Résumé : Nous étudions dans cette thèse plusieurs propriétés du gaz d’électrons bidimensionnel (GE2D) dans le graphène et la bicouche de graphène (BG). Nous commençons par étudier la nature des excitations à une particule du GE2D dans le graphène près des facteurs de remplissage entiers dans les niveaux de Landau N [pas égal à] 0. Nous utilisons une approche de type Hartree-Fock (HF) pour comparer l’énergie de l’excitation d’une paire électron-trou à celle d’une paire skyrmion (SK)-antiskyrmion (ASK). Dans le graphène, les excitations SK et ASK sont des excitations chargées avec une texture de spin et/ou de pseudospin de vallée qui est quantifiée topologiquement. Nos calculs montrent que les paires SK-ASK sont les excitations chargées de plus basse énergie jusqu’au niveau de Landau |N| = 3. Notre approche permet en plus de calculer le domaine de couplage Zeeman pour lequel les paires SK-ASK sont les excitations de plus basse énergie et de déterminer comment l’énergie de ces paires est modifiée par les corrections d’écrantage. Le diagramme de phase du GE2D dans la bicouche de graphène a fait l’objet d’intenses recherches théoriques et expérimentales [8, 13, 15, 16], mais jusqu’à maintenant, seuls les états uniformes ont été considérés. Nous adaptons notre approche HF à l’étude des états non uniformes pour montrer que le GE2D dans la BG à remplissage ν = −1 dans le niveau de Landau N = 0 subit une série de transitions de phase lorsqu’un champ électrique perpendiculaire à la BG est appliqué. Nous étudions tout particulièrement les phases comportant une texture de pseudospin orbital soit un cristal de skyrmions et une phase spirale. Nous calculons les modes collectifs de ces phases ainsi que leur absorption électromagnétique. Nous poursuivons ensuite avec une étude des phases cristallines autour de certains remplissages entiers dans la BG. Le GE2D dans la bicouche de graphène a principalement été étudié dans le niveau de Landau N = 0. Comme dernier problème, nous étudions le diagramme de phase lorsqu’un nombre entier de niveaux de Landau est occupé dans les niveaux supérieurs |N| > 0. Alors que l’état fondamental du GE2D dans le graphène pour ces mêmes niveaux est un ferroaimant de Hall quantique (FHQ) avec une symétrie SU(2) pour le spin (en l’absence de couplage Zeeman) et le pseudospin de vallée, le GE2D dans la BG a plutôt un comportement FHQ de type Ising avec une symétrie Z[indice inférieur 2] à champ électrique nul. Cette différence de comportement a une grande influence sur la nature des transitions de phase possibles ainsi que sur celle des excitations topologiques. // Abstract : In this thesis, we study several properties of the two-dimensional electron gas (2DEG) in graphene and bilayer graphene. We first study the nature of the single-particle excitations in graphene near integer filling factors in Landau levels (LLs) N [not equal to] 0. We use a Hartree-Fock approach to compare the energy of an electron-hole excitation pair with that of a Skyrmion-antiskyrmion pair. In graphene, Skyrmions are charged excitations with a topological quantized spin and/or valley pseudo-spin texture. We give the range of Zeeman coupling for which Skyrmion-antiskyrmion has the lowest energy up to LL N = 3. Then we discuss how screening corrections modifies these results. The phase diagram of the 2DEG in bilayer graphene had been studied previously by a number of authors [8, 13, 15, 16] but only uniform states had been considered. Extending the Hartree-Fock approach to non-uniform states, we show that at filling factor ν = −1 in LL N = 0, the 2DEG goes through a series of phase transitions as the bias from an external electric field between two layers is increased. We study a crystal phase with orbital SK textures and a spiral state with the orbital pseudospin rotating in space. We compute the collective mode of these phases and their signatures in electromagnetic absorption experiments. We finally extend the Hartree-Fock approach to study the crystal states with valley or orbital textures near integer filling factors. The research on the 2DEG in bilayer graphene has been focussed almost exclusively in LL N = 0. As our last problem, we study the phase diagram at quarter and half fillings of the quartet of states in LLs |N| > 0. While the ground state of the 2DEG in graphene in |N| > 0 is a valley and spin quantum Hall ferromagnet with SU(2) symmetry in the absence of Zeeman coupling, the ground state in bilayer graphene is an Ising quantum Hall ferromagnet with a Z[subscript 2] valley symmetry at zero bias. We note that this change has important consequences on the nature of the transport properties and the single-particle excitations at integer fillings.

