985 resultados para MAGNETORESISTANCE OSCILLATIONS
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Individual milk samples taken every two weeks from parturition to the end of lactation from 34 animals of three different herds and breeds were analyzed for free-GMP. A milk pool of each herd was analyzed for free and total GMP (released from k-casein by the action of rennin) and the data were correlated with sanitary conditions of animal and udder, phase of lactation and milk production. Most udder problems were concentrated near parturition, with few and spaced occurrences of clinical mastitis. The Californian Mastitis Test (CMT) results showed oscillations compatible with the phases of lactation period and environmental conditions. The widest variations in free-GMP occurred as a function of lactation period and as a consequence of clinical or subclinical mastitis. Higher levels were observed at the beginning of lactation (5.87mg L-1 of sialic acid), becoming normal with mean values of about 3.30mg L-1 at the end of the second month, and increasing again during the final third of lactation. On average, the same trends were observed for total GMP released by commercial rennet, beginning with slightly high values (35.59mg L-1), becoming normal by the sixth month with values close to 27.15mg L-1, and rising gradually up to the end of lactation, with 58.35mg L-1 of sialic acid. These results prove to be useful for the correct interpretation of tests applied to milk selection with respect to proteolytic status or even to restrain frauds by the addition of whey to milk.
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The objective was to determine the glycemic index and glycemic load of tropical fruits and the potential risk for chronic diseases. Nine fruits were investigated: coconut water (for the purpose of this study, coconut water was classified as a “fruit”), guava, tamarind, passion fruit, custard apple, hog plum, cashew, sapodilla, and soursop. The GI and GL were determined according to the Food and Agriculture Organization protocol. The GL was calculated taking into consideration intake recommendation guidelines; 77.8% of the fruits had low GI although significant oscillations were observed in some graphs, which may indicate potential risks of disease. Coconut water and custard apple had a moderate GI, and all fruits had low GL. The fruits evaluated are healthy and can be consumed following the daily recommended amount. However, caution is recommended with fruits causing early glycemic peak and the fruits with moderated GI (coconut water and custard apple).
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Perovskite manganite compounds, Lai-xDxMnOs (D-divalent alkaline earth Ca, Sr or Ba), whose electrical and magnetic properties were first investigated nearly a half century ago, have attracted a great deal of attention due to their rich phase diagram. From the point of view of designing a future application, the strong pressure dependence of the resistivity and the accompanying effects in thin films have potential for application in pressure sensing and electronic devices. In this study we report our experimental investigations of pressure dependence of the resistivity of Lao.siSvo^iQMnOs and Lai-xSvxMnOs (LSMO) epitaxial films with x= 0.15, 0.20, 0.25, 0.30, 0.35, on SrTiOs substrates.
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The perovskite crystal structure is host to many different materials from insulating to superconducting providing a diverse range of intrinsic character and complexity. A better fundamental description of these materials in terms of their electronic, optical and magnetic properties undoubtedly precedes an effective realization of their application potential. SmTiOa, a distorted perovskite has a strongly localized electronic structure and undergoes an antiferromagnetic transition at 50 K in its nominally stoichiometric form. Sr2Ru04 is a layered perovskite superconductor (ie. Tc % 1 K) bearing the same structure as the high-tem|>erature superconductor La2_xSrrCu04. Polarized reflectance measurements were carried out on both of these materials revealing several interesting features in the far-infrared range of the spectrum. In the case of SmTiOa, although insulating, evidence indicates the presence of a finite background optical conductivity. As the temperature is lowered through the ordering temperature a resonance feature appears to narrow and strengthen near 120 cm~^ A nearby phonon mode appears to also couple to this magnetic transition as revealed by a growing asymmetry in the optica] conductivity. Experiments on a doped sample with a greater itinerant character and lower Neel temperature = 40 K also indicate the presence of this strongly temperature dependent mode even at twice the ordering temperature. Although the mode appears to be sensitive to the magnetic transition it is unclear whether a magnon assignment is appropriate. At very least, evidence suggests an interesting interaction between magnetic and electronic excitations. Although Sr2Ru04 is highly anisotropic it is metallic in three-dimensions at low temperatures and reveals its coherent transport in an inter-plane Drude-like component to the highest temperatures measured (ie. 90 K). An extended Drude analysis is used to probe the frequency dependent scattering character revealing a peak in both the mass enhancement and scattering rate near 80 cm~* and 100 cm~* respectively. All of these experimental observations appear relatively consistent with a Fermi-liquid picture of charge transport. To supplement the optical measurements a resistivity station was set up with an event driven object oriented user interface. The program controls a Keithley Current Source, HP Nano-Voltmeter and Switching Unit as well as a LakeShore Temperature Controller in order to obtain a plot of the Resistivity as a function of temperature. The system allows for resistivity measurements ranging from 4 K to 290 K using an external probe or between 0.4 K to 295 K using a Helium - 3 Cryostat. Several materials of known resistivity have confirmed the system to be robust and capable of measuring metallic samples distinguishing features of several fiQ-cm.
