Made available in DSpace on 2014-10-09T12:51:20Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:03:31Z (GMT). No. of bitstreams: 0 / Fez-se a separação, enriquecimento e purificação de iantânio e ítrio partindo-se de um concentrado de terras raras empobrecido em cério, conhecido como LCC, \"low cerium carbonate\", um concentrado de ítrio designado como \"carbonato de ítrio\" e um terceiro concentrado designado como \"oxido de terras ítricas\". Os dois primeiros concentrados foram produzidos industrialmente pela NUCLEMON - Nuclebrás de Monazita e Associados Ltda, usando monazita brasileira. O \"oxido de terras ítricas\" é proveniente do processo de obtenção de Iantânio durante a execução do trabalho experimental desta tese. Fez-se uso das seguintes tecnologias: 1) precipitação fracionada com uréia; 2) lixiviação fracionada do LCC com carbonato de amônio e 3) precipitação dos peroxicarbonatos de terras raras usando-se seus carbonatos complexos. Obtidas frações enriquecidas em terras raras estas foram refinadas por meio de tecnologia de troca iônica em leito de resina catiônica sem uso de ion retentor e eluição com sais de amônio do ácido etilenodiaminotetraacético. Com a associação das técnicas acima mencionadas foram obtidos óxidos puros de ítrio (>97,7%), oxido de Iantânio (99,9%), óxido de gadolínio (96,6 %) e oxido de samário (99,9%). O processo aqui desenvolvido tem viabilidade técnica econômica para a instalação de uma unidade de maior porte visando a industrialização. / Tese (Doutoramento) / IPEN/T / Instituto de Pesquisas Energeticas e Nucleares - IPEN/CNEN-SP

The structural properties of the very neutron deficient systems around N~Z~40 have been studied in two experiments performed at the GANIL and Legnaro laboratories. The fragmentation of a 60 MeV/u92 Mo beam on a natural nickel target at the GANIL Laboratory, France, produced exotic nuclei along the proton drip line in the mass 80 region. Isomeric decays have been observed for the first time in the N=Z+2 systems 74 36Kr, 80 39Y and 84 41Nb. The isomer in 74 Kr is interpreted as the hindered decay from an excited 0+ state, supporting the long-standing prediction of prolate/oblate shape coexistence in this nucleus. Transitions from states below an isomer in the N=Z nucleus 86 43Tc have also been tentatively identified, making this the heaviest N=Z system for which gamma-ray decays from excited states have been observed. Conclusive evidence for the existence of the Z=N+1 isotopes 77 39Y, 79 40Zr and 83 42Mo has also been obtained together with upper limits on the particle decay lifetimes of the odd-proton systems 81 41 Nb and 85 43Tc. The reported instability of the lighter odd-Z, Tz = -1/2 systems 69Br and 73Rb makes the observed existence for 77 39Y particularly interesting. A possible explanation for the relative particle stability of 77 39Y is given in terms of the shape polarising effect of the N=Z=38 prolate shell gap on the nuclear mean field and the increased centrifugal barrier associated with the occupation of a g9/2 proton orbital. The second experiment was performed to further investigate the oblate nature of the isomeric state in 74Kr. The reaction 40Ca(40Ca, alpha2p)74Kr was used at a beam energy of 135 MeV obtained from the Tandem XTU accelerator. The EUROBALL gamma-ray array was used in conjunction with the ISIS charged particle silicon ball to study the states above and below the isomer. The ISIS ball was used to highlight channel selection of non-yrast states by particle gating. No evidence for the 0+2 isomer in 74Kr was observed in this work.

