The purpose of the work described in this thesis was to explore the use of fractional crystallization as a technology that can be used to separate medium-curie waste from the Hanford Site tank farms into a high-curie waste stream, which can be sent to a Waste Treatment and Immobilization Plant (WTP), and a low-curie waste stream, which can be sent to Bulk Vitrification. The successful semi-batch crystallization of sodium salts from two single shell tank simulant solutions (SST Early Feed, SST Late Feed) demonstrated that the recovered crystalline product met the purity requirement for exclusion of cesium, sodium recovery in the crystalline product and the requirement on the sulfate-to-sodium molar ratio in the stream to be diverted to the WTP. The experimental apparatus, procedures and results obtained in this thesis on scaled-down experiments of SST Early and Late Feed simulated solutions were adapted and reproduced under hot-cell with actual wastes by our partners at Hanford. To prepare the application of the pretreatment process to pilot scale process, several varation to the feed solutions were investigated including the presence of carboxylates and amines organics compounds and solids particles. Results of the study showed that 4 organics species presented complications to the process (NTA, HEDTA, EDTA and sodium citrate) while the other species (Formate, acetate, glycolate and IDA) and solids particles did not in the conditions of the stored wastes. In this thesis, the kinetics of the crystalline species formed at the condition of the early feed certification run (66 °C and 25 g/h evaporation) were determined along with the effect of the operating temperature and evaporation rate on these kinetics. On one hand, the study of evaporation rate values ranging from 25g/h to 75g/h showed that an increase in evaporation rate increased the specific nucleation while decreasing the specific growth rate. On the other hand, experiments on operating temperature ranging from 35 °C to 75 °C displayed that the nucleation rate of all species increased with temperature at the exception of sodium carbonate monohydrate and burkeite crystals, and that the growth rate of all species increased with temperature at the exception of sodium nitrate. Furthermore, sulfate based crystals such as trisodium fluoride sulfate were only roduced at 45 °C and 75 °C. A simple steady state MSMPR population balance model was developed expressing the total population density function as the sum of the specific population density functions. The specific semi-batch crystallization kinetics were implemented in this model.

In this work, atomic scale investigation of pressure-induced transformations in the solid state have been carried out. A series of compounds including GaN, ZnO, CaF2, and AgI, in addition to elemental phosphorus have been studied. The corresponding transition mechanisms have been elucidated with a clear description of atomic displacements and intermediate structures involved therein. In the first group of compounds, the long standing debate on the transition path of the wurtzite(WZ)-to-rocksalt(RS) transition in semiconductors, GaN and ZnO was resolved using geometrical modeling combined with molecular dynamics (MD) simulations conducted in the frame of transition path sampling (TPS) method. In GaN, a two-step mechanism through a metastable intermediate phase with a tetragonal structure iT has been revealed from simulations. In ZnO, the tetragonal intermediate structure was kinetically less stable, although still part of the real transition mechanism. It appeared at the interface between WZ and RS as consequence of a layers shearing. The transition regime in ZnO was characterized by a competition between iT structure and another hexagonal intermediate with hexagonal symmetry iH. Although possible, the latter is not functional for the transition. In both cases, GaN and ZnO, two points of agreement with experiments have been revealed. The tilting of structures after transition, and the phonon mode softening associated with atomic displacements leading to the tetragonal structure iT In the second group of compounds, the investigation of transitions in superionic conductors, CaF2 and AgI, demonstrated a different and particular behavior of atomic motion under pressure. The solid-solid reconstruction of CaF2 structure was shown to be initiated and precedented by high disorder of the anionic sublattice. The percolation of fluoride ions through voids in the fluorite structure created a thin interface of liquid like state. The sparce regions caused by the departure of anions facilitates the cation sublattice reconstruction. In AgI, ion diffusion during the wurtzite/zincnlende(ZB)$rocksalt transition was more pronounced due to the extended stacking disorder WZ/ZB. The Ag+ ions profited not only from the structure of the interface but used the combination of interstitial voids offered by both phases, WZ and ZB, to achieve long diffusion paths and cause the cation sublattice to melt. Clearly, a proper account for such phenomena cannot be provided by geometry-designed mechanisms based on symmetry arguments. In phosphorus, the question of how the stereochemically active lone pairs are reorganized during the orthorhombic (PI) to trigonal (PV) structural transition was answered by means of simulations. Computation was performed at different levels