Advanced high strength steels (AHSS) have high susceptibility to hydrogen embrittlement, and are often exposed to hydrogen environments in processing. In order to study the embrittlement and recovery of steel, tensile tests were conducted on two different types of AHSS over time after hydrogen charging. Concentration measurements and hydrogen microprinting were carried out at the same time steps to visualize the hydrogen behavior during recovery. The diffusible hydrogen concentration was found to decay exponentially, and equations were found for the two types of steel. Hydrogen concentration decay rates were calculated to be -0.355 /hr in TBF steel, and -0.225 /hr in DP. Hydrogen concentration thresholds for embrittlement were found to be 1.04 mL/100 g for TBF steel, and 0.87 mL/100g for DP steel. TBF steel is predicted to recover from embrittlement within 4.1 hours, compared to 7.2 hours in DP steel. A two-factor method of evaluating recovery from embrittlement, requiring hydrogen concentration threshold and decay rate, is explained for use in predicting recovery after exposure to hydrogen. Anisotropic hydrogen diffusion rates were also observed on the surface of both steels for a short time after charging, as hydrogen left the surface through <001> and <101> grains faster than grains with <111> orientations. This could be explained by differences in surface energies between the different orientations.

Neste trabalho são estudados os mecanismos de desgaste, atuantes na escala do tamanho de grão (meso-escala), durante ensaios de cavitação vibratória, para diferentes amostras de aços inoxidáveis austeníticos ligados com nitrogênio. Amostras com teores superficiais de nitrogênio de aproximadamente 0, 9 % massa, 1, 4%massa e 20%massa, obtidas a partir do a¸co inoxidável dúplex UNS S31803, foram estudadas. As amostras do a¸co inoxidável duplex UNS S31803, com aproximadamente 0, 9 % N massa, foram obtidas por nitretação gasosa em alta temperatura (temperatura de nitretação entre 1050 e 1200 C) e consistiram em três grupos diferentes: amostras com nitrogênio em solução sólida e solubilizadas, amostras com precipitação de nitretos e amostras com nitrogênio em solução sólida e encruadas. Já as amostras com teor de nitrogênio próximo de 20 % N massa foram processadas por meio de nitretação a plasma na temperatura de 400 C, obtendo-se uma camada superficial de austenita expandida. As amostras de ensaio foram submetidas à caracterização de textura por difração de elétrons retroespalhados, EBSD, e posteriormente à cavitação vibratória em ´agua destilada. Os ensaios de cavitação foram periodicamente interrompidos com o intuito de estudar a deteriora¸cao das amostras por exame das mesmas no microscópio eletrônico de varredura, MEV, e por medidas de perda de massa. Quando comparadas com os aços inoxidáveis austeníticos convencionais (UNS S30403 solubilizado e UNS S31803 como recebido), sem adição de nitrogênio e livre de encruamento, as amostras estudadas apresentaram resistência ao desgaste por cavitação superior, quantificada tanto pelo tempo de incubação do dano com perda de massa quanto pela taxa máxima de perda de massa nos estágios avançados do dano. A taxa máxima de perda de massa para cada tipo de amostra estudada, com relação `a taxa máxima do material de comparação, o aço inoxidável convencional sem adição de nitrogênio e livre de encruamento (UNS S30403) solubilizado, foi de: amostras com precipitação de nitretos (318HTGN+Nit), 6,9 vezes menor; amostras com nitrogênio em solução sólida e solubilizadas (318HTGH+Sol) e laminadas e solubilizadas (318HTGN+Lam+Sol), 26,8 e 25 vezes menor, respectivamente; amostras com nitrogênio em solução sólida e encruadas (318HTGN+Enc) 145 vezes menor; e amostras com camada superficial de austenita expandida (obtidas por nitretação a plasma), (318HTGN+Plas e 304LSol+Plas) 290 e 1,77 e vezes menor respectivamente. O efeito benéfico da adição de nitrogênio na resistência à erosão por cavitação dos aços inoxidáveis austeníticos estudados foi atribuído a: (i) aumento na resistência à deformação plástica; (ii) distribuição mais homogênea da deformação plástica induzida pelas ondas de choque e micro-jatos característicos do processo de cavitação; e (iii) aumento da importância relativa dos mecanismos de perda de massa com elevado consumo de energia de impacto. Nos primeiros estágios do dano erosivo por cavitação se observou clara evidência de deformação plástica, acompanhada de formação de microreelevo superficial e de protrusão de bandas de escorregamento. A perda de massa em nível microscópico (observações no MEV) começa como destacamento de material em microtrincas e micropites. Observou-se que tanto a nucleação do dano como o seu crescimento se apresenta de forma