Thesis (M.S. in Physics)--United States Naval Postgraduate School, California. / Includes bibliographical references (p. 23). 9

The present work is focused on the nucleation and growth mechanism of carbon nanotubes (CNT) that we have studied through different field emission techniques (FEM, FIM and atom-probe (PFDMS)). Reaction conditions associated with the CVD synthesis method were modeled inside the microscope aiming at studying nucleation phenomena at high resolution. The interaction between different metals (Fe, Co, Ni, conditioned as sharp tips) and gases (acetylene, ethylene and ethanol) was analyzed operando at high temperatures (500–900K), with the aim of reproducing growth conditions during the imaging process. Ni was, in the end, the only metal studied, due to the poor quality of images acquired from Co and Fe. Aimed at reproducing the conditioning step of the catalyst often observed in CVD protocols, a first study showed that the crystal adopts a polyhedral morphology at the working temperature (873K) in an hydrogen atmosphere or under Ultra-High-Vacuum conditions, by the extension of dense crystal planes like {111} or {100}. The presence of hydrogen in the chamber does not seem to present any influence on the final crystal morphology at temperatures above 600K. When exposed to a carbon-containing gas, nickel crystals present two distinct behaviors following the temperature region that is explored. At temperatures below ~623K, exposing Ni to ethylene or acetylene leads to the formation of a stable and poorly structured nickel carbide layer. The superficiality of this carbide is proven by the ease of its physical (by increasing the electrical field) or chemical (exposure to hydrogen or oxygen) evacuation. These three treatments initiate a clean-off phenomenon that evacuates the carbide layer. Reproducing these experiments in the atom-probe confirmed the carbidic nature of the surface as NiCy compounds were collected. At temperatures above 623K, the carbide layer (formed by exposing Ni to the same gases) becomes unstable. Its formation is related to a transition period that precedes the nucleation of graphenes on the surface. The Ni crystal undergoes a massive morphological transformation when acetylene is introduced in the chamber at 873K. This phenomenon is induced by the presence of carbon on the surface which adsorbs so strongly on step sites that it provokes their creation. Carbon also induces a considerable enhancement of Ni atoms mobility that allows for this transition to occur. Once the new morphology is attained, nucleation of graphenes is observed to start on the extended and carbon-enriched step-containing crystal planes. By reproducing these experiments in the atom-probe, a high surface concentration of carbon dimers and trimers was observed. A kinetic study of their formation was thus achieved and showed that they were formed on the surface by the recombination of Cad. Their potential role as building-blocks of the CNT growth process (which had previously been proposed following theoretical considerations) is thus suggested on the basis of experimental results for the first time. Two critical surface concentrations are highlighted in the present work. The first one is needed for the formation of carbon dimers and trimers and the second one has to be attained, during the morphological transformation, before the onset of graphene nucleation, probably providing a sufficient growth rate of the graphitic nuclei and allowing them to attain their critical size before their decomposition. Finally, the observation of rotational circular patterns, most probably related to carbon nanotubes, suggests that CNT growth (and not only graphene nucleation) occurred episodically in our conditions, confirming the validity of our model.

Thesis (Ph. D.)--University of Washington, 1998. / Vita. Includes bibliographical references (leaves 128-129).

Thesis (Ph. D.)--Brigham Young University. Dept. of Chemistry and Biochemistry, 2007. / Includes bibliographical references.