theory. First, the mechanism of the transition was obtained from TPS MD simulations. MD runs were performed within density functional tight binding method (DFTB). The analysis of atomic displacements along the real transformation path indicated a fast bond switching mechanism. In a second step, the nature of the interplay between orbitals of phosphorus during the bond switching was investigated. A simultaneous deformation of lone pair and P−P bond showed a mutual switching of roles during the transformation. This interplay caused a low dimensional polymerization of phosphorus under pressure. The corresponding structure formed as zigzag linear chain of fourfold coordinated phosphorus atoms (· · ·(P(P2))n · · ·) at the interface between PI and PV phases. A further result of this work was the development of a simulation strategy to incorporate defects and chemical doping to structural transformations. On top of the transition path sampling iterations, a Monte Carlo like procedure is added to stepwise substitute atoms in the transforming system. Introducing a chemically different dopant to a pure system represents a perturbation to the energy landscape where the walk between different phases is performed. Therefore, any change in the transition regime reflects the kinetic preference of a given structural motif at times of phase formation. This method was applied to the elucidation of WZ-RS transition mechanism in the series of semiconducting compounds AlN, GaN, and InN. Simulations showed that In atoms adopt the same transformation mechanism as in GaN and favor it, while Al atoms demonstrated a significant reluctance to the path going through tetragonal intermediate iT. The difference between transition regime in mixed systems InxGa1−xN and AlxGa1−xN is in agreement with experiments on high pressure behavior of AlN, GaN, and InN. While transitions in GaN and InN are reversible down to ambient conditions, AlN is stable. The work presented in this thesis constitutes the seed of new perspectives in the understanding of pressure-induced phase transformations in the solid state, where the physics and the chemistry are brought together by means of computer simulations.

No description available.

L’amélioration des performances des dispositifs photovoltaïques organiques passe par le contrôle de la morphologie de leurs couches actives. Nous avons cherché à préparer une hétérojonction volumique donneur-accepteur nanostructurée en utilisant la nucléation hétérogène du poly (3-hexylthiophène) (P3HT, donneur) par des fibres d’organogélateurs à base de naphthalène diimide (NDI, accepteur). La première partie de ce travail présente l’étude des propriétés d’auto-assemblage d’organogélateurs à cœur NDI substitué par des groupements amides et des dendrons trialkoxyphényles. Nous avons évalué l’influence de la longueur de la chaîne flexible entre le cœur naphthalène et les groupements amides (2 liaisons C-C pour NDI2 et 4 pour NDI4) sur les propriétés physico-chimiques des organogélateurs. La seconde partie de ce travail met en évidence le polymorphisme du composé NDI2 en identifiant 4 polymorphes ainsi que leurs signatures optiques, spectroscopiques et structurales. Un diagramme de phase de l’état solide du NDI2 est proposé. La dernière partie de la thèse concerne l’élaboration de nano-composites donneur-accepteur entre les organogélateurs à cœur NDI et le P3HT. Le processus de formation en solution de ces nano-composites est analysé en suivant les cinétiques de cristallisation du P3HT par spectroscopie d’absorption UV-Visible et les morphologies obtenues (structures shish-kebab) par microscopie électronique en transmission. L’effet nucléant des organogélateurs sur le P3HT a été montré. Les études en cellules solaires des composés P3HT:PCBM : organogélateur ont prouvé que le rendement de conversion énergétique peut être augmenté en présence d’organogélateurs. / Improving the performances of organic photovoltaic devices requires morphology control of the active layers. Highly nanostructured donor-acceptor bulk heterojunctions were prepared by heterogeneous nucleation of poly (3-hexylthiophene) (P3HT, donor) on naphthalene diimide organogelators fibers (NDI, acceptor). The first part of this work was dedicated to the self-assembly of NDI-core organogelators substituted by amide groups and trialkoxyphenyls dendrons. We evaluated the influence of the flexible chain between the naphthalene core and the amide groups (2 C-C bonds for NDI2 and 4 for NDI4) on the physico-chemical properties of the organogelators.The second part of this work focused on the polymorphism of NDI2 with identification of four different polymorphs with their optical, spectroscopic and structural signatures. A phase diagram of NDI2 in the solid state was determined. The last part of this manuscript concerns the fabrication of donor-acceptor nano-composites between NDI organogelators and P3HT. The formation process in solution of these nano-composites was analyzed by following the crystallization kinetics of P3HT by UV-Vis absorption spectroscopy and the thin film morphology (shish-kebab structures) by transmission electron microscopy. The nucleating effect of various organogelators on P3HT was demonstrated. Solar cells were made from the composites P3HT:PCBM : organogelator and their energetic conversion yield was shown to be increased in the presence of organogelators.