heterogênea na escala do tamanho de grão. Os sítios microestruturais nos quais se iniciou o dano com perda de massa foram preferencialmente protuberâncias nas protrusões de bandas de escorregamento, protuberâncias nos contornos de grão e as interfaces matriznitreto. O incremento do teor de nitrogênio (em solução sólida) na amostra aumentou a importância relativa dos contornos de grão como locais de nucleação do dano, em relação ao dano iniciado no interior dos grãos. Observou-se que o interior dos grãos com planos 100 ou 111 orientados de forma aproximadamente paralela à superfície das amostras são regiões muito suscetíveis à incubação do dano e ao crescimento do mesmo. Já os grãos com planos 101 orientados aproximadamente paralela à superfície das amostras, apresentam regiões com resistência ao dano bem maior. Esses resultados são discutidos, considerando as diferenças de tensão (resultantes da ação de ondas de choque causadas pela implosão de bolhas de cavitação) crítica projetada para cisalhamento de grãos com diferentes orientações. O dano ocorre preferencialmente em contornos de grãos com acentuados gradientes de tensão resolvida para a deformação plástica, onde se desenvolve elevada concentração de tensões. Em particular, os contornos de macla CSL 3 são acentuadamente mais suscetíveis à incubação do dano que os outros tipos de contornos CSL e que os contornos não CSL. / High nitrogen austenitic stainless steels containing 0.9 wt-% N and 20 wt- % N were tested in a ultrasonically induced vibratory cavitation testing device. Incubation times for damage initiation and mass losses were periodically measured during the cavitation-erosion tests. Scanning Electron Microscopy observation of the damaged surfaces allowed identifying the wear mechanisms operating during each step of the cavitation-erosion test. 0.9 wt-% N specimens were obtained through High Temperature Gas Nitriding UNS S31803 duplex stainless steel, at temperatures between 1050 and 1200 oC. Three groups of specimens were obtained: solubilized with all nitrogen in solid solution, solubilized and work hardened specimens and nitride containing specimens. The 20 wt- % N specimens were obtained through Low Temperature Plasma Nitriding the already High Temperature Gas Nitrided specimens and getting an expanded austenite layer at the surface. The specimens were firstly characterized by Electron Backscattered Diffraction - EBSD techniques and then submitted to the cavitation-erosion tests in distilled water. When compared to conventional UNS S30403 lean nitrogen solubilized austenitic stainless steel specimens, greater incubation times and smaller maximum wear rates were observed. The maximum wear rates (compared to those of the solubilized UNS S30403 steel) were: for the nitride containing specimen 6.9 times smaller; for textured and non-textured all nitrogen in solid solution specimens 26.8 and 25 times smaller, respectively; for the solubilized and work hardened specimen 145 times smaller; for the expanded austenite layer, with circa 20 wt- % N, specimens 300 times smaller. The beneficial effect of nitrogen on the cavitation-erosion resistance of the studied specimens was attributed to: (i) an increase in resistance to plastic deformation; (ii) a more homogeneous distribution of the plastic deformation; and (iii) an increase of the relative participation of energy consuming mass loss mechanisms. Plastic deformation accompanied by formation of micro relief at the surface and slip bands protrusions were clearly identified, during the first stages of cavitation erosion. The first evidences of mass loss (detected by SEM observations) were seen as particles detaching from micro cracks and micro pits formed at the grain surface. Nucleation and growth of cavitation damage was heterogeneously distributed at the grain scale. Slip bands protrusions, grain boundary protrusions and nitride matrix interfaces sites were more prone to nucleating the damage. Increasing nitrogen contents in solid solution increased the relative contribution of grain boundary nucleated damage, compared to the total amount of nucleation sites. Grains with 100 and 111 crystallographic planes approximately parallel to the surface were more prone to nucleation and growth of cavitation damage. Grains with 101 planes // surface were much more resistant to cavitation-erosion damage. These results are discussed considering differences of critical resolved shear stresses for grains with different orientations. Cavitation erosion damage occurs preferentially at grain boundaries across which steep stress gradients arise. Particularly, CSL -3 twin boundaries are much more susceptible to cavitation erosion damage incubation than other types of CSL boundaries and non CSL boundaries.

