The objective of this dissertation is to understand the structural and optoelectronic properties of group III-nitride materials grown by High-Pressure Metal Organic Chemical Vapor Deposition (HP-MOCVD) and Migration Enhanced Plasma Assisted MOCVD by FTIR reflectance spectroscopy, Raman spectroscopy, X-ray diffraction, and Atomic Force Microscopy. The influence of the substrates/templates (Sapphire, AlN, Ga-polar GaN, N-polar GaN, n-GaN, and p-GaN) on the free carrier concentration, carrier mobility, short-range crystalline ordering, and surface morphology of the InN layers grown on HP-MOCVD were investigated using those techniques. The lowest carrier concentration of 7.1×1018 cm-3 with mobility of 660 cm2V-1s-1 was found in the InN film on AlN template, by FTIR reflectance spectra analysis. Furthermore, in addition to the bulk layer, an intermediate InN layers with different optoelectronic properties were identified in these samples. The best local crystalline order was observed in the InN/AlN/Sapphire by the Raman E2 high analysis. The smoothest InN surface was observed on the InN film on p-GaN template. The influence of reactor pressures (2.5–18.5 bar) on the long-range crystalline order, in plane structural quality, local crystalline order, free carrier concentration, and carrier mobility of the InN epilayers deposited on GaN/sapphire by HP-MOCVD has also been studied using those methods. Within the studied process parameter space, the best material properties were achieved at a reactor pressure of 12.5 bar and a group-V/III ratio of 2500 with a free carrier concentration of 1.5x1018 cm-3, a mobility in the bulk InN layer of 270 cm2 V-1s-1 and the Raman (E2 high) FWHM of 10.3 cm-1. The crystalline properties, probed by XRD 2θ–ω scans have shown an improvement with the increasing reactor pressure. The effect of an AlN buffer layer on the free carrier concentration, carrier mobility, local crystalline order, and surface morphology of InN layers grown by Migration-Enhanced Plasma Assisted MOCVD were also investigated. Here, the AlN nucleation layer was varied to assess the physical properties of the InN layers. This study was focused on optimization of the AlN nucleation layer (e.g. temporal precursor exposure, nitrogen plasma exposure, and plasma power) and its effect on the InN layer properties.

The signal resulting from the IR-FSE sequence has been thoroughly analyzed in order to improve the accuracy of quantitative T1 mapping of the human brain. Several optimized post-processing algorithms have been studied and compared in terms of their T1 mapping accuracy. The modified multipoint two-parameter fitting method was found to produce less underestimation compared to the traditional multipoint three-parameter fitting method, and therefore, to result in a smaller T1 estimation error. Two correction methods were proposed to reduce the underestimation problem which is commonly seen in IR-FSE sequences used for measuring T1, especially when a large turbo factor is used. The intra-scan linear regression method corrects the systematic error effectively but the RMSE may still increase due to the increase of uncertainty in sequences with large turbo factors. The weighted fitting model corrects not only the systematic error but also the random error and therefore the aggregate RMSE for T1 mapping can be effectively reduced. A new fitting model that uses only three different TI measurements for T1 estimation was proposed. The performance for the three-point fitting method is as good as that of the multipoint fitting method with correction in the phantom simulation. In addition, a new ordering scheme that implements the three-point fitting method is proposed; it is theoretically able to reduce the total scan time by 1/3 compared to the TESO-IRFSE sequence. The performance of the three-point fitting method on the real human brain is also evaluated, and the T1 mapping results are consistent to with the conventional IR-FSE sequence. More samples of true anatomy are needed to thoroughly evaluate the performance of the proposed techniques when applied to T1 mapping of the human brain.