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Interest in mixed-valent perovskite manganese oxides of La\-xAxMnO^ (v4-divalent alkaline earth Ca, Sr or Ba), whose unusual properties were discovered nearly a half century ago, has recently been revived. The discovery of the colossal magnetoresistance and pressure effects introduced new questions concerning the complex interplay between lattice structure, magnetism and transport in doped perovskite manganites. In this study, we report our experimental investigations of pressure and magnetic field dependencies of La-i/sCai/sMnOs (LCMO) epitaxial films with various thickness on SrTiO$ substrate. An analysis of film thickness dependency of the resistivity of LCMO epitaxial films under pressure and magnetic field has been performed by taking into account substrate contributions. This verifies the correlation of lattice distortion with magnetic and transport properties. Strong dependencies of Mn — O — Mn bond bending and Mn — O bond stretching with pressure as well as Mn spin alignment with magnetic field, and the lattice distortion induced by the substrate are discussed.
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Perovskite type piezoelectric and manganese oxide materials have gained a lot of attention in the field of device engineering. Lead zirconium titananium oxide (PbZri.iTiiOa or PZT) is a piezoelectric material widely used as sensors and actuators. Miniaturization of PZTbased devices will not only perfect many existing products, but also opens doors to new applications. Lanthanum manganese oxides Lai-iAiMnOa (A-divalent alkaline earth such as Sr, Ca or Ba) have been intensively studied for their colossal magnetoresistance (CMR) properties that make them applicable in memory cells, magnetic and pressure sensors. In this study, we fabricate PZT and LSMO(LCMO) heterostructures on SrTiOa substrates and investigate their temperature dependency of resistivity and magnetization as a function of the thickness of LSMO(LCMO) layer. The microstructure of the samples is analysed through TEM. In another set of samples, we study the effect of application of an electric field across the PZT layer that acts as an external pressure on the manganite layer. This verifies the correlation of lattice distortion with transport and magnetic properties of the CMR materials.
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Polycrysttdline samples of NaiCoOa were prepared using the "Rapid heat-up" method. One set of samples was annealed in flowing O2, while the other set in flowing Argon. X-Ray diffraction measurements indicated a stable phase of Nao.7Co02 mixed with C03O4 for all the samples even though they differed in concentration of Na. Argon annealed samples were insulators, whereas the ones annealed in O2 were metallic. Most of the measurements were performed on the sample Nao.7Co02, because it is the host compound for the superconductor sample Nao.35Co02-H20. Magnetization measurement showed that the magnetic moment decreased with increasing sodium concentration. This is due to the existence of C03O4 in samples with Na^ 0.7. As sodium concentration decreases, the magnetic moment increases due to the increasing concentration of C03O4 and its large magnetic moment. Magnetization measurements showed that the magnetic moment of Nao.7Co02 is field-dependent in low fields eind field-independent in fields higher than 100 G. Resistivity changes with temperature (dp/dT) increased with increasing Na concentration. Also resistivity measurements were performed under different hydrostatic pressures on Nao.7Co02. Two transitions were observed; one at a temperature Ti ~20 K and the other at T2 ^280 K, the transition at Ti has a magnetic origin and the one at T2 is a structiural transition. It was noticed that pressure aJfects resistivity of the sample. At higher pressures resistivity changes faster with temperature. Magnetoresistance measurement showed a small change in the resistivity, especially at lower temperatures. A novel layered superconductor Nao.35Co02H20 was prepared using de-intercalation of Na from the host compound Nao.7Co02. FVom the temperature dependence of the magnetization, the superconducting transition temperature and lower critictil field have been estimated as Tc=4.12 K and Hci=66 G, respectively.