Ziel dieser Doktorarbeit war es, den Einfluss von verschiedenen Parametern auf die spektroskopischen Eigenschaften von Lanthanid-basierten Aufkonversions-Materialien zu erforschen. Ein besonderer Fokus lag dabei auf hexagonalen Natrium-Yttrium-Tetrafluorid Kristallen, die mit dreifachgeladenen Yb und Er oder Tm Ionen kodotiert wurden. Eine wesentliche Voraussetzung für mögliche Anwendungen dieser Kristalle ist ein Verständnis aller ihrer wichtigen photophysikalischen Besonderheiten. Die erste Studie dieser Doktorarbeit untersuchte daher, wieso Nanokristalle viel weniger absorbierte in ausgesendete Photonen umwandeln als mikrokristalline Teilchen. Die Ergebnisse zeigten, dass man ungeschalte Kristalle aufgrund von Oberflächen-Lösch-Effekten in zwei Teile unterteilen kann, einen strahlenden Kern und eine Schale aus stark oder vollständig gelöschten oberflächennahen Lanthanid-Ionen, welche für Kristalle abnehmender Größe einen immer größeren Volumenanteil einnimmt. Die zweite Studie untersuchte exemplarisch, ob eine kompliziertere Partikelarchitektur, bestehend aus einem einfach-dotierten Er Kern und Yb als Schalenmaterial, diesen Effizienzverlust der Lumineszenz reduzieren kann. Die Ergebnisse zeigten jedoch, dass dies nicht der Fall ist. Eine weitere Studie untersuchte den Einfluss der Konzentration der Tm Ionen in Yb, Tm kodotierten Nanokristallen auf die spektroskopischen Eigenschaften dieser Materialien und zeigte, dass für eine maximale Emission im Lichtwellenbereich über 700 nm andere Tm Konzentrationen benötigt werden als für maximale Lichtemissionen in den unteren Lichtwellenbereichen. Die letzte Studie untersuchte den Einfluss eines zuvor berichteten Zersetzungsprozesses von exemplarisch ausgewählten Yb, Tm kodotierte Nanokristallen in wässrigen Dispersionen auf deren spektroskopische Eigenschaften. Mithilfe dieser Ergebnisse war es möglich, mehrere Emissionsbanden als Parameter für das Langzeit-Stabilitäts-Monitoring dieser Materialien zu identifizieren. / This PhD thesis investigated the influence of various parameters on the spectroscopic properties of so-called upconversion nanoparticles (UCNPs). A special emphasis was dedicated to hexagonal-phase sodium yttrium tetrafluoride crystals that were codoped with trivalent Yb and either Er or Tm ions. Such UCNPs can, however, experience no breakthrough in the field of UC nanotechnology before all of their important photophysical features are understood. The first study of this PhD thesis therefore investigated, why nanocrystalline upconverters with different surface chemistries convert less absorbed to emitted photons than their microcrystalline counterparts. The results revealed that upconverting crystals apparently have to be subdivided into two parts, with one being the luminescent core and the other being a completely dark shell that is quenched by surface effects and assumes an ever increasing volumetric content for small UCNPs. The second study exemplarily investigated, if a more complex particle nanostructure that consisted of a Er doped core, surrounded by a Yb doped shell, could overcome these efficiency losses, however, it concluded that it does not. Another study explored the influence of Tm doping concentrations of Yb, Tm codoped nanocrystals on their spectroscopic properties and concluded that different Tm doping concentrations are required for a maximum upconversion luminescence in the wavelength regions above 700 nm, than for the wavelength regions below that. The last study of this PhD thesis investigated the influence of a previously reported dissolution process of UCNPs in aqueous solutions on the spectroscopic properties of exemplarily chosen Yb, Tm codoped nanocrystals. These results were then utilized to identify several upconversion emission bands that can be used as a screening parameter for the long-term stability monitoring of UCNPs.

Cette thèse est dédiée à l’étude des interactions entre les défauts lacunaires et les solutés (Y, Ti, O) pour mieux comprendre la formation des nanoparticules d’oxyde dans les aciers ODS (Oxide Dispersion Strengthened). Ces aciers sont envisagés comme matériau de structure dans la prochaine génération de réacteurs nucléaires fission et fusion. Leurs bonnes propriétés reposent essentiellement sur une répartition homogène de nanoparticules (YxTiyOz) de très faible taille. Cependant, l’obtention de cette répartition n’est pas encore maitrisée et le mécanisme de formation de ces nanoparticules n’est pas encore bien défini. Des modèles théoriques montrent que la présence de lacunes pendant l’étape de broyage pourrait impacter la formation de ces nanoparticules. Cette étude fait suite à la thèse de C. He et apporte de nouveaux résultats et de nouvelles interprétations et conclusions. Des implantations avec des ions Y, Ti, O ont été réalisées afin de simuler l’étape de broyage de ces aciers ODS. Elles ont permis d’introduire des défauts et les solutés désirés dans la matrice de fer α. Nous avons ensuite étudié les interactions entre les solutés et les défauts générés dans la matrice. La nature des défauts induits a été étudiée en fonction de l’ion implanté et de traitements thermiques après implantation par spectroscopie d’annihilation de positons (PAS) et corrélée avec les profils en profondeur des solutés obtenus par spectrométrie de masse des ions secondaires (SIMS). Les caractéristiques d’annihilation de certains défauts encore inconnues ont pu être déterminées. Les mesures SIMS ont montré que le titane ne migre pas entre 100 et 450°C et que l’oxygène présente un comportement complexe de migration et de piégeage dépendant de la température et de la microstructure des matériaux. Les résultats PAS montrent que les implantations ioniques conduisent à la formation de clusters lacunaires, de complexes lacunes-solutés et de dislocations dont la proportion change en fonction de la profondeur et de la nature de l’ion implanté. Les clusters de lacunes Vn et les dislocations sont détectés au-delà du pic d’implantation avec une fraction plus importante pour les dislocations indiquant que les défauts ont pu migrer pendant l’implantation. La proportion des complexes lacunes-solutés est maximale dans la zone d’arrêt des ions. Elle est en accord avec les énergies de liaison théoriques des complexes lacunes-soluté. La nature et la distribution des défauts formés évoluent en fonction de la température de recuit. Les clusters lacunaires Vn disparaissent entre RT et 300°C alors que les dislocations sont éliminées à partir de 400°C. Des phases oxydes sont détectées pour des recuits à 500 et 550°C en lien avec la contamination en oxygène. Des défauts dont la nature est non identifiée ont été mis en évidence pour des recuits réalisés entre 300 et 400°C dans les implantations O, Y et Y+O. / This PhD thesis is dedicated to the study of interaction between vacancies and Y, Ti,O solutes for a better understanding of formation of oxide nanoparticles in ODS steel (Oxide Dispersion Strengthened). These ODS steels are considered as structural material for the next generation of fission and fusion nuclear reactors. Their good properties are induced by the fine dispersion of low size oxide nanoparticles. However, obtaining this distribution is not mastered and atomic scale clustering is not yet defined. Furthermore, it was shown by theoretical models that the presence of vacancy during mechanical alloying could affect the formation of these nanoparticles. This study follows upon on a previous study made by C.He, and bring new results, new interpretation and conclusions. Some implantations with Y, Ti, O ions with several energy have been made in order to simulate the mechanical alloying step used for ODS steel fabrication. Theses irradiations have induced defects and solutes into the iron matrix. Then we characterized samples using positron annihilation spectroscopy (PAS) and secondary ion mass spectrometry (SIMS). The nature of defects was studied according to nature of the implanted ion and the annealing temperature by PAS and correlated to depth profiles of solutes obtained by SIMS. Annihilation characteristics of some defects still unknown were able to be determined thanks to positron lifetime measurements. SIMS analysis showed that titanium doesn’t migrate for annealing experiments between 100°C and 450°C and that oxygen show a complex behavior of migration and trapping dependent on the microstructure of the material. PAS results show that ionic implantations produce vacancy clusters, dislocations and solutes-vacancies complex. Their proportion changes as a function of depth and nature of these irradiations. Vacancy clusters and dislocations are detected deeper than the implantation peak with a higher fraction for the dislocations indicating that the defects were able to migrate during implantations. The fraction of vacancy-solutes complexes is the highest in the ion stopping zone and is in a good agreement with the theoretical binding energy of vacancies-solutes complex. The nature and the distribution of the defects evolve according to the annealing temperature. Vacancy clusters disappear between RT and 300°C while the dislocations are eliminated from 400°C. Oxide phases are detected for annealing at 500 and 550°C in relation with the oxygen contamination during these annealings. Some defects which the nature is not yet identified were highlighted for annealing between 300 and 400°C for Y, O and Y+O irradiations

In the last decade new materials appeared that are candidates to be used as an electrolyte in a Solid Oxide Fuel Cell, SOFC. Some materials show high ionic conductivity but lack in important properties, such as mechanical stability or chemical compatibility with other materials in the fuel cell. Scandia Stabilised Zirconia, SSZ, became a possibility when the scandia price dropped with the opening of the Chinese and Russian markets. In the starting system Ce[subscript(x)]Y[subscript(0.2-x)]Sc₀.₆Zr₃.₂O[subscript(8-δ)], (0≤x≤0.2), scandia is introduced to improve conductivity and stabilise the cubic phase; yttria is introduced to fully stabilise the cubic phase and ceria to enhance conductivity lost with the introduction of yttria. The aim of this project is to develop a reliable new method to produce quality ceramics that are not strongly composition dependent, then to prepare a range of compositions and compare intrinsic properties without having to be concerned that poor sintering dominates conduction properties. This project can be divided in two sections, the first section the powder production method, the characteristics of the powders and its final products are in focus. In the second section the relation between electric characteristics and microstructure of the material is reported. In the first section, the effect of different compositions of the system Ce[subscript(x)]Y[subscript(0.2-x)]Sc₀.