DNA DSBs are most toxic to cells because they can lead to genomic rearrangements and even cell death. Most DSBs induced by ionizing radiation or radiomimetic drugs such as calicheamicin and bleomycin, bear 3′-phosphate or 3′- PG moieties that must be removed to allow subsequent gap filling and ligation. DSBs can be repaired by two main pathways: the homologous recombination (HR) pathway and the non-homologous end-joining (NHEJ) pathway, NHEJ is the primary repair pathway in mammalian cells. While HR repairs single strand breaks (SSBs) or DSBs accurately by using an undamaged copy of the sequence mostly at late S phase and G2 phase, the NHEJ pathway repairs DSBs without the requirement for sequence homology in a processing that may be error-free or error- prone and is most active at G1 phase. TDP1 is a DNA repair enzyme in both pathways, It associates with DNA SSB repair proteins XRCC1 and DNA ligase III and plays a role in processing of topoisomerase I- mediated SSBs. Our early results suggested that TDP1 also can remove protruding 3’- PG and other 3’ blocks from DSBs ends in vitro. A homozygous H493R mutation in the active site of TDP1 causes spinocerebellar ataxia with axonal neuropathy (SCAN1), a rare autosomal recessive genetic disease with neurological symptoms including peripheral neuropathy. DNA damage and misrepair can be determined by measuring the incidence of chromosomal aberrations such as rings, breaks, dicentrics, acentric fragments, and translocations in metaphase cells, and micronuclei in interphase cells. To assess the possible role of TDP1 in DSB repair in intact cells, the radiosensitivity of SCAN1 cells was determined by using a dose-fractionation method of irradiation. The data indicated that, when exposed to fractionated radiation doses, the SCAN1 cells were more sensitive than normal cells. Moreover, following treatment of cells with calicheamicin, SCAN1 cells showed a significantly higher incidence of dicentric chromosomes, acentric fragments, and micronuclei compared to normal cells, indicating that calicheamicin-induced DSBs were repaired less accurately and less efficiently, or more slowly in SCAN1 cells than in normal cells. All these results are consistent with a role for TDP1 in repair of 3’-PG DSBs in vivo. Oxidative stress is thought to induce replicative senescence and DNA damage in mouse embryo fibroblasts (MEFs). To determine the possible roles of oxidative stress on Tdp1-deficient MEFs, Tdp1-knockout MEFs and normal MEFs were cultured in 20% oxygen (atmospheric) and 3% (physiological) oxygen. The data from growth assays indicated that normal MEFs showed replicative senescence in 20% oxygen but not in 3% oxygen. Tdp1-knockout MEFs showed very poor growth compared to Tdp1 normal MEFs in both oxygen conditions, clearly suggesting an influence of repair of Tdp1 on oxidative stress induced DNA-DSBs in MEFs. Taken together, our results indicated that TDP1 is capable of removing protruding 3’-PG from DSB ends in intact cells. Moreover, DSBs induced by oxidative stress were repaired more slowly or inefficiently in MEFs when Tdp1 is absent, resulting in cell cycle arrest and poor cell growth.

