieg der unterkoordinierten AlV- und AlIV-Spezies verknüpft ist. Bei etwa 300 °C sind die Phasen weitestgehend dehydratisiert, allerdings kommt es bei Kontakt mit Luft zu einer Reaktion mit atmosphärischen H2O Molekülen. Bei ausreichend langer Zeit und hoher Luftfeuchtigkeit führt dies zu einer vollständigen Rehydratisierung der Probe, die wiederum mit dem Rückgang der AlV- und AlIV-Spezies verknüpft ist. Kalziniert man die F-Al(OH)3-Phasen im Vakuum bei 700 °C, erhält man ein schwach kristallines, übergangsaluminiumoxidähnliches F-Al2O3. Das so hergestellte F-Al2O3 besitzt kontrollierbare Mengen Fluorid und ist katalytisch aktiv. Der Einfluss von Fluorid auf die katalytische Aktivität und die Oberflächenbeschaffenheit der Proben wurde umfassend untersucht und über zwei unterschiedliche Testreaktion evaluiert. In diesem Zuge konnte auch die Bildung von Brønsted-Zentren auf der Oberfläche gesteuert und ihr Bildungsmechanismus besser verstanden werden. Ein besseres Verständnis zur katalytischen Lewis-Aktivität der Probe konnte durch die direkte Beobachtung der aktiven Oberfläche erreicht werden. Hier wurden reaktive und koordinativ ungesättigte AlV- und AlIV-Sites beobachtet, die durch den Kontakt mit Luft zerstört werden und dadurch ihre katalytische Aktivität verlieren. / The present work deals with the synthesis and properties of fluorine-doped aluminum (hydr)oxides. For this purpose, a synthesis protocol was first developed, which allowed the controlled and reproducible synthesis of F-Al(OH)3 phases. Based on this sol-gel route, parameters such as the fluorine content of the phases could be controlled and the influence on structural properties could be systematically investigated. The amorphous F-Al(OH)3 samples show a number of interesting properties. The characterization was carried out mainly by MAS NMR spectroscopic methods. Outstanding structural feature of the samples is the presence of AlV- and AlIV-sites, which are characteristic of the high degree of structural disorder in the samples. The investigation of the thermal properties has shown that even at temperatures below 80 °C there is a proportional dehydroxylation of the phases, which is associated with a strong increase of the undercoordinated AlV- and AlIV-species. At around 300 °C, the phases are largely dehydrated, but contact with air causes a reaction with atmospheric H2O molecules. With sufficient time and high humidity, this leads to complete rehydration of the sample, which in turn is associated with the decline of the AlV- and AlIV-species. If the F-Al(OH)3 phases are calcined in vacuum at 700 °C, a weakly crystalline transition alumina-like F-Al2O3 is obtained. Thus, the F-Al2O3 produced has controllable amounts of fluoride and is catalytically active. The influence of fluoride on the catalytic activity and surface finish of the samples was extensively studied and evaluated by two different test reactions. In this context, the formation of Brønsted centers on the surface could be controlled which also led to a better understanding of the mechanism of the formation. A better understanding of the catalytic Lewis activity of the sample could be achieved by direct observation of the active surface. Here, reactive and coordinatively unsaturated AlV- and AlIV-sites were observed which were destroyed by contact with air, thereby losing their catalytic activity.