A unique Raman spectroscopic investigation combining a number of different techniques has been conducted in situ on the composition of the passive film on iron, both during its growth in 0.05 M NaOH by potentiodynamic polarization and during localized breakdown by pitting after addition of 0.05 M NaCl. There are differing theories for the mechanism of pit initiation and formation in the passive film on iron, and while these are in part due to different environmental factors, they are also influenced by differing theories for the nature of the passive film. The detailed information obtained in this study corroborate the two layer model for the passive film on iron, with γ-Fe2O3 forming the inner layer and the outer layer consisting of δ-FeOOH, α-FeOOH, γ-FeOOH, other components such as Fe(OH)2 and other intermediates. In the passive region of anodic polarization the film became increasingly hydrated with increasing anodic potential and with increased cycles became amorphous, comparing well with the Hydrated Polymeric Oxide model. Pre-resonance enhancement of the Raman bands of iron oxides and particularly iron oxy-hydroxides was afforded by excitation at 636.4 nm, and particularly at low wavenumbers. The use of Multivariate Curve Resolution with Alternating Least Squares (MCR-ALS) enabled determination of the relative amounts of the iron oxide and oxy-hydroxide components from the complex spectra recorded during potentiodynamic polarization. The amount of water incorporated in the passive film under the same conditions was also monitored in situ at similar potentials using excitation at 514.5 nm. Addition of chloride ions resulted in an increase in hydration and a change of the composition of the passive film to comprise mainly β-FeOOH and Green complex with some γ-Fe2O3 and γ-FeOOH. At the pitting potential significant changes in the composition occurred along with reduction in hydration, so that re-passivation could no longer be maintained at the same rate as dissolution by the chloride ions, enabling stable pitting. These observations indicate that water plays a protective role in the passive film and reinforce the mechanisms for pit initiation based on the De-passivation–Re-passivation theory and Chemical Dissolution theory.

Ce travail de thèse propose une investigation des dynamiques régissant la réactiond’hydrogénation du dioxyde de carbone sur une nanoparticule modèle de rhodium àl’échelle moléculaire. Cette recherche s’inscrit dans le contexte de la valorisation du CO2 parla voie catalytique. Une meilleure compréhension de la relation entre la structurecristallographique de la surface et les mécanismes réactionnels permettrait, à terme,d’améliorer l’optimisation des matériaux catalytiques. Dans ce but, la réaction est étudiée àl’échelle moléculaire sur une nanoparticule modèle de rhodium. Sa surface est observée àl’aide de l’ensemble des techniques d’émission de champ :la microscopie d’émission dechamp (FEM), la microscopie ionique à effet de champ (FIM), la sonde atomique unidimensionnelle(1DAP) et la sonde atomique tomographique (APT). Afin d’identifier lesdifférents phénomènes observés, ces derniers sont comparés à d’autres systèmes réactifsimpliquant l’O2, le N2O et le CO, sur du rhodium, du platine et un alliage de platine rhodium(10% en masse de rhodium).Dans ce travail nous avons observé et caractérisé l’adsorption dissociative du CO2 sur lerhodium et sa réaction avec l’hydrogène. À l’aide d’études comparatives avec les autressystèmes, des phénomènes réactifs ont été identifiés. Les traitements des donnéesrecueillies indiquent qu’à 700 K, les gaz CO2 et H2 réagissent via un processus en surface etforment les produits CO(g) et H2O(g). Cette réaction est connue sous le nom de « réaction dugaz à l’eau inverse ». Cette réaction s’accompagne de transformations observables par FEM.La présence d’atomes d’oxygène adsorbés provoque une augmentation du travail de sortiedes électrons de la plupart des facettes cristallographiques de la surface de rhodium, ce quise traduit par un assombrissement global de l’image FEM. Cependant, certaines régionsparticulières correspondant aux facettes {113} présentent une tendance inverse. Grâce audéveloppement d’une nouvelle méthodologie adaptant la sonde atomique tomographique àl’étude de processus dynamiques, il a été possible de relier les observations faites par FEM àla diffusion d’atomes d’oxygène sous la surface. Cette diffusion n’est pas homogène etdépend de la structure cristallographique des facettes. L’oxygène, formé à la suite d’uneadsorption dissociative sur les facettes du type {012}, ne pénètre le coeur de phase qu’autravers de certaines régions telles que les {113}, les {011} et les {111}. La construction desdiagrammes d’adsorption du CO2 et les diagrammes de phase cinétique du systèmeH2+O2/Rh ont permis de mettre en évidence les mouvements des atomes d’oxygène entre lasurface et la sous-surface. Finalement ces observations ont été étendues à d’autresmatériaux :Le platine et l’alliage PtRh. L’accumulation d’atomes d’oxygène sur et sous lasurface peut donc être observée en temps réel et à l’échelle moléculaire. / Doctorat en Sciences / info:eu-repo/semantics/nonPublished