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The Bi2Sr2CaCu20g single crystal with a superconducting transition temperature equal to 90 ± 2 K was prepared. The irreversibility line of the single crystal for a mgnetic field direction along the c-axis and T* in the ab-plane was determined. The reduced temperature (l - T ) is proportional to H 1.1 for fields below 004 T and proportional to HO.09 for fields above 0.4 T. The zero temperature upper critical field Hc2(0) and coherence length ~ (0) were determined from the magnetization meaurements to be H-lC2=35.9T , H//C2=31.2T, ~c(0)=35.0 A, and ~ab(0)=32.5A,and from the magnetoresistance measurements to be H-lc2 = 134.6T , H//C2=55.5T '~c(0)=38.1 A, and ~ab(0)=2404 A for both directions of the applied magnetic field. The results obtained for Hc2(0) and ~(O) are not reliable due to the rounding that the single crystal exhibits in the magnetization and magnetoresistance curves. The magnetization relaxation of the single crystal was investigated, and was found to be logarithmic in time, and the relaxation rate increases with temperature up to 50 -60 K, then decreases at higher temperatures.
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To investigate the thennal effects of latent heat in hydrothennal settings, an extension was made to the existing finite-element numerical modelling software, Aquarius. The latent heat algorithm was validated using a series of column models, which analysed the effects of penneability (flow rate), thennal gradient, and position along the two-phase curve (pressure). Increasing the flow rate and pressure increases displacement of the liquid-steam boundary from an initial position detennined without accounting for latent heat while increasing the thennal gradient decreases that displacement. Application to a regional scale model of a caldera-hosted hydrothennal system based on a representative suite of calderas (e.g., Yellowstone, Creede, Valles Grande) led to oscillations in the model solution. Oscillations can be reduced or eliminated by mesh refinement, which requires greater computation effort. Results indicate that latent heat should be accounted for to accurately model phase change conditions in hydrothennal settings.
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Accuracy at reporting a second-target (T2) is reduced if it is presented within approximately 500 ms of the first target (T1) – an attentional blink (AB). Early models explained the AB in terms of attentional limitations creating a processing bottleneck such that T2 processing would be impaired while T1 processing was ongoing. Theoretical models of the AB have more recently been expanded to include the role of cognitive control. In this dissertation I propose that cognitive control, defined as the optimization of information processing in order to achieve goals, is maladapted to the dual-task conditions of the AB task in that cognitive control optimizes the T1 goal, due to its temporal proximity, at the cost of T2. I start with the concept that the role of cognitive control is to serve goals, and that how goals are conceived of and the degree of motivation associated with those goals will determine whether cognitive control will create the condition that cause the AB. This leads to the hypothesis that electrophysiological measures of cognitive control and the degree of attentional investment resulting from cognitive control modulate the AB and explain individual differences in the AB. In a series of four studies feedback-related N2 amplitude, (reflecting individual differences in the strength of cognitive control), and event-related and resting alpha frequency oscillatory activity (reflecting degree of attentional investment), are used to explain both intra- and inter-individual variability in performance on the AB task. Results supported the hypothesis that stronger cognitive control and greater attentional investment are associated with larger AB magnitudes. Attentional investment, as measured by alpha frequency oscillations, and cognitive control, as measured by the feedback-related N2, did not relate to each other as hypothesized. It is proposed that instead of a measure of attentional investment alone, alpha frequency oscillatory activity actually reflects control over information processing over time, in other words the timing of attention. With this conceptualization, various aspects of cognitive control, either related to the management of goals (feedback-related N2) or the management of attention over time to meet goals, explain variability in the AB.
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This study used three Oculomotor Delayed Response (ODR) tasks to investigate the unique cognitive demands during the delay period. Changes in alpha power were used to index cognitive efforts during the delay period. Continuous EEGs from 25 healthy young adults (18-34 years) were recorded using dense electrode array. The data was analyzed by 6-cycle Morlet wavelet decompositions in the frequency range of 2-30 Hz to create time- frequency decompositions for four midline electrode sites. The 99% confidence intervals using the bootstrapped 20% trimmed mean of the 10 Hz frequency were used to examine the differences among conditions. Compared to two Memory conditions (Match and Non-Match), Control condition yielded significant differences in all frequencies over the entire trial period, suggesting a cognitive state difference. Compared to Match condition, the Non–Match condition had lower alpha activity during the delay period at each midline electrode site reflecting the higher cognitive effort required.