O objetivo deste estudo foi comparar a resistência de união e a interface de falha da colagem de braquetes colados pela técnica indireta após o condicionamento do esmalte com jato de óxido de alumínio de 27, 50 e 90 m seguido da aplicação de ácido fosfórico a 37%; e avaliar quantitativa e qualitativamente as alterações da superfície do esmalte após os diferentes tipos de condicionamento. A amostra foi constituída por 104 pré-molares superiores. Na primeira parte da pesquisa 80 dentes foram divididos aleatoriamente em 4 grupos (n=20) que receberam diferentes condicionamentos das faces linguais: G1 (controle)- ácido fosfórico a 37%; G2, G3 e G4- jato de óxido de alumínio de 27, 50 e 90 m, respectivamente, antes da aplicação de ácido fosfórico. Braquetes linguais foram colados indiretamente com o mesmo material e metodologia nos 4 grupos. A força máxima de cisalhamento requerida para descolar os braquetes foi determinada por meio de uma máquina de ensaios mecânicos universal, e a interface de falha na colagem, por meio do Índice de Resina Remanescente (ARI). Para a avaliação quantitativa dos efeitos provocados no esmalte pelos diferentes condicionamentos, 20 dentes foram divididos aleatoriamente em 4 grupos, e suas faces linguais foram condicionadas de acordo com o protocolo proposto anteriormente. A rugosidade do esmalte (Ra) antes e após o seu condicionamento foi determinada por meio de um microscópio a laser confocal. Na avaliação qualitativa foram utilizados 4 dentes, que foram condicionados segundo protocolo descrito anteriormente. O teste ANOVA de um critério foi utilizado para comparar a resistência adesiva e o incremento de rugosidade entre os grupos. As diferenças entre as pontuações do ARI foram avaliadas com o teste de Kruskal-Wallis. Foi adotado nível de significância de 5% em todas as avaliações estatísticas. Não foram observadas diferenças estatisticamente significantes entre os quatro tipos de condicionamento de esmalte quando avaliou-se as médias de resistência de união e o incremento de rugosidade. Também não foram verificadas diferenças estatisticamente significativas entre as pontuações do ARI. O resultado da avaliação qualitativa evidenciou padrões diferentes de condicionamento entre o esmalte condicionado com ácido fosfórico e o esmalte condicionado com óxido de alumínio associado ao ácido. No esmalte condicionado com ácido, observaram-se leves irregularidades correspondentes com o padrão tipo III de Silverstone; enquanto no esmalte condicionado com jato de óxido de alumínio de 27, 50 e 90 m mais ácido fosfórico verificaram-se padrões similares de condicionamento, com superfícies de textura áspera bastante uniforme, presença de múltiplas elevações com diferentes alturas e bordas arredondadas, semelhantes ao padrão tipo II de Silverstone. Assim, concluiu-se que o condicionamento do esmalte com óxido de alumínio associado ao ácido não incrementou a resistência de união de braquetes colados indiretamente, não modificou a quantidade de resina remanescente, nem aumentou a rugosidade do esmalte. No entanto, produz um padrão de condicionamento diferente ao obtido com o ácido. / The purpose of this study was to compare the bond strength and the bond failure location of indirectly bonded brackets after enamel conditioning with 27, 50 and 90 m aluminum oxide followed by application of 37% phosphoric acid; and to analyze quantitatively and qualitatively the alterations on the enamel surface after the different conditionings. The sample consisted of 104 superior premolars. In the first stage of this research, 80 teeth were randomly divided into 4 groups (n=20) that received different conditionings at the lingual faces: G1 (control)- 37% phosphoric acid, G2, G3 and G4- 27, 50 and 90 m aluminum oxide, respectively, before applying phosphoric acid. The lingual brackets were indirectly bonded using the same material and methodology in the 4 groups. The maximum shear bond strength required to debond the brackets was determined using a mechanical testing machine, and the bond failure location through the Adhesive Remnant Index (ARI). For the quantitative analysis of the effects caused in the enamel due to the different conditionings, 20 teeth were randomly divided into 4 groups, and their lingual faces were conditioned according to the previously described protocol. The enamel roughness (Ra) before and after conditioning was measured using a confocal laser scanning microscope. In the qualitative analysis 4 teeth that were conditioned according to the previously described protocol were used. One-way ANOVA analysis was used to compare the bond strength and the roughness increment between the groups. The differences among the ARI scores were analyzed with the Kruskal-Wallis test. A 5% significance level was adopted for all statistical analysis. No statistical differences were observed among the 4 types of enamel conditionings when the mean shear bond strength and roughness increase were compared. There were not also statistically significant differences between the ARI scores. The results of the qualitative analysis showed different conditioning patterns between the enamel prepared with phosphoric acid and the enamel treated with aluminum oxide associated to phosphoric acid. In the acid-etching enamel, slight irregularities corresponding to Silverstones type III pattern were found; while in the enamel conditioned with aluminum oxide of 27, 50 and 90 m followed by phosphoric acid, similar conditioning patterns were found, with rough surfaces highly uniform, presence of multiple elevations of different heights and rounded edges, similar to Silverstones type II pattern. In conclusion, the enamel conditioning with aluminum oxide associated to phosphoric acid did not increase the bond strength of indirectly bonded brackets; it did not modify the quantity of remnant resin nor increased the enamel roughness. However, it produced a conditioning pattern different to the one obtained with acid.