Ultrasound contrast agents (CAs) are typically used in clinic for perfusion studies (blood flow through a specific region) and border delineating (differentiate borders between tissue structures) during cardiac imaging. The CAs used during ultrasound imaging usually consist of gas filled microbubbles (MBs) (diameter 1-5 μm) that are injected intravenously into the circulatory system. This thesis partially involves a novel polymer-shelled ultrasound CA that consists of air filled MBs stabilized by a polyvinyl alcohol (PVA) shell. These MBs could be coupled with superparamagnetic iron oxide nanoparticles (SPIONs) in order to serve as a combined CA for ultrasound and magnetic resonance imaging. The first three papers (Paper A-C) in this thesis investigate the structural characteristic and the elimination process of the CA. In Paper A, two types (PVA Type A and PVA Type B) of the novel CA were analyzed using transmission electron microscopy (TEM) images of thin sectioned MBs. The images demonstrated that the SPIONs were either attached to the PVA shell surface (PVA Type A) or embedded in the shell (PVA Type B). The average shell thickness of the MBs was determined in Paper B by introducing a model that calculated the shell thickness from TEM images of cross-sectioned MBs. The shell thickness of PVA Type A was determined to 651 nm, whereas the shell thickness of PVA Type B was calculated to 637 nm. In Paper C, a prolonged blood elimination time was obtained for PVA-shelled MBs compared to the lipid-shelled CA SonoVue used in clinic. In addition, TEM analyzed tissue sections showed that the PVA-shelled MBs were recognized by the macrophage system. However, structurally intact MBs were still found in the circulation 24 h post injection. These studies illustrate that the PVA-shelled MBs are stable and offer large chemical variability, which make them suitable as CA for multimodal imaging. This thesis also involves studies (Paper D-E) of the molecular chaperones (Hsp21 and DNAJB6). The small heat shock protein Hsp21 effectively protects other proteins from unfolding and aggregation during stress. This chaperone ability requires oligomerization of the protein. In Paper D, cryo-electron microscopy together with complementary structural methods, obtained a structure model which showed that the Hsp21 dodecamer (12-mer) is kept together by paired C-terminal interactions.The human protein DNAJB6 functions as a very efficient suppressor of polyglutamine (polyQ) and amyloid-β42 (Aβ42) aggregation. Aggregation of these peptides are associated with development of Huntington’s (polyQ) and Alzheimer’s (Aβ42) disease. In Paper E, a reconstructed map of this highly dynamic protein is presented, showing an oligomer with two-fold symmetry, indicating that the oligomers are assembled by two subunits. / <p>QC 20160527</p>

The thermal velocity fluctuations of microscopic particles mediate the transition from microscopic statistical mechanics to macroscopic long-time diffusion. Prior to this work, detection methods lacked the sensitivity necessary to resolve motion at the length and time scales at which thermal velocity fluctuations occur. This dissertation details two experiments which resulted in velocity measurement of the thermal motion of dielectric microspheres suspended by an optical trap in gases and liquids. First, optical tweezers were used to trap glass microspheres in air over a wide range of pressures and a detection system was developed to track the trapped microspheres' trajectories with MHz bandwidth and <100 fm/rt(Hz) position sensitivity. Low-noise trajectory measurements allowed for observation of fluctuations in the instantaneous velocity of a trapped particle with a signal to noise ratio (SNR) of 26 dB, and provided direct verification of the equipartition theorem and of the Maxwell-Boltzmann velocity distribution for a single Brownian particle. Next, the detection technology was further optimized and used to track optically trapped silica and barium titanate glass microspheres in water and acetone with >50 MHz bandwidth and <3 fm/rt(Hz) sensitivity. Brownian motion in a liquid is influenced by hydrodynamic, time-retarded coupling between the particle and the fluid flow its motion generates. Our measurements allowed for instantaneous velocity measurement with an SNR of up to 16 dB and confirmed the Maxwell Boltzmann distribution for Brownian motion in a liquid. The measurements also revealed several unusual features predicted for Brownian motion in the regime of hydrodynamic coupling, including faster-than-exponential decay of the velocity autocorrelation function, correlation of the thermal force and non-zero cross-correlation between the particle's velocity and the thermal force preceding it. / text