In Pressurised Water Reactors, the reactor pressure vessel (RPV) is considered a life limiting component due to the degradation of its mechanical properties. Nano-scale Cu-enriched precipitates are known to cause embrittlement in the form of increases in hardness and the ductile-to-brittle transition temperature. The effect of irradiation on the RPV is the dominant contributor to this embrittlement. This is due to the increased mobility of Cu from the high number of vacancies, and the matrix damage providing many heterogeneous nucleation sites. However, there are also thermal effects which may be difficult to separate from the irradiation effects. To understand the contribution of the long term thermal ageing to RPV embrittlement a series of weld and plate materials containing systematic variations of Ni and Cu has been thermally aged for times up to 100,000 hrs at 330 degrees C, 365 degrees C and 405 degrees C. Microstructural characterisation using Atom Probe Tomography has been performed. Complimentary Monte-Carlo simulations have been used to investigate the early stages of formation of Cu-enriched precipitates. Thermal ageing produces a high number density of nano-scale Cu-enriched precipitates. These nanometre precipitates have a Ni-Mn-Si rich interface which was found to be wider with increased precipitate size, lower ageing temperature and higher bulk Ni content. This interface reduces the interfacial energy of the Cu-enriched precipitates through a combination of the minimising of unfavourable Fe-Cu bonds and reduction in lattice strain. The matrix Cu levels after ageing for 90,000 - 100,000 hrs were found to be around 0.06 - 0.07 at.%, close to the expected solubility limits for Cu in Fe. The Fe content of the precipitates has been characterised and found to be higher at lower ageing temperature and for smaller precipitate sizes. Cu precipitation and solute segregation at dislocations were observed, particularly in the SG steels aged at higher temperatures where the supersaturation is lowest. Movies were produced from the Kinetic Monte-Carlo modelling (see accompanying DVD) and along with other analyses indicated that sub-critical Ni and Mn clusters may be active in the formation of Cu-enriched precipitates. This mechanism appears to occur in both the high and low Ni steels. Thus, the higher number density of larger precipitates observed with increased bulk Ni content is thought to be a consequence of the greater number of sub-critical Ni-Mn clusters providing more nucleation sites. A small number of grain boundaries were examined. Segregation of many solute species to them was observed, which is thought to result from a multi-element co-segregation process. Ni-Mn-Si precipitates were observed at grain boundaries and dislocations in the high Ni steels with high and low Cu levels. These are consistent with similar phases in found in irradiated high Ni steels. In the high Cu steels these particles were much larger and associated with Cu-enriched precipitates.

In this work, new reconstruction and analysis methods were developed for 3D field ion microscopy (FIM) data, motivated by the goal of atomic scale characterisation of radiation damage for fusion applications. A comparative FIM/ atom probe tomography (APT) study of radiation damage in self-implanted tungsten revealed FIM advantages in atomistic crystallographic characterisation, able to identify dislocations, large vacancy clusters, and single vacancies. While the latter is beyond the detection capabilities of APT, larger damage features were observed indirectly in APT data via trajectory aberrations and solute segregation. An automated 3DFIM reconstruction approach was developed to maintain reliable, atomistic, 3D insights into the atomic arrangements and vacancies distribution in ion-implanted tungsten. The new method was utilized for the automated ‘atom-by-atom' reconstruction of thousands of tungsten atoms yielding highly accurate reconstructions of atomically resolved poles but also applied to larger microstructural features such as carbides and a grain boundary, extending across larger portions of the sample. Additional tools were developed to overcome reconstruction challenges arising from the presence of crystal defects and the intrinsic distortion of FIM data. Those were employed for the automated 3D mapping of vacancies in ion-implanted tungsten, analysing their distribution in a volume extending across 50nm into the depth of the sample. The new FIM reconstruction also opened the door for more advanced analyses on FIM data. It was applied to the preliminary studies of the distortion of the reconstructed planes, found to depend on crystallographic orientation, with an increased variance in atomic positions measured in a radial direction to the centre of the poles. Additional analyses followed the subtle displacements in atomic coordinates on consecutive FIM images, to find them affected by the evaporation of atoms from the same plane. The displacements were found to increase with size as the distance to the evaporated atom decreased, and are likely to be the result of a convolution between image gas effects, surface atoms relaxation, and charge re-distribution. These measurements show potential to probe the dynamic nature of the FIM experiment and possibly resolve contributions from the different processes effecting the final image. Finally, APT characterisation was performed on bulk and pre-sharpened needles to determine the effect of sample's geometry on the resulting implantation profiles, and the extent to which pre-sharpened needles could be employed in radiation damage studies. While the ions depth profiles in needles were not found within a good match to SRIM simulations, the damage profiles exhibited closer agreement. Further, the concentration of implanted ions in bulk samples was found significantly higher than in the respective needle implanted samples, with excessive loss found for the light ion implantation.