A dosimetria das radiações alfa, beta e gama é importante para diversas áreas aplicadas, sendo utilizada na proteção radiológica de pacientes e profissionais que se expõem a esses tipos de radiações. Com estudos dosimétricos pode-se obter melhores estimativas de dose absorvida, e ter mais precisão na estimativa de riscos populacionais. As técnicas de Termoluminescência (TL) e Luminescência Oticamente Estimulada (OSL) são utilizadas para essas aplicações dosimétricas. Estudos recentes têm mostrado que alguns materiais dosimétricos conhecidos como óxido de alumínio dopado com carbono (Al$_2$O$_3$:C) e óxido de berílio (BeO) sofrem mudanças no formato observado dos sinais OSL com relação as taxas de dose e tipos de radiação. O principal objetivo desse trabalho foi analisar os formatos dessas curvas e verificar quantitativamente, se existem ou não mudanças nos formatos dos sinais OSL dos dosímetros irradiados com diferentes tipos de radiação e taxas de dose. Sob o modelo de uma armadilha e um centro de recombinação (OTOR) foram estudados os sinais OSL com estímulo contínuo (CW-OSL). O modelo OTOR é simples, mas não possui solução analítica e as soluções computacionais são custosas pelo número grande de variáveis e parâmetros. Nesse trabalho, foi necessário realizar algumas simplificações para obtenção de um modelo ainda mais simples para ajuste nos dados. O modelo OTOR simples apresenta um comportamento de decaimento exponencial na descrição do sinal CW-OSL. Uma outra abordagem de extensão do modelo OTOR-simples foi a utilização do modelo com duas armadilhas independentes e um centro de recombinação, que resulta em dois decaimentos exponenciais. Para obtenção dos parâmetros que descrevem o sinal CW-OSL com esses modelos, foi utilizado o método dos mínimos quadrados (MMQ), com refinamento dos parâmetros pelo método de Gauss. O modelo de dois decaimentos exponenciais mostrou-se superior em qualidade com análise do parâmetro $\\chi^2$ e do comportamento dos resíduos em relação ao modelo de um decaimento exponencial para ambos os materiais utilizados. Com os ajustes, foi possível verificar diferenças nos comportamentos do sinal CW-OSL das amostras irradiadas em diferentes situações. As diferenças observadas nos comportamentos são apresentadas pelos parâmetros de decaimento ou de sinal inicial, ou pelas relações entre esses. Os parâmetros ajustados mostram que os sinais OSL provenientes do Al$_2$O$_3$:C e do BeO irradiados com alfa, beta e gama apresentam diferenças significativas nos comportamentos. As diferenças verificadas pelos ajustes dos sinais CW-OSL apresentados pelos dosímetros irradiados com beta e gama podem ter sido em parte causadas por efeito de fading, que afeta de maneira distinta os formatos das curvas e parâmetros ajustados. Nas irradiações com radiação gama com faixas de doses (de 22 a 122 mGy) e taxas doses absorvidas (de 0.024 a 1.66 Gy/s) não foram observados diferenças significativas nos sinais OSL. / The dosimetry of alpha, beta and gamma radiation is important in various applied areas, it is used in radiation protection of patients and professionals who are exposed at this kind of radiation. With dosimetric studies, it is possible to better estimate the absorbed dose, and population risks. Thermoluminescence (TL) and Optically Stimulated Luminescence (OSL) techniques are used for these dosimetric applications. Recent studies have shown that some known dosimetric materials as carbon doped aluminum oxide (Al$_2$O$_3$:C) and berilium oxide (BeO) undergo changes in OSL signal behavior related to dose rates and types of radiation. The main objective of this work was to analise the formats of these curves and quantitatively verify whether or not there are changes in OSL signal of the dosimeters irradiated with different types of radiation and dose rates. Under the model of one trap one recombination center (OTOR) the continuous wave OSL (CW-OSL) signals were studied. The OTOR model is the simplest model, but has no analytical solution and the computational solutions are costly by the large number of variables and parameters. In this work, it was necessary to make some simplifications in order to obtain a simple model that could be fitted to the data. The simple-OTOR model shows an exponential decay behavior in the CW-OSL signal description. Another extension approach to the simple-OTOR model was the model with two independent traps and one recombination center, that results in two exponential decays. To obtain the parameters that describe the CW-OSL signal with these models, the least square method (LSM) was used, with parameter refinement by Gauss method. For both the materials the two exponential decay model proved to be superior in quality to the one exponential decay by the analysis of the parameter $\\chi^2$ and the behavior of the residuals. With the fittings, it was possible to verify differences in the behavior of the CW-OSL signal of the samples irradiated in different situations. These differences observed are presented in the decay or initial signal parameters, or in their ratios. Fitted parameters show that OSL signals from Al$_2$O$_3$:C and BeO irradiated with alpha, beta and gamma exhibit significant differences in behavior. The differences verified by the fittings of the CW-OSL signals presented by beta and gamma irradiated dosimeters may in part have been caused by fading effect, which affects in a different way the shapes of the curves and fitted parameters. Gamma irradiation with dose and absorbed dose rate ranges from 22 to 122 mGy and from 0.024 to 1.66Gy/s respectively did not produce significant differences in OSL signals.