The last decade has seen substantial advances in single-molecule tracking methods with nano-metre level precision. A powerful tool in single-molecule tracking is fluorescence imaging. One particular application, total internal reflection microscopy, can capture biological processes at high contrast video rate imaging at the single-particle level. This thesis presents methodologically novel methods in analysing single particle tracking data. Presented here is an application of a Bayesian statistical approach that can discriminate between the different diffusive modes that appear with the presence of membrane architecture. This algorithm is denoted BARD; a Bayesian Analysis to Ranking Diffusion. These algorithms are applied to a total internal fluorescence microscopy based experimental data of a novel membrane probe in Escherichia coli. This probe is a plasmid expressed, non-native membrane integrating trans-membrane helix and thus acts as an ideal protein based probe under no specific native control. Two experiments were performed using a combination of varying helix probe size and growth temperature experiments effectively altering the transition temperature of the membrane. These data are suggestive of a passive partitioning of the helix protein into mobile and immobile domains that emerge from the underlying phase behaviour of the membrane.

Septinas são GTPases consideradas como um novo componente do citoesqueleto. Essas proteínas interagem entre si para formar heterocomplexos filamentosos e estruturas de alta ordem que são importantes para a citocinese e uma variedade de outros processos celulares. Existem muitos aspectos mecânicos dessas proteínas que não são totalmente compreendidos, incluindo a forma como os heterocomplexos se agrupam corretamente. Em humanos, há 13 genes que codificam septinas, classificadas em quatro grupos quanto à similaridade em relação à estrutura primária. O complexo hexamérico SEPT7-SEPT6-SEPT2-SEPT2-SEPT6-SEPT7 foi o melhor caracterizado, com uma estrutura cristalina resolvida à 4 &Aring;. Segundo às Regras de Kinoshita, as septinas desse complexo podem ser substituídas nesse arranjo por outras pertencentes ao mesmo grupo. Neste trabalho utilizamos a técnica de microscopia eletrônica de transmissão com análise de partícula única para estudar dois complexos de septinas. Um dos complexos estudados neste projeto é formado por septinas humanas, para as quais atualmente não há informações estruturais disponíveis. O complexo SEPT5-SEPT6-SEPT7 foi expresso heterólogamente em E. coli e purificado em alta concentração salina para evitar a polimerização. A análise de partículas únicas de imagens por contrastação negativa mostrou a presença de partículas alongadas de aproximadamente 25 nm de comprimento, compostos por seis monômeros, como esperado. Com o objetivo de localizar a posição da SEPT5 no complexo, foi realizada uma fusão com MBP (Maltose Binding Protein) e imunomarcação com anticorpo monoclonal anti-SEPT5, concluindo que a SEPT5 está localizada na extremidade do complexo hexamérico. Porém, a SEPT5 pertence ao mesmo grupo da SEPT2, que foi relatada estar localizada no centro do hexâmero. Este resultado possibilitou uma nova discussão sobre a maneira que as septinas formam os complexos e, como a sensibilidade à concentração salina está relacionada com a fragilidade da interface NC, análogo ao observado em complexos de Saccharomyces cerevisiae. Um complexo de Ciona intestinalis incluindo a SEPT2, SEPT6, SEPT7 e SEPT9, também expresso heterólogamente em E. coli, foi preparado por contrastação negativa. A análise de partícula única das imagens coletadas mostrou um heterocomplexo aparentemente hexamérico, embora fosse esperado um octâmero devido à presença das quatro septinas diferentes, sendo uma pertencente à cada um dos quatro grupos. Os resultados deste trabalho proporcionaram um avanço na compreensão da formação de heterocomplexos de septinas e como essas proteínas interagem umas com as outras nesta montagem. / Septins are GTPases that appear to be a novel component of the cytoskeleton. These proteins interact with each other to form filamentous heterocomplexes and high order structures which are important for cytokinesis and a variety of other cellular processes. There are many mechanistic aspects of these proteins that are not fully understood, including how the heterocomplexes correctly assemble. In humans, there are 13 genes encoding septins, classified in four groups based on primary structure. The SEPT7-SEPT6-SEPT2-SEPT2-SEPT6-SEPT7 hexameric complex was the best characterized, with a crystalline structure solved at 4 &Aring;. According to Kinoshita´s Rules, the septins of this complex can be replaced in this arrangement by others belonging to the same group. In this work, we used transmission electron microscopy with single particle analysis to study two septin complexes. One of the complexes studied in this project is composed of three human septins, for which there is currently no structural information available. The SEPT5-SEPT6-SEPT7 complex was heterologously expressed in E. coli and purified at high salt concentration to avoid polymerization. Single particle analysis of negatively stained samples showed the presence of elongated particles of approximately 25 nm in length. To locate SEPT5 in the complex, a fusion with MBP (Maltose Binding Protein) and immunoblotting with anti-SEPT5 monoclonal antibody was performed, concluding that SEPT5 is located at the end of the hexameric complex. However, SEPT5 belongs to the same group as SEPT2, which was reported to be located in the center of the hexamer. This result allowed for a new discussion on the way that septins form heterocomplexes and also, on how the sensitivity of the NC interface in related to salt concentration, analogous to that observed in the heterocomplex of Saccharomyces cerevisiae. A Ciona intestinalis complex including SEPT2, SEPT6, SEPT7 and SEPT9, also expressed heterologously in E. coli, was prepared by negative staining. The single particle analysis of the collected images showed an apparently hexameric heterocomplex, although an octamer was expected due to the presence of the four different septins, one belonging to each of the four groups. The results of this work represent advances in the understanding of the formation of septin heterocomplexes and how these proteins interact with each other during assembly.

Neurons are polarized cells with dendrites and an axon projecting from their cell body. Due to this polarized structure a major challenge for neurons is the transport of material to and from the cell body. The transport that occurs between the cell body and axons is called Axonal transport. Axonal transport has three major components: molecular motors which act as vehicles, microtubules which serve as tracks on which these motors move and microtubule associated proteins which regulate the transport of material. Axonal transport maintains the integrity of a neuron and its dysfunction is linked to neurodegenerative diseases such as, Alzheimer’s disease, Frontotemporal dementia linked to chromosome 17 and Pick’s disease. Therefore, understanding the process of axonal transport is extremely important. Single particle tracking is one method in which axonal transport is studied. This involves fluorescent labelling of molecular motors and microtubule associated proteins and tracking their position in time. Single particle tracking has shown that both, molecular motors and microtubule associated proteins exhibit motion with multiple components. These components are directed, where motion is in one direction, diffusive, where motion is random, and static, where there is no motion. Moreover, molecular motors and microtubule associated proteins also switch between these different components in a single instance of motion. We have developed a MATLAB program, called MixMAs, which specializes in analyzing the data provided by single particle tracking. MixMAs uses a sliding window approach to analyze trajectories of motion. It is capable of distinguishing between different components of motion that are exhibited by molecular motors and microtubule associated proteins. It also identifies transitions that take place between different components of motion. Most importantly, it is not limited by the number of transitions and the number of components present in a single trajectory. The analysis results provided by MixMAs include all the necessary parameters required for a complete characterization of a particle’s motion. These parameters are the number of different transitions that take place between different components of motion, the dwell times of different components of motion, velocity for directed component of motion and diffusion coefficient for diffusive component of motion. We have validated the working of MixMAs by simulating motion of particles which show all three components of motion with all the possible transitions that can take place between them. The simulations are performed for different values of error in localizing the position of a particle. The simulations confirm that MixMAs accurately calculates parameters of motion for a range of localization errors. Finally, we show an application of MixMAs on experimentally obtained single particle data of Kinesin-3 motor.