The primary reason for incorporating pigments into plastic materials is to impart the desired colour to finished articles. Some pigments however, may interact with the polymer leading to unexpected deleterious effects. Organic pigments, especially phthalocyanines, are favourable for their brilliant shade but are also well known for causing part distortion or warpage. This causes problems in parts which require good dimensional stability such as crates, containers, trays, caps and closures. Despite that, there are not many published studies on the root cause and mechanism of warpage induced by the pigment. Hence, the objective of this research is to study the influence of such pigments on the dimensional stability, crystallisation behaviour and morphology of polyethylenes in order to have a better understanding on the mechanism of warpage, which could possibly lead to a solution in overcoming this problem.

Neste trabalho são estudados os mecanismos de desgaste, atuantes na escala do tamanho de grão (meso-escala), durante ensaios de cavitação vibratória, para diferentes amostras de aços inoxidáveis austeníticos ligados com nitrogênio. Amostras com teores superficiais de nitrogênio de aproximadamente 0, 9 % massa, 1, 4%massa e 20%massa, obtidas a partir do a¸co inoxidável dúplex UNS S31803, foram estudadas. As amostras do a¸co inoxidável duplex UNS S31803, com aproximadamente 0, 9 % N massa, foram obtidas por nitretação gasosa em alta temperatura (temperatura de nitretação entre 1050 e 1200 C) e consistiram em três grupos diferentes: amostras com nitrogênio em solução sólida e solubilizadas, amostras com precipitação de nitretos e amostras com nitrogênio em solução sólida e encruadas. Já as amostras com teor de nitrogênio próximo de 20 % N massa foram processadas por meio de nitretação a plasma na temperatura de 400 C, obtendo-se uma camada superficial de austenita expandida. As amostras de ensaio foram submetidas à caracterização de textura por difração de elétrons retroespalhados, EBSD, e posteriormente à cavitação vibratória em ´agua destilada. Os ensaios de cavitação foram periodicamente interrompidos com o intuito de estudar a deteriora¸cao das amostras por exame das mesmas no microscópio eletrônico de varredura, MEV, e por medidas de perda de massa. Quando comparadas com os aços inoxidáveis austeníticos convencionais (UNS S30403 solubilizado e UNS S31803 como recebido), sem adição de nitrogênio e livre de encruamento, as amostras estudadas apresentaram resistência ao desgaste por cavitação superior, quantificada tanto pelo tempo de incubação do dano com perda de massa quanto pela taxa máxima de perda de massa nos estágios avançados do dano. A taxa máxima de perda de massa para cada tipo de amostra estudada, com relação `a taxa máxima do material de comparação, o aço inoxidável convencional sem adição de nitrogênio e livre de encruamento (UNS S30403) solubilizado, foi de: amostras com precipitação de nitretos (318HTGN+Nit), 6,9 vezes menor; amostras com nitrogênio em solução sólida e solubilizadas (318HTGH+Sol) e laminadas e solubilizadas (318HTGN+Lam+Sol), 26,8 e 25 vezes menor, respectivamente; amostras com nitrogênio em solução sólida e encruadas (318HTGN+Enc) 145 vezes menor; e amostras com camada superficial de austenita expandida (obtidas por nitretação a plasma), (318HTGN+Plas e 304LSol+Plas) 290 e 1,77 e vezes menor respectivamente. O efeito benéfico da adição de nitrogênio na resistência à erosão por cavitação dos aços inoxidáveis austeníticos estudados foi atribuído a: (i) aumento na resistência à deformação plástica; (ii) distribuição mais homogênea da deformação plástica induzida pelas ondas de choque e micro-jatos característicos do processo de cavitação; e (iii) aumento da importância relativa dos mecanismos de perda de massa com elevado consumo de energia de impacto. Nos primeiros estágios do dano erosivo por cavitação se observou clara evidência de deformação plástica, acompanhada de formação de microreelevo superficial e de protrusão de bandas de escorregamento. A perda de massa em nível microscópico (observações no MEV) começa como destacamento de material em microtrincas e micropites. Observou-se que tanto a nucleação do dano como o seu crescimento se apresenta de forma heterogênea na escala do tamanho de grão. Os sítios microestruturais nos quais se iniciou o dano com perda de massa foram preferencialmente protuberâncias nas protrusões de bandas de escorregamento, protuberâncias nos contornos de grão e as interfaces