Made available in DSpace on 2017-07-21T20:42:41Z (GMT). No. of bitstreams: 1 Graciela Aparecida Santos Silva.pdf: 4725206 bytes, checksum: 1b5275fc3c55802f9ed0465ffbc48d75 (MD5) Previous issue date: 2013-02-22 / Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / The purpose of this work was the synthesis of nanoscaled BaO-Al2O3-MnO2 system and its characterization. The nanoparticulate system was prepared by mixing salts of Ba, Al and Mn in a chamber of low temperature, lyophilizing the solutions of their salts, and followed by calcination in the temperature range from 230 °C to 1190° C.This synthesis was compared with two other systems, prepared using a chemical mixture of oxides, with a particle size of conventional size and also with the phase of nanoscale oxides, followed by calcination in the same temperature conditions. The colorimetric properties of ceramic powders were evaluated by UV-visible spectroscopy and coordinates CIE-L a b and characterized by X-ray diffraction, Xray fluorescence, simultaneous thermal analyisis, scanning electron microscopy and laser scattering technique. This nanoscaled synthesis provides a possible application in the production on ceramic pigments because the resulting powder showed different color in comparison to the other systems. The nanoparticulate system showed the advantage of needing lower calcination temperatures, and, at 1135ºC,showed a different color that was not presented by powders synthetized by other methods. / A proposta deste trabalho consiste na síntese em nanoescala do sistema BaO-Al2O3-MnO2, bem como sua caracterização. O sistema nanoparticulado foi preparado misturando sais de Ba, Al e Mn em câmara de baixa temperatura, liofilizando-se assim as soluções dos respectivos sais, seguidos de calcinação na faixa de temperatura de 230 °C a 1190 °C. Comparou-se esta síntese com duas metodologias, preparadas através de uma mistura química de óxidos, com tamanho de partícula convencional e também com tamanho de fase dos óxidos em nanoescala, seguidas de calcinação nas mesmas condições de temperatura. Os pós cerâmicos foram avaliadas por espectroscopia no UV-visível e coordenadas CIE-L a b e caracterizado por difração raios X, fluorescência de raios X, termogravimetria e análise termodiferencial simultânea, microscopia eletrônica de varredura e espectroscopia de fotocorrelação. Essa síntese por nanoescala traz a possível aplicação na produção de pigmentos cerâmicos, pois trouxe alterações colorimétricas diferentes comparando com os outros sistemas. Esse método teve vantagem, pois trouxe temperaturas de calcinação mais baixa, e em 1135 ºC, o sistema nanoparticulado apresentou uma coloração que não foi observado para os outros métodos de síntese.