Dans ce travail nous avons étudié des réactions chimiques sur la surface de deux métaux : le platine et l'or, en utilisant la microscopie ionique à effet de champ électrique (FIM) et la spectrométrie de masse de désorption par champ pulsé (PFDMS). En complément de ces données expérimentales, nous apportons des résultats obtenus par la théorie de la fonctionnelle de la densité (DFT). La taille et la morphologie de nos échantillons font qu’ils sont de bons modèles de grains de phase active dans un catalyseur réel. Sur le platine nous avons observé l'interaction du monoxyde d'azote. En présence d'un champ électrique, la dissociation du NO est promue, laissant sur la pointe une couche d'oxygène que l'on peut titrer par la suite avec du NO pour former du dioxyde d'azote. L'interaction de l'hydrogène avec une pointe de platine est différente en fonction de la température. A basse température (<200 K), l’hydrogène met en image la pointe avec un assombrissement de petites régions de la pointe. A partir de 200 K, l'hydrogène induit une transformation de la pointe : les faces denses s'élargissent au détriment des faces rugueuses, avec une rangée d'atomes le long des lignes de zone [100] et le pôle central passe d’une forme circulaire à une forme carrée. L'hydrogène est supposé être à l'état atomique sur la surface; sous sa forme moléculaire, il ne contribue qu'à la mise en image. C’est sous sa forme atomique qu’il contribue aux transformations observées. La réaction NO+H2 sur le platine conduit à l'observation d'instabilités cinétiques pour des pressions et températures données. Les régions d'amorçage ont été identifiées comme étant tout ensemble de sites de cran situé le long des lignes de zone [100]. L'observation de phénomènes oscillants n'est pas liée exclusivement à une morphologie de type polyédrique : il est possible d’observer ces instabilités cinétiques sur des pointes de rayon de courbure différent, ces pointes ne subissent pas nécessairement un changement de morphologie. L'analyse chimique au cours de la réaction a révélé la présence d'oxydes de surface ce qui nous a conduit à penser que la surface du catalyseur de platine doit être oxydée plutôt que de rester à l'état métallique. Une étape intermédiaire dans le mécanisme de site vacant a été proposée pour permettre de rendre compte de l'apparition de phénomènes oscillants. L’étape déterminante est la décomposition du monoxyde d’azote adsorbé à la surface. L’apport d’hydrogène atomique nécessaire à la formation d’eau n’est pas une étape lente, au contraire l’hydrogène semble être largement présent sous forme atomique. L’influence du champ électrique reste important, ce qui pourrait expliquer les différences de gammes de température auxquelles d’autres groupes et le nôtre observons des oscillations. L'étude de l'interaction du CO seul sur l'or a été motivée par l'observation de la réaction CO+O2 sur pointe d'or. Sous nos conditions expérimentales, il est possible de former des mono- et dicarbonyles d’or sous forme cationique. En présence d'un champ électrique, la formation de carbonyles d'or est promue au niveau des sites de cran de la surface. Les résultats obtenus par DFT sont concordants avec les résultats expérimentaux. A l'instar du Pt, nous avons étudié l'interaction du monoxyde d'azote sur pointe d'or. Nous avons observé la formation de protoxyde d'azote et d'un dimère de monoxyde d'azote. Le mécanisme de formation de ces espèces reste encore inconnu. Une couche d'oxygène adsorbée à la surface peut être titrée par du NO en formant du dioxyde d'azote. En présence d'oxygène seul sur une pointe d'or sans champ électrique, les spectres de masse ne révèlent que la présence d'oxygène moléculaire. En présence d'un champ électrique, il est possible de détecter de l'oxygène atomique sans toutefois avoir la formation d'un oxyde d'or. Il est possible de former de l'ozone à partir d'une pointe recouverte d'oxygène atomique en présence d'oxygène moléculaire gazeux. Les calculs par DFT nous laissent à penser que la formation du cation O3+ ne se fait pas à la surface mais à proximité. Ils montrent entre autres que le champ électrique déstabilise l'oxygène atomique, ce qui pourrait le pousser vers des régions où l'effet du champ est le moins intense (la tige de la pointe).