matriznitreto. O incremento do teor de nitrogênio (em solução sólida) na amostra aumentou a importância relativa dos contornos de grão como locais de nucleação do dano, em relação ao dano iniciado no interior dos grãos. Observou-se que o interior dos grãos com planos 100 ou 111 orientados de forma aproximadamente paralela à superfície das amostras são regiões muito suscetíveis à incubação do dano e ao crescimento do mesmo. Já os grãos com planos 101 orientados aproximadamente paralela à superfície das amostras, apresentam regiões com resistência ao dano bem maior. Esses resultados são discutidos, considerando as diferenças de tensão (resultantes da ação de ondas de choque causadas pela implosão de bolhas de cavitação) crítica projetada para cisalhamento de grãos com diferentes orientações. O dano ocorre preferencialmente em contornos de grãos com acentuados gradientes de tensão resolvida para a deformação plástica, onde se desenvolve elevada concentração de tensões. Em particular, os contornos de macla CSL 3 são acentuadamente mais suscetíveis à incubação do dano que os outros tipos de contornos CSL e que os contornos não CSL. / High nitrogen austenitic stainless steels containing 0.9 wt-% N and 20 wt- % N were tested in a ultrasonically induced vibratory cavitation testing device. Incubation times for damage initiation and mass losses were periodically measured during the cavitation-erosion tests. Scanning Electron Microscopy observation of the damaged surfaces allowed identifying the wear mechanisms operating during each step of the cavitation-erosion test. 0.9 wt-% N specimens were obtained through High Temperature Gas Nitriding UNS S31803 duplex stainless steel, at temperatures between 1050 and 1200 oC. Three groups of specimens were obtained: solubilized with all nitrogen in solid solution, solubilized and work hardened specimens and nitride containing specimens. The 20 wt- % N specimens were obtained through Low Temperature Plasma Nitriding the already High Temperature Gas Nitrided specimens and getting an expanded austenite layer at the surface. The specimens were firstly characterized by Electron Backscattered Diffraction - EBSD techniques and then submitted to the cavitation-erosion tests in distilled water. When compared to conventional UNS S30403 lean nitrogen solubilized austenitic stainless steel specimens, greater incubation times and smaller maximum wear rates were observed. The maximum wear rates (compared to those of the solubilized UNS S30403 steel) were: for the nitride containing specimen 6.9 times smaller; for textured and non-textured all nitrogen in solid solution specimens 26.8 and 25 times smaller, respectively; for the solubilized and work hardened specimen 145 times smaller; for the expanded austenite layer, with circa 20 wt- % N, specimens 300 times smaller. The beneficial effect of nitrogen on the cavitation-erosion resistance of the studied specimens was attributed to: (i) an increase in resistance to plastic deformation; (ii) a more homogeneous distribution of the plastic deformation; and (iii) an increase of the relative participation of energy consuming mass loss mechanisms. Plastic deformation accompanied by formation of micro relief at the surface and slip bands protrusions were clearly identified, during the first stages of cavitation erosion. The first evidences of mass loss (detected by SEM observations) were seen as particles detaching from micro cracks and micro pits formed at the grain surface. Nucleation and growth of cavitation damage was heterogeneously distributed at the grain scale. Slip bands protrusions, grain boundary protrusions and nitride matrix interfaces sites were more prone to nucleating the damage. Increasing nitrogen contents in solid solution increased the relative contribution of grain boundary nucleated damage, compared to the total amount of nucleation sites. Grains with 100 and 111 crystallographic planes approximately parallel to the surface were more prone to nucleation and growth of cavitation damage. Grains with 101 planes // surface were much more resistant to cavitation-erosion damage. These results are discussed considering differences of critical resolved shear stresses for grains with different orientations. Cavitation erosion damage occurs preferentially at grain boundaries across which steep stress gradients arise. Particularly, CSL -3 twin boundaries are much more susceptible to cavitation erosion damage incubation than other types of CSL boundaries and non CSL boundaries.