Made available in DSpace on 2016-12-23T14:08:11Z (GMT). No. of bitstreams: 1 Roberto Balarini Junior - Parte 1.pdf: 4732272 bytes, checksum: 0c0798e2e5b19f7834c4ce1d56156d8f (MD5) Previous issue date: 2013-11-27 / Este trabalho é uma investigação tribológica envolvendo o par cerâmico composto por esferas de nitreto de silício (Si3N4) deslizando contra discos de óxido de alumínio (Al2O3) em água. No total, dez ensaios foram conduzidos com a intenção de reproduzir o fenômeno de Ultra Baixo Coeficiente de Atrito (UBCA) em laboratório, o qual é caracterizado pela obtenção de valores de coeficiente de atrito (&#956;) da ordem dos milésimos (&#956; < 0,01) no regime estacionário. Uma vez alcançado os valores de UBCA, o objetivo principal deste trabalho foi o de investigar o período de running-in, através de uma série de análises em relação ao comportamento do coeficiente de atrito durante o regime transitório, incluindo correlações com algumas variáveis, como rugosidade superficial, erros de batimento axial, íons formados durante o deslizamento e desgaste das cerâmicas. Para isto, as curvas de coeficiente de atrito por tempo foram expandidas para intervalos de tempos pré-determinados e o comportamento de &#956; em cada um destes intervalos foi investigado e comparado entre os ensaios realizados, sendo que o caráter oscilatório do coeficiente de atrito foi inserido nas análises do período transitório. Em geral, foi comprovado que maiores valores de rugosidade superficial resultaram em maiores períodos de running-in e que existe uma tendência de aumento de desgaste com o aumento do tempo de transição. Para todos os ensaios, a taxa de desgaste das esferas de Si3N4 foi superior à dos discos de Al2O3. Em adição, através de comparações entre a medida da soma das rugosidades das superfícies desgastadas com a espessura mínima do filme lubrificante, este trabalho confirma a hipótese de que é necessário um regime de lubrificação misto (hidrodinâmico e limítrofe) para a obtenção do regime de UBCA, sendo que, para a eficácia do modo de lubrificação esperado, estima-se que é necessário concentrações de íons de silício (Si) superiores a 1,3 mg/l, aproximadamente. Esta quantidade de íons Si é supostamente a mínima necessária para a formação de uma camada de sílica adequada para conferir a parcela de lubrificação limítrofe necessária para a obtenção do regime de UBCA / This work is a tribological investigation involving the ceramic pair composed by balls of silicon nitride (Si3N4) sliding against disks of aluminum oxide (Al2O3) under water. A total of ten tests were conducted in order to reproduce the phenomenon of Ultra Low Friction Coefficient (ULFC) in laboratory, which is characterized by obtaining values of friction coefficient (&#956;) below of 0,01 in the steady state. Once reached these values, the main objective of this study was to investigate the running-in period by a series of analyses in relation to the behavior of the friction coefficient during the running-in period, including correlations with some variables such as surface roughness, axial parallelism errors, ions formed during the sliding and wear of samples. For this reason, the curves of friction coefficient versus time were expanded for some predetermined intervals and the behavior of &#956; for each one of these intervals was investigated and compared between themselves, and the oscillatory behavior of the friction coefficient was inserted into the analysis of the running-in period. In general, it was concluded that higher values of surface roughness resulted in longer periods of running-in and that there is a trend of increasing wear with increasing time of transition. For all tests, the wear rate of the silicon nitride balls was higher than alumina disks. In addition, by comparing the measure of the sum of the roughness of the worn surfaces with minimum thickness of the lubricant film, the present work confirms the hypothesis that it is necessary a mixed lubrication (hydrodynamic combined with boundary) to obtain the regime of ULFC and for effective lubrication expected mode it is estimated that is required an ions concentration of silicon (Si) higher than 1.3 mg/l approximately. This amount of ions Si is supposed to be the minimum necessary for the formation of a silica layer enable to confer the boundary lubrication participation for obtaining the ULFC

O objetivo deste estudo foi comparar a resistência de união e a interface de falha da colagem de braquetes colados pela técnica indireta após o condicionamento do esmalte com jato de óxido de alumínio de 27, 50 e 90 m seguido da aplicação de ácido fosfórico a 37%; e avaliar quantitativa e qualitativamente as alterações da superfície do esmalte após os diferentes tipos de condicionamento. A amostra foi constituída por 104 pré-molares superiores. Na primeira parte da pesquisa 80 dentes foram divididos aleatoriamente em 4 grupos (n=20) que receberam diferentes condicionamentos das faces linguais: G1 (controle)- ácido fosfórico a 37%; G2, G3 e G4- jato de óxido de alumínio de 27, 50 e 90 m, respectivamente, antes da aplicação de ácido fosfórico. Braquetes linguais foram colados indiretamente com