PVDF, Poly(vinylidene fluoride), is a polymer that has been studied for over four decades due to its good electromechanical properties, stability, and durability in various environments. Currently, PVDF is the only commercially available piezoelectric polymer. PVDF is a polymorph, which indicates the presence of several crystalline phases such as α, β, γ, and δ-phase. Oriented β-phase PVDF exhibits ferroelectric properties and displays the largest piezoelectricity amongst the four phases, which makes it the most desirable phase. Preparing oriented β-phase PVDF is a multi-step process, which is cost intensive, due to the time, labor and energy utilized. The main goal of this work is to prepare oriented β-phase PVDF using the electrospraying technique in a one step process. During the electrospraying process a polymer jet is ejected. This jet disintegrates into droplets due to overwhelming surface tension, resulting in a sprayed coating on the collector substrate. Because of the combination of jet ejection and the high voltage applied between the needle tip and the substrate, the droplets can be stretched and the polymer chains can be oriented. Both the stretching and the high electric field are required for the transformation of α-phase to the oriented β-phase. This study proposes that by using the electrospraying technique it is possible to transform the α-phase to the β-phase in a one step process starting from solution. This research focuses on the processing and characterization of electrosprayed PVDF as well as electrosprayed PVDF/carbon nanotubes (PVDF/CNT) nanocomposites. The specific tasks are to determine the changes to the PVDF phases due to the electrospraying technique, and to determine the changes in the PVDF morphology due to the addition of carbon nanotubes to the polymer matrix.PVDF with two different molecular weights were electrosprayed using different solvents and parameters. Initial observations after electrospraying were that, high boiling point solvents resulted in the spraying of the solution and forming films, whereas a low boiling point volatile solvent such as acetone resulted in the spinning of the solution thus forming non-woven fiber mats. The thermal and electrical properties of the electrosprayed PVDF and PVDF/CNT composites are measured using several characterization techniques, including Modulated Differential Scanning Calorimetry (MDSC), Dielectric spectroscopy, Thermally Stimulated Current (TSC), Fourier Transform Infrared Spectroscopy (FT-IR), and X-Ray Diffraction (XRD). MDSC results show that electrosprayed PVDF has a lower melting point temperature than that of PVDF commercially available pellets. In addition, electrosprayed PVDF/CNT nanocomposites show a linear increase in the percentage of crystallinity with the increase of CNT concentration in the composite. Dielectric spectroscopy results indicate that by increasing the CNT concentration in the composite, the dielectric constant and the polymer conductivity increase.From the four characterizing techniques used, two of them, FT-IR and XRD, show that it is possible to transform α-phase to β-phase PVDF in a one-step process using electrospraying. The other two techniques, TSC and dielectric spectroscopy, show α-phase for the electrosprayed samples without CNT, and some β-phase formation with samples electrosprayed with CNT. These last two techniques; TSC and dielectric spectroscopy have results that differ from the FT-IR and XRD techniques. This contradiction may be a result of the small amounts of β-phase in the sample, which cannot be detected using these techniques. Another reason may be due to the difference in the probing levels between these techniques. XRD and FT-IR probe at the molecular level, whereas TSC and dielectric probe at a much larger scale, which may make it hard to detect small amounts of β-phase.

Mémoire numérisé par la Direction des bibliothèques de l'Université de Montréal.

This work provides an innovative solution for monitoring fatigue for users behind workstations. A web camera was adjusted to work in near infrared range and a system of 880 nm IR diodes was implemented to create an IR vision system to localize and track the eye pupils. The software developed monitors and tracks eyes for signs of fatigue by measuring PERCLOS. The software developed runs on the workstation and is designed to draw limited computational power, so as to not interfere with the user task. To overcome low-frame rate imposed by the hardware limitations and to improve real time monitoring, two-phases detection and tacking algorithm is implemented. The proposed system successfully monitors fatigue at a rate of 8 fps. The system is well suited to monitor users in command centers, flight control centers, airport traffic dispatches, military operation and command centers, etc., but the work can be extended to wearable devices and other environments.

No description available.

This study examines how two teachers in grade 3 support their students with problem solving in the teaching and what strategies the students may use in their tasks. The study was of a qualitative nature and was carried out with observations and complementary interrogation questions. The result showed that the teachers supported their students with two forms of feedback.