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"Mémoire présenté à la Faculté des études supérieures en vue de l'obtention du grade de maîtrise en droit, option recherche"
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Environ 2-3% d’enfants avec convulsions fébriles (CF) développent une épilepsie, mais les outils cliniques existants ne permettent pas d’identifier les enfants susceptibles de développer une épilepsie post-convulsion fébrile. Des études ont mis en évidence des anomalies d’EEG quantifiée, et plus particulièrement en réponse à la stimulation lumineuse intermittente (SLI), chez des patients épileptiques. Aucune étude n’a analysé ces paramètres chez l’enfant avec CF et il importe de déterminer s’ils sont utiles pour évaluer le pronostic des CF. Les objectifs de ce programme de recherche étaient d’identifier, d’une part, des facteurs de risque cliniques qui déterminent le développement de l’épilepsie après des CF et, d’autre part, des marqueurs électrophysiologiques quantitatifs qui différencieraient les enfants avec CF des témoins et pourraient aider à évaluer leur pronostic. Afin de répondre à notre premier objectif, nous avons analysé les dossiers de 482 enfants avec CF, âgés de 3 mois à 6 ans. En utilisant des statistiques de survie, nous avons décrit les facteurs de risque pour développer une épilepsie partielle (antécédents prénataux, retard de développement, CF prolongées et focales) et généralisée (antécédents familiaux d’épilepsie, CF récurrentes et après l’âge de 4 ans). De plus, nous avons identifié trois phénotypes cliniques distincts ayant un pronostic différent : (i) CF simples avec des antécédents familiaux de CF et sans risque d’épilepsie ultérieure; (ii) CF récurrentes avec des antécédents familiaux d’épilepsie et un risque d’épilepsie généralisée; (iii) CF focales avec des antécédents familiaux d’épilepsie et un risque d’épilepsie partielle. Afin de répondre à notre deuxième objectif, nous avons d’abord analysé les potentiels visuels steady-state (PEVSS) évoqués par la SLI (5, 7,5, 10 et 12,5 Hz) en fonction de l’âge. Le tracé EEG de haute densité (128 canaux) a été enregistré chez 61 enfants âgés entre 6 mois et 16 ans et 8 adultes normaux. Nous rapportons un développement topographique différent de l’alignement de phase des composantes des PEVSS de basses (5-15 Hz) et de hautes (30-50 Hz) fréquences. Ainsi, l’alignement de phase des composantes de basses fréquences augmente en fonction de l’âge seulement au niveau des régions occipitale et frontale. Par contre, les composantes de hautes fréquences augmentent au niveau de toutes les régions cérébrales. Puis, en utilisant cette même méthodologie, nous avons investigué si les enfants avec CF présentent des anomalies des composantes gamma (50-100 Hz) des PEVSS auprès de 12 cas de CF, 5 frères et sœurs des enfants avec CF et 15 témoins entre 6 mois et 3 ans. Nous montrons une augmentation de la magnitude et de l’alignement de phase des composantes gamma des PEVSS chez les enfants avec CF comparés au groupe témoin et à la fratrie. Ces travaux ont permis d’identifier des phénotypes électro-cliniques d’intérêt qui différencient les enfants avec CF des enfants témoins et de leur fratrie. L’étape suivante sera de vérifier s’il y a une association entre les anomalies retrouvées, la présentation clinique et le pronostic des CF. Cela pourrait éventuellement aider à identifier les enfants à haut risque de développer une épilepsie et permettre l’institution d’un traitement neuroprotecteur précoce.