o mesmo material e metodologia nos 4 grupos. A força máxima de cisalhamento requerida para descolar os braquetes foi determinada por meio de uma máquina de ensaios mecânicos universal, e a interface de falha na colagem, por meio do Índice de Resina Remanescente (ARI). Para a avaliação quantitativa dos efeitos provocados no esmalte pelos diferentes condicionamentos, 20 dentes foram divididos aleatoriamente em 4 grupos, e suas faces linguais foram condicionadas de acordo com o protocolo proposto anteriormente. A rugosidade do esmalte (Ra) antes e após o seu condicionamento foi determinada por meio de um microscópio a laser confocal. Na avaliação qualitativa foram utilizados 4 dentes, que foram condicionados segundo protocolo descrito anteriormente. O teste ANOVA de um critério foi utilizado para comparar a resistência adesiva e o incremento de rugosidade entre os grupos. As diferenças entre as pontuações do ARI foram avaliadas com o teste de Kruskal-Wallis. Foi adotado nível de significância de 5% em todas as avaliações estatísticas. Não foram observadas diferenças estatisticamente significantes entre os quatro tipos de condicionamento de esmalte quando avaliou-se as médias de resistência de união e o incremento de rugosidade. Também não foram verificadas diferenças estatisticamente significativas entre as pontuações do ARI. O resultado da avaliação qualitativa evidenciou padrões diferentes de condicionamento entre o esmalte condicionado com ácido fosfórico e o esmalte condicionado com óxido de alumínio associado ao ácido. No esmalte condicionado com ácido, observaram-se leves irregularidades correspondentes com o padrão tipo III de Silverstone; enquanto no esmalte condicionado com jato de óxido de alumínio de 27, 50 e 90 m mais ácido fosfórico verificaram-se padrões similares de condicionamento, com superfícies de textura áspera bastante uniforme, presença de múltiplas elevações com diferentes alturas e bordas arredondadas, semelhantes ao padrão tipo II de Silverstone. Assim, concluiu-se que o condicionamento do esmalte com óxido de alumínio associado ao ácido não incrementou a resistência de união de braquetes colados indiretamente, não modificou a quantidade de resina remanescente, nem aumentou a rugosidade do esmalte. No entanto, produz um padrão de condicionamento diferente ao obtido com o ácido. / The purpose of this study was to compare the bond strength and the bond failure location of indirectly bonded brackets after enamel conditioning with 27, 50 and 90 m aluminum oxide followed by application of 37% phosphoric acid; and to analyze quantitatively and qualitatively the alterations on the enamel surface after the different conditionings. The sample consisted of 104 superior premolars. In the first stage of this research, 80 teeth were randomly divided into 4 groups (n=20) that received different conditionings at the lingual faces: G1 (control)- 37% phosphoric acid, G2, G3 and G4- 27, 50 and 90 m aluminum oxide, respectively, before applying phosphoric acid. The lingual brackets were indirectly bonded using the same material and methodology in the 4 groups. The maximum shear bond strength required to debond the brackets was determined using a mechanical testing machine, and the bond failure location through the Adhesive Remnant Index (ARI). For the quantitative analysis of the effects caused in the enamel due to the different conditionings, 20 teeth were randomly divided into 4 groups, and their lingual faces were conditioned according to the previously described protocol. The enamel roughness (Ra) before and after conditioning was measured using a confocal laser scanning microscope. In the qualitative analysis 4 teeth that were conditioned according to the previously described protocol were used. One-way ANOVA analysis was used to compare the bond strength and the roughness increment between the groups. The differences among the ARI scores were analyzed with the Kruskal-Wallis test. A 5% significance level was adopted for all statistical analysis. No statistical differences were observed among the 4 types of enamel conditionings when the mean shear bond strength and roughness increase were compared. There were not also statistically significant differences between the ARI scores. The results of the qualitative analysis showed different conditioning patterns between the enamel prepared with phosphoric acid and the enamel treated with aluminum oxide associated to phosphoric acid. In the acid-etching enamel, slight irregularities corresponding to Silverstones type III pattern were found; while in the enamel conditioned with aluminum oxide of 27, 50 and 90 m followed by phosphoric acid, similar conditioning patterns were found, with rough surfaces highly uniform, presence of multiple elevations of different heights and rounded edges, similar to Silverstones type II pattern. In conclusion, the enamel conditioning with aluminum oxide associated to phosphoric acid did not increase the bond strength of indirectly bonded brackets; it did not modify the quantity of remnant resin nor increased the enamel roughness. However, it produced a conditioning pattern different to the one obtained with acid.