L’acier inoxydable est un alliage important pour le développement technique d’une société moderne; cela a été découvert au début du 20ème siècle. Cependant, leur système d'alliage de base, Fe-Cr, est affecté par une lacune de miscibilité à basse température (<600 °C) présent dans le diagramme de phases. Les alliages présentant une lacune de miscibilité dans leur diagramme de phase ont tendance à se décomposer. Ce phénomène également connu sous le nom de "fragilisation à 475 °C", est d’une importance technique, car la décomposition modifie les propriétés mécaniques de ces alliages; dans ce cas présente, par la perte de ductilité et de résistance aux chocs. La tendance à la décomposition augmente avec la diminution de la température, ce qui limite la température de service supérieure à environ 300 °C, limitant ainsi la durée de vie de ces alliages. Étant donné que la fragilisation peut provoquer une défaillance soudaine de ces alliages, cet aspect nuit à leur utilisation en tant que composants structurels dans les secteurs du transport et de l’énergie. La décomposition des alliages Fe-Cr pose un défi aux techniques de caractérisation traditionnelles, car les variations de composition se produisent à l'échelle nanométrique. Par conséquent, la sonde atomique tomographique de pointe a été utilisée pour étudier ces variations de composition à l'échelle atomique en 3D. La modélisation atomistique corrélative a été utilisée pour améliorer davantage la compréhension du processus de décomposition dans ces alliages ; ce modèle était basé sur la théorie de la fonction de densité atomique. Pour émuler la décomposition améliorée du matériau, causée par la température et/ou une charge externe, la décomposition dans ce projet est stimulée par une température de service supérieure à la normale. Dont la nécessité de connaître la limite exacte de la lacune de miscibilité. Ainsi, la nécessité d'évaluer la limite supérieure de température de cette décomposition dans le système Fe-Cr est née de résultats non concluants des analyses de la littérature existant. Par conséquent, un four de haute précision en combinaison avec une sonde atomique tomographique a été utilisé pour étudier la décomposition et l’agglomération dans le système Fe-Cr d’une manière plus précise que jamais. En outre, d’explorer en détail l’emplacement de la limite de la lacune de miscibilité. La décomposition de ces alliages au cours du vieillissement modifie les propriétés mécaniques. Ainsi, en raison de leur utilisation en tant que composants structurels, le comportement de décomposition dû au vieillissement a été étudié, ainsi que le vieillissement dû à la charge externe. Cette dernière situation se rencontre également dans des applications réelles pendant le service, émulées par le vieillissement dû à la pression en utilisant une simple force de traction. Afin d'examiner en détail l'effet de la pression externe, l'orientation du grain par rapport à la direction de traction a été prise en compte lors d'un simple vieillissement thermique et lors de l’application d’une force de traction continue. Ainsi, l'orientation cristallographique et les niveaux de charge ont été pris en compte pour leur effet sur le processus de décomposition/dégradation. / Stainless steel is an important alloy for the technical development of a modern society, they were discovered in the early 20th century. However, their base alloying system, Fe-Cr, is affected by a low temperature (<600°C) miscibility gap present in the phase diagram. Alloys with a miscibility gap in their phase diagram tend to decompose. This phenomenon is also known as the “475°C embrittlement”, it is of technical importance as decomposition alters the mechanical properties of these alloys, in this specific case, by loss of ductility and impact toughness. The tendency to decompose increases with decreasing temperature, restricting the upper service temperature to around 300°C and limiting the service lifetime of these alloys. Because embrittlement can cause sudden failure of these alloys, this phenomenon is detrimental to their use as structural components in transportation and energy industry. The decomposition of Fe-Cr alloys poses a challenge for traditional characterisation techniques, as composition variations occur at the nanoscale. Therefore, the state-of-the-art atom probe tomography have been utilised to study these composition variations at the atomic scale in 3D. Correlative atomistic modelling has been used to further enhance the understanding of the decomposition process in these alloys, this model was based on atomic density function theory. To emulate enhanced decomposition of the material, caused by temperature and/or an external load, decomposition in this work is stimulated by a higher than the normal service temperature. Hence, a need to know the exact limit of the miscibility gap. Thus, a need to evaluate the upper-temperature limit of this decomposition in the Fe-Cr system arose from inconclusive results in the literature. Hence, a high precision furnace in combination with atom probe was utilised to study decomposition and clustering in the Fe-Cr system more accurately than ever before. Furthermore, to explore in detail the location of the limit of the miscibility gap. The decomposition of these alloys during ageing alter the mechanical properties. Thus, due to their use as structural components, the decomposition behaviour during ageing was investigated, as well as ageing during external load. This last situation is also encountered in real applications during service, mimicked by stress-ageing using a simple tensile force. In order to in detail investigate the effect of the external stress, grain orientation with respect to the tensile direction was considered during simple thermal ageing, and during the constantly applied tensile force. Thus, crystallographic orientation and load levels were considered for their effect on the decomposition process.