₆Zr₃.₂O[subscript(8-δ)], (0≤x≤0.2) is studied, in terms of structure, phase and microstructure. The nature, size and shape of the powders are discussed, and their effect on the final product. The sol-gel and combustion method gives the formation of hard agglomerates (shells), during the combustion, a wide range of grain sizes, between less than 1µm and 200 µm, and the formation of grains with non spherical shape. In this project, the sol-gel and combustion process and solid state method are also compared. In the second section of this project, AC Impedance measurements, as a function of temperature, oxygen partial pressure and time are discussed. The Arrhenius plot for all compositions shows two regions (high and low temperature) and the change of region occurs at 580 °C. At low temperatures there is a slight difference between compositions but this difference is less at high temperatures. The obtained ionic conductivity, at 350 °C, varies from 3.84×10⁻⁶ to 5.53×10⁻⁵ S/cm; at 700 °C, ionic conductivity from 0.013 to 0.044 S/cm. At low temperatures, the activation energy associated with bulk process is generally lower than grain boundary process; for example, the composition Ce₀.₁Y₀.₁Sc₀.₆Zr₃.₂O₇.₆₅ has an activation energy, for the bulk process, of 1.05 eV and an activation energy, for the grain boundary process, of 1.17 eV. For compositions with higher ceria content, activation energy, for bulk and grain boundary, have similar values. The AC impedance as function of oxygen partial pressure show that the amount of ceria introduced as an effect on the conductivity at low oxygen partial pressure. For the sample with no ceria in its composition, Y₀.₂Sc₀.₆Zr₃.₂O₇.₆₀, the conductivity does not vary significantly as the oxygen partial pressure is decreased; for oxygen partial of 0.21 atm, conductivity is 0.018 S/cm and when oxygen partial pressure is approximately 10⁻²⁴ atm conductivity is 0.018 S/cm. For the sample with a higher content of ceria, Ce₀.₁₂Y₀.₀₈Sc₀.₆Zr₃.₂O₇.₆₆, there is a decrease in conductivity while oxygen partial pressure decreases; and there is also the appearance of a semi-circle for lower oxygen partial pressures. For oxygen partial pressure approximately 0.21 atm, conductivity is 0.019 S/cm, but when oxygen partial pressure is decreased to 10⁻²⁴ atm conductivity decreases to 0.011 S/cm. AC impedance measurements as a function of annealing time at 600 °C were performed. Total conductivity is fairly stable, for all compositions, until 1800 hours but after this time, conductivity slowly decreases. Some compositions show a second semi-circle in the AC impedance spectra, either from the beginning, time equals 0 hours, or after some working hours. Here, the changes in conduction and conduction processes with time are discussed.

Ce travail s'inscrit dans un cadre de recherches qui a pour objectif essentiel l'étude de l'effet des éléments réactifs sur l'oxydation à haute température (1373 K) d'alliages alumino-formaurs de type FeCrAl. Un alliage modèle, ne contenant pas d'éléments mineurs d'addition, a été utilisé pour cette étude. L'originalité de cette étude réside dans l'utilisation de la technique de revêtement sol-gel contenant le lanthane, le cérium ou l'yttrium. Les échantillons revêtus de sol-gel ont été recuits sous argon aux températures de 600, 800 et 1000°C. Les tests de cyclage thermiques montrent que les dépôts sol-gel de lanthane recuits à 1000°C et de cérium recuits à 600°C apportent une protection efficace à l'alliage. Le dépôt sol-gel d'yttrium n'a pas d'effet bénéfique sur le comportement à haute température même après recuit sous argon. L'analyse par la thermogravimétrie (ATG) montre que les recuits sous argon provoquent les prises de masse les plus importantes. Ceci est dû à l'augmentation de la diffusion anionique au stade initial de l'oxydation. L'utilisation de la DRX in situ nous permet de suivre l'évolution des réactions d'oxydation en identifiant les phases formées sur la surface des alliages. Après recuit ou exposition à 1100°C, le lanthane peut former des oxydes mixtes avec l'aluminium : LaAlO3 et LaAl11O18, le cérium ne forme aucun oxyde mixte avec les éléments d'alliages. L'yttrium est l'élément qui a l'affinité avec l'alumine la plus élevée. Pendant les recuits ou expositions à 1100°C, il peut former des oxydes mixtes avec l'aluminium : YAlO3 et Y3Al5O12. Les micro-observations montrent que la couche d'alumine développée sur l'alliage recouvert des dépôts sol-gel est généralement convolutée. Cette morphologie est le résultat de la formation des nouveaux oxydes dans la couche existante dû à un processus de diffusion mixte. Cette étude montre que les éléments réactifs lanthane, cérium et yttrium se localisent toujours à l'interface externe de la couche d'oxyde.

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