Electron beam induced current (EBIC) and atom probe tomography (APT) were used in this study to determine electrical activities and impurity compositions at extended defects in multicrystalline silicon (mc-Si) samples. The results provide, for the first time, information regarding the chemical species present at defects whose electrical activity has previously been measured. A new APT specimen fabrication process was developed with the ability to select a specific defect for APT analysis. Development of the APT specimen fabrication process proceeded by first selecting and optimising the preferential etching for nano-scale defect delineation. Three etchants were evaluated, namely Secco, Sirtl and Dash, from which the Secco etch was selected. Three parameters were optimised to produce etch pits with geometries that meet the requirements imposed by APT specimen fabrication methods. The optimum parameters were 0.05M potassium dichromate concentration, 20°C etch temperature, and 30sec etch time. In the second stage, marking techniques were developed in order for the defects to be located throughout the APT specimen fabrication process. However, it became apparent that the conventional APT specimen fabrication method could not be used to fabricate APT specimens containing selected defects in a mc-Si sample. This led to the development of a novel APT specimen fabrication approach which allowed APT specimens to be fabricated, reproducibly, containing grain boundaries and isolated dislocations. In order to evaluate accurately iron contamination in mc-Si, four atom probe parameters were optimised to maximise detection sensitivity: the evaporation rate, the laser beam energy, the pulse repetition rate and the specimen temperature. The optimisation process can be divided in to two parts. In the first part, a matrix of pre-sharpened single-crystal silicon specimens was subjected to a variety of experimental parameters. The optimised parameters were determined to be 0.3% evaporation rate, 0.5nJ beam energy, 160kHz repetition rate and 55K specimen temperature. The second part was to determine the iron detection efficiency –the percentage of detected Fe ions that can be correctly identified as Fe– and sensitivity using these parameters to analyse a specially prepared iron calibration specimen. The values were determined to be a detection efficiency of about 35% and sensitivity of 54ppm or 2.70x10¹⁸ atom/cm³. The APT specimen fabrication process and the optimised APT analysis parameters were used to analyse four extended defects in mc-Si samples subjected to three different processing conditions, namely gold-contaminated, as-grown and phosphorus diffusion gettering (PDG). The important aspects of the analysis are listed below: • Gold was not detected at the grain boundary and its associated dislocations in the gold-contaminated specimen. The binding enthalpy of gold to such defects is thus less than 0.63eV. • Iron was not detected in any specimen. • Copper was observed at the grain boundary in the as-grown specimen in the form of individual atoms as well as clusters with diameters ranging between 4nm and 9nm. The electrical activity of the grain boundary was about 58%. • Nickel and carbon were detected at the grain boundary in the post-PDG specimen with the former having platelet structures with diameters and thicknesses ranging between 4nm-7nm and 2nm-4nm, respectively. The recombination strength of the defect was about 22%. • Two nickel clusters were found at the isolated dislocation in the post-PDG specimen. The clusters were spherical with an average diameter of 10nm. The distance between the two clusters was 35nm. The recombination strength of the defect was about 4%.