Le travail présenté dans ce manuscrit concerne la modélisation du comportementthermomécanique de films thermoplastiques déformés à l’état caoutchoutique. Lamodélisation du comportement des films amorphes isotropes est réalisée sur la base desmodèles de Lodge ou MSF. L’amélioration des prédictions des modèles pour destempératures de déformations proches de la température de transition vitreuse est possible enconsidérant dans le spectre des temps de relaxation des temps courts provenant de la zone detransition vitreuse. La modélisation du comportement de films amorphes anisotropes a étéeffectuée en considérant que l’anisotropie est due à une pré-déformation équivalente lors duprocédé de fabrication.Au cours de cette étude, les relations entre l’orientation de la phase cristalline et les propriétésmécaniques à température ambiante des films semi-cristallins ont été démontrées Au cours dela déformation à l’état caoutchoutique de ces films, la phase cristalline tend à s’orienterparallèlement à la direction de sollicitation par fragmentation des cristaux initiaux. En sebasant sur ces observations expérimentales, la modélisation du comportement mécanique desfilms semi-cristallins est possible en découplant les contributions en contrainte de la phasecristalline et de la phase. La réorientation des cristaux génère un phénomène de durcissementstructural sous contrainte qui peut être prédit par le modèle. / The work presented in this manuscript is devoted to the modeling of the thermomechanicalbehavior of polymer films deformed at the rubbery state. The modeling of the isotropicamorphous films is realized using the Lodge and the MSF models. For deformations appliednear the glass transition temperature, the predictions of these models are improved byincluding relaxation times coming from the glass transition domain in the spectra. Forpre-oriented amorphous films, the anisotropy is modeled by considering that it is due to aprevious equivalent deformation during the fabrication process.The relationship between the crystalline phase and the mechanical behavior at roomtemperature for the semi-crystalline films is established. During the deformation at therubbery sate of the semi-crystalline films, a reorientation of the crystalline phase occurs alongthe stretching direction. Based on the experimental observations, a semi-empirical model isdeveloped in order to describe the mechanical behavior of the semi-crystalline films. In thismodel, the contributions of both phases, amorphous and crystalline are separated. Thereorientation of the crystalline phase leads to a strain hardening stage which could bepredicted by the model

La miniaturisation des pièces est une étape importante pour la progression de la microtechnologie dans plusieurs domaines (connectique, médical, optique, microsystèmes mécaniques). Pour cela, le moulage par microinjection, semble être la solution clé pour la production à grande échelle de micro-composants de polymères. Pour les polymères semi-cristallins, la cristallisation, sous fort taux de cisaillement et sous des vitesses de refroidissement élevées (about 100 K/s), induit des morphologies et des propriétés spécifiques. Elle prend donc une importance considérable dans le processus de microinjection par rapport au moulage par injection classique où les épaisseurs injectées sont généralement supérieures à 1 mm. Ces microstructures ont une grande influence sur les propriétés mécaniques du produit final. La prédiction de ces propriétés à partir de la description de la microstructure est un défi technique et scientifique. Durant cette thèse, deux polymères semi-cristallins ont été microinjectés, le polyéthylène haute densité et le polyamide 12. Les analyses obtenues par la microscopie otiques montrent que les morphologies cristallines varient entre les micro- et les macro-pièces. Tandis que la morphologie de ‘peau-cœur' est présente dans les macropièces, les micropièces présentent une morphologie plutôt particulière. Les analyses combinées de diffusion et de diffraction des rayons X (SAXS et WAXS) avec un microfaisceau synchrotron, nous ont permis de déterminer la microstructure induite par le processus de microinjection dans toute l'épaisseur des pièces. Nous avons constaté que la morphologie et les orientations cristallines induites sont très dépendantes des conditions d'injection ou de microinjection. Une diminution de l'épaisseur, de la vitesse et de la température du moule, augmente l'orientation cristalline en limitant la relaxation des chaînes de polymères. / The components miniaturization is an important step in the evolution of micro technology in several domain (connectivity, medical, optical, mechanical, microsystems). For this purpose, the micro-injection molding seems to be the key solution for the large-scale micro-polymer components production.The crystallization of the semi-crystalline polymers under high shear and cooling rates (about 100 K / s), induces specific properties and morphologies, consequently, it takes a substantial importance in the process of micro-injection compared to conventional injection molding where the usually injected thicknesses is over 1 mm. These micro-structures have a great influence on the mechanical propertie of the final product. The prediction of the final product's properties based on the illustration of the micro-structure is a technical and scientific challenge. In this thesis, two semi-crystalline polymers were micro-injected, the high density polyethylene and the polyamide 12. The obtained analyzes with the use of an optical microscope showed that the Morphology of Crystals vary between micro-and macro-pieces. While the morphology of 'peau-cœur' is present in the macro-pieces, the micro-parts have a particular morphology. The combined analysis of diffusion and X-ray diffraction (WAXS and SAXS) along with the synchrotron microbeam, has allowed us to determined the micro-structure induced by the micro-injection process throughout the thickness of the pieces.We have identified that the morphology and the induced crystal's orientation are very dependent on the conditions of injection or micro-injection. The decrease of the thickness,speed and temperature of the mold will increase the crystal orientation by limiting the relaxation of the polymer chains.

Nach der Entwicklung des Nicht-Kontakt-Rasterkraftmikroskops (NC-AFM) konnten dessen Leistung, Empfindlichkeit und Anwendungsmöglichkeiten deutlich gesteigert und somit neue grundlegende physikalische Eigenschaften von Festkörperoberflächen mit hoher Auflösung und Präzision untersucht werden. Dabei gibt es jedoch immer wieder neue Errungenschaften, die die Technik noch weiter verbessern können – sei es auf dem Gebiet der Signalverarbeitung, der -detektion oder der prinzipiellen Funktionsweise des Mikroskops. So wird in der vorliegenden Arbeit das theoretische Verständnis der Regelkreise und des Rauschverhaltens des NC-AFMs im Messbetrieb verbessert. Die Regelkreise verhalten sich – anders als im freischwingenden System – in Wechselwirkungsnähe mit der Probe hochgradig dynamisch, sodass die ursprünglich gewählten Parameter der Regelkreise sich nicht eins zu eins auf den echten Messbetrieb übertragen lassen und suboptimale Einstellungen die Bildqualität dadurch beeinträchtigen können. Mithilfe der korrekten Modellierung der Regelkreise in Probennähe kann diese Störquelle nun minimalisiert werden, was durch experimentell bestimmte Spektren bestätigt wird. Bei der Exfoliation von Graphen auf CaF2 an der Raumluft werden Wassermoleküle eingeschlossen, die nicht durch Heizen entfernt werden können, ohne dass das Graphen Blasen schlägt und reißt. Unterschiedliche Mengen an Wasser zwischen den Graphenflocken und dem Substrat haben einen großen Einfluss auf das elektrische Kontaktpotenzial, das mithilfe der Kelvin-Sonden-Kraftmikroskopie vermessen werden kann. Ergebnisse der Kapitel sind die berechnete Adhäsionsenergie von Graphen auf CaF2, inwieweit das Wasser das Graphen dotieren kann und die Erklärung des großen Unterschieds des Kontaktpotenzials.

No description available.