In this work, atomic scale investigation of pressure-induced transformations in the solid state have been carried out. A series of compounds including GaN, ZnO, CaF2, and AgI, in addition to elemental phosphorus have been studied. The corresponding transition mechanisms have been elucidated with a clear description of atomic displacements and intermediate structures involved therein. In the first group of compounds, the long standing debate on the transition path of the wurtzite(WZ)-to-rocksalt(RS) transition in semiconductors, GaN and ZnO was resolved using geometrical modeling combined with molecular dynamics (MD) simulations conducted in the frame of transition path sampling (TPS) method. In GaN, a two-step mechanism through a metastable intermediate phase with a tetragonal structure iT has been revealed from simulations. In ZnO, the tetragonal intermediate structure was kinetically less stable, although still part of the real transition mechanism. It appeared at the interface between WZ and RS as consequence of a layers shearing. The transition regime in ZnO was characterized by a competition between iT structure and another hexagonal intermediate with hexagonal symmetry iH. Although possible, the latter is not functional for the transition. In both cases, GaN and ZnO, two points of agreement with experiments have been revealed. The tilting of structures after transition, and the phonon mode softening associated with atomic displacements leading to the tetragonal structure iT In the second group of compounds, the investigation of transitions in superionic conductors, CaF2 and AgI, demonstrated a different and particular behavior of atomic motion under pressure. The solid-solid reconstruction of CaF2 structure was shown to be initiated and precedented by high disorder of the anionic sublattice. The percolation of fluoride ions through voids in the fluorite structure created a thin interface of liquid like state. The sparce regions caused by the departure of anions facilitates the cation sublattice reconstruction. In AgI, ion diffusion during the wurtzite/zincnlende(ZB)$rocksalt transition was more pronounced due to the extended stacking disorder WZ/ZB. The Ag+ ions profited not only from the structure of the interface but used the combination of interstitial voids offered by both phases, WZ and ZB, to achieve long diffusion paths and cause the cation sublattice to melt. Clearly, a proper account for such phenomena cannot be provided by geometry-designed mechanisms based on symmetry arguments. In phosphorus, the question of how the stereochemically active lone pairs are reorganized during the orthorhombic (PI) to trigonal (PV) structural transition was answered by means of simulations. Computation was performed at different levels theory. First, the mechanism of the transition was obtained from TPS MD simulations. MD runs were performed within density functional tight binding method (DFTB). The analysis of atomic displacements along the real transformation path indicated a fast bond switching mechanism. In a second step, the nature of the interplay between orbitals of phosphorus during the bond switching was investigated. A simultaneous deformation of lone pair and P−P bond showed a mutual switching of roles during the transformation. This interplay caused a low dimensional polymerization of phosphorus under pressure. The corresponding structure formed as zigzag linear chain of fourfold coordinated phosphorus atoms (· · ·(P(P2))n · · ·) at the interface between PI and PV phases. A further result of this work was the development of a simulation strategy to incorporate defects and chemical doping to structural transformations. On top of the transition path sampling iterations, a Monte Carlo like procedure is added to stepwise substitute atoms in the transforming system. Introducing a chemically different dopant to a pure system represents a perturbation to the energy landscape where the walk between different phases is performed. Therefore, any change in the transition regime reflects the kinetic preference of a given structural motif at times of phase formation. This method was applied to the elucidation of WZ-RS transition mechanism in the series of semiconducting compounds AlN, GaN, and InN. Simulations showed that In atoms adopt the same transformation mechanism as in GaN and favor it, while Al atoms demonstrated a significant reluctance to the path going through tetragonal intermediate iT. The difference between transition regime in mixed systems InxGa1−xN and AlxGa1−xN is in agreement with experiments on high pressure behavior of AlN, GaN, and InN. While transitions in GaN and InN are reversible down to ambient conditions, AlN is stable. The work presented in this thesis constitutes the seed of new perspectives in the understanding of pressure-induced phase transformations in the solid state, where the physics and the chemistry are brought together by means of computer simulations.