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L’analyse spectrale de la fréquence cardiaque, de la pression artérielle systolique, de la pression artérielle diastolique ainsi que de la respiration par la transformée de Fourier rapide, est considérée comme une technique non invasive pour la détermination de l’activité du système nerveux autonome (SNA). Dans une population de sujets normaux volontaires, nous avons obtenu à l’état basal, des oscillations de basses fréquences (0,05-0,15Hz) reliées au système nerveux sympathique autonome et des oscillations de hautes fréquences (0,2Hz) représentant sur les intervalles entre chaque ondes R de l’électrocardiogramme (RR), l’arythmie sinusale respiratoire correspondant à une activité vagale. Nous avons comparé les tests de stimulation du système nerveux sympathique autonome déclenché par le passage de la position de repos (en décubitus dorsal), à la position orthostatique volontaire et le passage de la position de repos à la position orthostatique avec la table basculante à 60o. Nous avons également comparé un groupe normotendu à un groupe hypertendu qui a été soumis au passage du repos à l’orthostation volontaire et pour lesquels nous avons évalué la sensibilité du baroréflexe et la réponse sympathique par la mesure des catécholamines circulantes. Dans un groupe de sujets ayant une hypertension artérielle essentielle, nous avons évalué l’effet de la thérapie hypotensive, par le Trandolapril qui est un Inhibiteur de l’enzyme de conversion (IEC) de l`angiotensine. Dans ce groupe hypertendu, nous avons procédé, en plus de la stimulation sympathique par l’orthostation volontaire, à un exercice isométrique de trois minutes à 30 % de la force maximale. Nous avons également complété notre évaluation par la mesure de la densité de récepteurs ß2 adrénergiques sur lymphocytes et par la mesure des indices de contractilité à l’aide de l’échocardiographie en M mode. Les résultats ont montré, dans les groupes normaux volontaires, dans les deux types de stimulation du système nerveux sympathique par la position orthostatique, une augmentation significative des catécholamines plasmatiques avec une augmentation de la fréquence cardiaque et des basses fréquences de RR, confirmant ainsi que l’on est en état de stimulation sympathique. On observe en même temps une diminution significative des hautes fréquences de RR, suggérant un retrait vagal lors de cette stimulation. On a observé au test de la table basculante six cas d’hypotension orthostatique. On a comparé la position orthostatique volontaire entre le groupe de sujets normaux et le groupe de sujets hypertendus. L’analyse spectrale croisée de RR et de la pression artérielle systolique a permis d’évaluer dans l’hypertension artérielle (HTA), essentielle une sensibilité du baroréflexe atténuée, accompagnée d’une réactivité vagale réduite en présence d’une activité et d’une réactivité sympathique augmentées suggérant une altération sympathovagale dans l’HTA. Dans le groupe de sujets hypertendus traités (Trandolapril 2mg/jour), nous avons identifié un groupe de répondeurs au traitement par le Trandolapril et un groupe de non répondeurs à ce type de thérapie anti-hypertensive. Le groupe répondeur avait un profil hyper-adrénergique avec une hyper-réactivité sympathique, une fréquence cardiaque et des pressions artérielles diastolique et systolique plus élevées au repos. Dans le groupe total traité au Trandolapril, la densité des récepteurs ß2 adrénergiques a doublé, après thérapie, alors que la réactivité des basses fréquences obtenues à l’analyse spectrale a augmenté. Nous avons montré dans notre étude qu’un IECA a pu inhiber le mécanisme facilitateur de l’angII sur les terminaisons nerveuses sympathiques et a permis ainsi de réduire l’hyperactivité sympathique et le mécanisme de « down regulation » des récepteurs ß2 adrénergiques rendant ainsi l’expression de l’influence du SNA post synaptique plus efficace. Dans l’ensemble de nos protocoles cliniques, par l’utilisation de l’analyse spectrale des signaux RR, de la pression artérielle systolique,de la pression artérielle diastolique et de la respiration, nous avons montré que cette technique non invasive permet de décrire et de mieux comprendre les mécanismes physiologiques, physiopathologiques et pharmacologiques reliés au système nerveux autonome et à l’hypertension artérielle essentielle.
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Les pulsateurs compacts sont des étoiles présentant des variations intrinsèques de luminosité dont les gravités de surface sont supérieures à 100,000 cm/s² On retrouve parmi ces objets deux familles des sous-naines chaudes de type B (sdB) pulsantes et quatre familles distinctes de naines blanches pulsantes. Dans le but d'observer les pulsations de tels objets pour ensuite analyser leur propriétés grâce à l'astéroséismologie, l'Université de Montréal, en collaboration avec le Imaging Technology Laboratory (ITL - University of Arizona), a développé la caméra Mont4K (Montreal4K) CCD qui est, depuis le printemps 2007, le principal détecteur employé au télescope Kuiper de 1.55 m du Mt Bigelow (Steward Observatory, University of Arizona). à l'aide de ce montage, des observations ont été menées pour quelques-uns de ces pulsateurs compacts. La première cible fut HS 0702+6043, un pulsateur hybride. Une importante mission pour cet objet, réalisée du 1er novembre 2007 au 14 mars 2008, a permis d'identifier 28 modes de pulsations pour cet objet en plus de mettre en évidence pour certains de ces modes d'importantes variations d'amplitude. Deux autres cibles furent les naines blanches pulsantes au carbone de type « Hot DQ » SDSS J220029.08-074121.5 et SDSS J234843.30-094245.3. Il fut possible de montrer de façon indirecte la présence d'un fort champ magnétique à la surface de J220029.08-074121.5 grâce à la présence de la première harmonique du mode principal. En outre, pour ces deux cibles, on a pu conclure que celles-ci font bel et bien partie de la classe des naines blanches pulsantes au carbone.