In the presented thesis thin praseodymia films on non-passivated and passivated Si(111) substrates were investigated. The first part deals with PDA of praseodymia films with fluorite structure under UHV conditions in the temperature region from RT to 600°C. Here, a sophisticated model of the annealing process of praseodymia films is established. This is done by detailed analysis of XRD measurements using the kinematic diffraction theory in combination with the analysis of GIXRD, XRR and SPA-LEED measurements. It is shown that the untreated films, which are oxidized in 1 atm oxygen to obtain fluorite structure, do not exhibit pure PrO2 stoichiometry as it was assumed before. Instead, they decompose into two laterally coexisting species exhibiting a PrO2 and a Pr6O11. oxide phase, respectively. These species are laterally pinned to the lattice parameter of bulk Pr6O11. Homogeneous oxide films with Pr6O11 phase can be observed after annealing at 100°C and 150°C. Here, lateral strain caused by the pinning of the species is minimized and an increase of the crystallite sizes is determined. If higher annealing temperatures are applied, the film decomposes again into two coexisting species. Finally, after annealing at 300°C, a mixed crystalline film with both Pr2O3 and Pr2O3+Delta oxide phases is formed, where Delta denotes a considerable excess of oxygen within the sesquioxide phase. Again the lateral strain increases due to the tendency of praseodymia phases to increase their lattice parameters during oxygen loss combined with the lateral pinning. This is accompanied by a decrease of crystallite sizes, which are afterwards comparable to those of the untreated films. Further annealing at temperatures above 300°C does not significantly change the structure of the oxide film. However, the increase of the amorphous Pr-silicate interface between Si substrate and oxide at the expense of the crystalline oxide can be observed after annealing at higher temperatures. Furthermore, an increased mosaic spread of the crystallites occurs, which reduces the lateral strain caused by the oxygen loss. Nevertheless, the crystalline structure is stable against further annealing up to temperatures of 600°C. Transportation of the sample under ambient conditions after annealing at 200°C and 300°C leads to the formation of an additional crystalline structure at the surface which cannot be allocated to any praseodymia phase and may be explained by the contamination of the topmost crystalline layers with Pr-hydroxides. The results obtained from praseodymia films annealed in 1 atm nitrogen show that these films are good candidates to form homogeneous oxide films with pure cub-Pr2O3 structure by subsequent annealing in UHV. Here, a single oxide species is already observed after annealing at 300°C by SPA-LEED measurements which is in contrast to praseodymia films with fluorite structure where higher annealing temperatures (600°C) are necessary. In this case, negative effects like interface growth or increased defect density (mosaics, grain boundaries) can be minimized. Investigations on oxygen plasma-treated praseodymia films to obtain pure PrO2 stoichiometry are presented in the second part. Oxygen plasma-treated samples are compared with samples oxidized in 1 atm oxygen regarding the structure of the crystalline film. For this purpose, XRR and XRD measurements are performed to get structural information of the oxide film, which can be used to identify the corresponding oxide phases. Here, significantly smaller lattice constants of the crystalline oxide species can be observed after plasma treatment, which points to the incorporation of additional oxygen atoms. This verifies former studies, where a higher oxidation state of the oxide film was found by XPS measurements and it shows that plasma-treated films exhibit a higher oxidation state than films oxidized in 1 atm oxygen due to the availability of reactive atomic oxygen in the plasma. Furthermore, the Pr-silicate interface between crystalline film and Si substrate is not increased during plasma treatment. In the last part of the presented thesis, first results from the epitaxy of praseodymia films on Cl-passivated Si substrates are shown. The aim is to suppress the Pr-silicate formation during the growth process. Thus, praseodymia films are grown on passivated and non-passivated substrates to compare the crystallinity of both samples using XSW and LEED measurements. The structure of the oxide films on Cl-passivated Si is determined afterwards by XRR. It is shown that crystalline films with cub-Pr2O3 structure and several nanometer thickness can be successfully grown on Cl-passivated substrates. Here, the Pr-silicate interface layer are restricted to a single mono-layer. In contrast, the films grown on non-passivated substrates are completely amorphous containing Pr-silicates and Pr-silicides.

In this work the structural transitions of the rare earth oxides praseodymia and ceria grown on Si(111) are investigated. It is demonstrated that several of the rare earth intermediate phases can be stabilizied by post deposition annealing in ultra high vacuum. However, in most cases no single phased but coexisting species are observed. In addition, the surface structure and morphology of hex-Pr2O3(0001) as well as reduced ceria films are investigated.