Neste trabalho foram estudados os níveis excitados do 193Ir produzidos a partir do decaimento β do 193Os (T1/2 ~ 30h). Para a obtenção das amostras radioativas, ~ 5mg de Ósmio metálico (99% enriquecido em 192Os) foram irradiados no reator IEA-R1, sob um fluxo de nêutrons da ordem de 1012cm2 s1 e depois analisadas, empregando-se a técnica de espectroscopia γ simples (unidimensional) com espectrômetro γ de alta resolução, bem como as técnicas de espectroscopia de coincidência γγ e de correlação angular direcional γγ (θ) usando um sistema de aquisição multiparamétrica composto por 4 detectores HPGe. A partir destes dados, foi possível adicionar 28 transições a este esquema de decaimento, 11 das quais já eram conhecidas de outros estudos envolvendo reações nucleares, além de 17 observadas pela primeira vez. Também foram acrescentados 8 níveis excitados ao esquema de decaimento, sendo 3 conhecidos por outras reações e 5 completamente novos. Além disso, foi possível confirmar a suspeita encontrada na literatura de que os níveis a 848,93keV e 849,093keV são o mesmo, além de confirmar a existência de um nível excitado a 806,9keV. A análise de correlação angular direcional permitiu a definição do spin de do nível excitado a 874kev (5/2+), além de propor uma probabilidade de 79% do nível a 1078keV ter spin 5/2, e de restringir as possibilidades de spin para o nível novo a 960keV para duas (1/2 ou 3/2). Também foi possível determinar a razão de mistura multipolar (δLn+1/Ln) para 43 transições, sendo 19 pela primeira vez e praticamente todas as restantes com precisão melhor que a encontrada na literatura. Finalmente, foi feita uma tentativa de compreender o núcleo através de um modelo teórico, o qual reproduziu muito bem o estado fundamental e os dois primeiros estados excitados do 193Ir. / In this work, the excited levels of 193Ir populated by the β decay of 193Os (T1/2 30h) were investigated. For that purpose, 5mg samples of 99%-enriched 192Os were irradiated under a thermal neutron flux of 1012s1 and then analysed both using single gamma spectroscopy and a 4-detector multiparametric acquisition facility, which provided data for both a γγ coincidence analysis and a directional angular correlation γγ (θ) study. From these data, 28 transitions were added to this decay scheme, 11 of which were previously known from nuclear reactions and 17 observed for the first time. Eight excited levels were also added to the decay scheme, 3 of which were known from nuclear reaction studies the remaining 5 are suggested for the first time. Moreover, it was possible to confirm suspicions found in reference that the levels at 848.93keV and 849.093keV are indeed the same; it was also possible to confirm the existence of an excited level at 806.9keV, which had been inferred, but not experimentally confirmed in β decay studies to date. The angular correlation analysis allowed for the definition of the spin of the excited level at 874keV as 5/2+; moreover, the results showed a 79% probability that the spin of the 1078keV level is 5/2, and also restricted the spin possibilities for the new excited level at 960keV to two values (1/2 or 3/2). It was also possible to measure the multipolarity mixing ratio (δLn+1/Ln) for 43 transitions 19 of them for the first time and most of the others with a better precision than previously known. Finally, an attempt was made to understand the low-lying levels structure for this nucleus using a theoretical model, which reproduced the ground state and the two lowest-lying excited levels in 193Ir.

Diodos poliméricos emissores de luz (PLEDs) foram produzidos utilizando poli(vinil-carbazol) (PVK), poli(2,7-(9,9-dioctilfluoreno)) (PFO) e poli((1,4-fenileno-2-flúor)-alt-2,7-(9,9-dioctilfluoreno)) (PFPF) dopados com diferentes concentrações de dopante fosforescente tris(2-fenilpiridinato) de irídio(III) [Ir(ppy)3] como camada ativa. Os resultados mostraram que o dispositivo a base de PFO dopado com 4% em massa de Ir(ppy)3 apresentou as maiores eficiências de corrente e de potência luminosa e o espectro eletromagnético do PLED a base de PVK puro apresentou emissão em 540 nm, sugerindo um desbalanceamento de cargas e emissão do óxido de zinco dopado com alumínio (AZO), camada injetora. Assim, estudos da influência da massa molar média do PVK e de sistemas híbridos PVK:AZO nas propriedades elétricas e ópticas dos PLEDs foram elaborados. Resultados mostraram que o AZO possui propriedades foto/eletroluminescentes e é responsável pela emissão larga na região do visível. Os dispositivos híbridos apresentaram emissão próxima ao branco puro, atingindo-se uma pureza de 0,19. / Polymer light emiting diodes (PLEDs) were manufactured using poly(9-vinylcarbazole) (PVK), poly(9,9-dioctylfluorene) (PFO) and poly(9,9-dioctylfluorene-alt-1,4-fluorphenylene) (PFPF) doped with different concentrations of tris-(2-phenylpyridinate) iridium(III) [Ir(ppy)3],a phosphorescent dye, as the active layer. Results showed that PFO based devices doped with 4 wt. % of Ir(ppy)3 presented the highest current and power efficiencies, and the PVK based devices\' electroluminescence spectrum showed an emission centered at 540 nm, suggesting that a charge unbalance and light emission from the injection layer of aluminum doped zinc oxide (AZO) occurred. Therefore, studies based on the PVK:AZO system and different PVK\'s average molar masses were elaborated to observe the PLEDs\' electrical and optical properties. Results showed that AZO is a photo/electroluminescent material and it is responsible for the broad emission in the visible range. The hybrid device showed near pure white light emission and its purity reached 0.19.