Cette étude, expérimentale et théorique, de physique des surfaces développe une méthode basée sur la spectroscopie de perte d'énergie des photoélectrons, pour déterminer les propriétés électroniques d'un matériau à partir de mesures XPS. Sur la base de la physique de la photoémission dans un solide homogène, la technique XPS-PEELS donne accès à la fonction de perte d'énergie ELF(E, q) liée à la partie imaginaire et la fonction diélectrique sur une large plage d’énergie (environ 50 eV) avec une sensibilité typique de ≈ 5 nm en profondeur. Dans les métaux ou les semi-conducteurs à faible gap, qui présentent un chevauchement important entre le pic quasi-élastique ZLP(E) et la région des pertes d'énergie, la technique est rendue applicable par la méthode de transformée de Fourier développée dans cette thèse. Les distributions en énergie de la source de rayons X et de la fonction d’appareil sont directement mesurées. La forme asymétrique du pic quasi-élastique ZLP(E) est obtenue à partir de la densité d’états électroniques (calcul par une méthode DFT), à l’aide du modèle de Hopfield-Wertheim-Citrin décrivant la réponse des électrons de valence à la création du trou (théorie multi-corps). L'algorithme XPS-PEELS utilise l'ensemble du spectre sans soustraction empirique d’une ligne de base. Il considère deux types d'excitations de plasmon - intrinsèques et extrinsèques - avec des taux de création différents mais impose la même distribution en énergie. Cette méthode originale permet d’accéder à des excitations électroniques de faible énergie (pertes proches du pic XPS) ; dans le cas de l'aluminium métallique, la transition inter-bandes est observée à 1.80 eV. En tant que technique de spectroscopie électronique, les effets de dispersion de la fonction de perte ELF(E, q) ont été considérés en utilisant un code TD-DFT (Exciting); quel que soit le niveau d'approximation (RPA, ALDA, LRC), les calculs ne décrivent pas correctement la largeur du spectre ELF expérimental (2.3 eV). À la fin du travail, nous comparons la méthode de la transformée de Fourier avec une méthode empirique d'élimination du pic élastique, valable pour les isolants, dans le cas de l'oxyde d'aluminium Al₂O₃. / This surface physics study, experimental and theoretical, develops a technique based on the energy loss spectroscopy of photoelectrons, to determine electronic properties of a material from XPS measurements. Based on the physics of photoemission in a homogeneous solid, the XPS-PEELS technique provides the energy loss function ELF(E, q) related to the imaginary part and the dielectric function with energy extension up to 50 eV and a typical sensitivity of ≈ 5 nm in depth. In metals or low-gap semiconductors, with important overlap between the elastic peak and the energy loss region, the technique became applicable by the Fourier transform method developed in this thesis. In addition to the distribution of the X-ray source and analyzer apparatus function, the asymmetric shape of the no-loss peak ZLP(E) is based on the calculation of the Density of Electronic States (DFT method) and the Hopfield-Wertheim-Citrin model describing the response of valence electrons to the creation of the hole (many body theory). The XPS-PEELS algorithm uses the entire spectrum without any empirical background subtraction. It considers two types of plasmon excitations - intrinsic and extrinsic - with different rates of creation but imposing the same distribution in energy. This original method was applied to the aluminum metal, allowing the analysis of the loss function and revealing interband excitations (1.80 eV) at low energy, very close to the no-loss peak. As an electron spectroscopy technique, dispersion effects of the loss function ELF(E, q) were considered using a TD-DFT code (Exciting); for any level of approximation (RPA, ALDA, LRC), the calculations do not describe properly the high width (2.3 eV) of the experimental ELF. At the end of the work, we compare the Fourier transform method with an empirical method of elastic peak elimination, valid for insulators, in the case of aluminum oxide Al₂O₃.