This work investigates the growth dynamic of the reactive molecular beam epitaxy of Fe3O4 films, and its impact on the cation distribution as well as on the magnetic and structural properties at the surface and the interfaces. In order to study the structure and composition of Fe3O4 films during growth, time-resolved high-energy x-ray diffraction (tr-HEXRD) and time-resolved hard x-ray photoelectron spectroscopy (tr-HAXPES) measurements are used to monitor the deposition process of Fe3O4 ultrathin films on SrTiO3(001), MgO(001) and NiO/MgO(001). For Fe3O4\SrTiO3(001) is found that the film first grows in a disordered island structure, between thicknesses of 1.5nm to 3nm in FeO islands and finally in the inverse spinel structure of Fe3O4, displaying (111) nanofacets on the surface. The films on MgO(001) and NiO/MgO(001) show a similar result, with the exception that the films are not disordered in the early growth stage, but form islands which immediately exhibit a crystalline FeO phase up to a thickness of 1nm. After that, the films grown in the inverse spinel structure on both MgO(001) and NiO/MgO(001). Additionally, the tr-HAXPES measurements of Fe3O4/SrTiO3(001) demonstrate that the FeO phase is only stable during the deposition process, but turns into a Fe3O4 phase when the deposition is interrupted. This suggests that this FeO layer is a strictly dynamic property of the growth process, and might not be retained in the as-grown films. In order to characterize the as-grown films, a technique is introduced to extract the cation depth distribution of Fe3O4 films from magnetooptical depth profiles obtained by fitting x-ray resonant magnetic reflectivity (XRMR) curves. To this end, x-ray absorption (XAS) and x-ray magnetic circular dichroism (XMCD) spectra are recorded as well as XRMR curves to obtain magnetooptical depth profiles. To attribute these magnetooptical depth profiles to the depth distribution of the cations, multiplet calculations are fitted to the XMCD data. From these calculations, the cation contributions at the three resonant energies of the XMCD spectrum can be evaluated. Recording XRMR curves at those energies allows to resolve the magnetooptical depth profiles of the three iron cation species in Fe3O4. This technique is used to resolve the cation stoichiometry at the surface of Fe3O4/MgO(001) films and at the interfaces of Fe3O4/MgO(001) and Fe3O4/NiO. The first unit cell of the Fe3O4(001) surface shows an excess of Fe3+ cations, likely related to a subsurface cation-vacancy reconstruction of the Fe3O4(001) surface, but the magnetic order of the different cation species appears to be not disturbed in this reconstructed layer. Beyond this layer, the magnetic order of all three iron cation species in Fe3O4/MgO(001) is stable for the entire film with no interlayer or magnetic dead layer at the interface. For Fe3O4/NiO films, we unexpectedly observe a magnetooptical absorption at the Ni L3 edge in the NiO film corresponding to a ferromagnetic order throughout the entire NiO film, which is antiferromagnetic in the bulk. Additionally, the magnetooptical profiles indicate a single intermixed layer containing both Fe2+ and Ni2+ cations.