Stainless steel is one of the most commonly used materials in most industries. Excellent corrosion resistance of stainless steel is due to the formation of an oxide film on the surface (passive film), which protects the material from continuous corrosion attacks. When subjected to an attack combining corrosion and erosion, the passive film is damaged and thus, higher and unpredictable degradation rates are observed, which may result in costly consequences. In the first part of this study a model was developed for erosion enhanced corrosion of 304 stainless steel. A new device was designed and constructed, which made possible the impingement of single particles on the surface of sample material at different impact velocities and angles. Based on the electrochemical response of material to the impact of single particles, a model was proposed that considered the number of the impacting particles on the surface. The predictions made by this model were later compared with the results of a slurry jet experiment, which was used to simulate the service conditions. The second part of the research included the basic mechanical and electrochemical studies of the interactions occurring between the particle and material surface during the particle impact. This included the effects of different impact parameters such as coefficient of friction, impact angle, impact energy and particle angular velocity on depassivation of 304 stainless steel and its erosion-corrosion. A depassivation mechanism was proposed that considered a combined effect of the friction force and its effective path of action on the surface. In the last part improving the erosion-corrosion properties of 304 stainless steel was tried based on the results of the second part of the study. Samples were cold rolled and the effect of hardness on the coefficient of friction was investigated, which in the second part was proven responsible for the depassivation of the surface. It was found that the coefficient of friction between the particles and the surface remains unchanged in different applied percentages of cold work. Also it was shown that work hardening is an effective method for increasing the resistance of the material to erosion-corrosion. / Materials Engineering

X-ray lasers are creating unprecedented research opportunities in physics,chemistry and biology. The peak brightness of these lasers exceeds presentsynchrotrons by 1010, the coherence degeneracy parameters exceedsynchrotrons by 109, and the time resolution is 105 times better. In theduration of a single flash, the beam focused to a micron-sized spot has the samepower density as all the sunlight hitting the Earth, focused to a millimetresquare. Ultrafast coherent X-ray diffractive imaging (CXDI) with X-ray lasers exploitsthese unique properties of X-ray lasers to obtain high-resolution structures fornon-crystalline biological (and other) objects. In such an experiment, thesample is quickly vaporised, but not before sufficient scattered light can berecorded. The continuous diffraction pattern can then be phased and thestructure of a more or less undamaged sample recovered% (speed of light vs. speed of a shock wave).This thesis presents results from the first ultrafast X-ray diffractive imagingexperiments with linear accelerator-driven free-electron lasers and fromoptically-driven table-top X-ray lasers. It also explores the possibility ofinvestigating phase transitions in crystals by X-ray lasers. An important problem with ultrafast CXDI of small samples such as single proteinmolecules is that the signal from a single measurement will be small, requiringsignal enhancement by averaging over multiple equivalent samples. We present anumerical investigation of the problems, including the case where samplemolecules are not exactly identical, and propose tentative solutions. A new software package (Hawk) has been developed for data processing and imagereconstruction. Hawk is the first publicly available software package in thisarea, and it is released as an open source software with the aspiration offostering the development of this field.

Single particle microscopy and spectroscopy strategies reveal hidden relationships between the surface plasmon resonances (SPRs) and the sizes, shapes, and arrangements of gold nanoparticles (Au NPs). The SPR, the coherent oscillation of the conduction electrons, leads to intense absorption and scattering of light at frequencies satisfying the resonance condition determined by the size, shape, and spacings between NPs. Growing and assembling NPs through wet chemistry yields a diversity of geometries. Together, optical spectroscopy, scanning electron microscopy (SEM), and computational modeling of individual NPs and NP assemblies elucidate the resulting variety of SPRs. Strong coupling of the SPRs in linear assemblies provokes particular interest for tunable structures that will benefit surface enhanced spectroscopies and optical computing. The influence of the constituents and imperfections in such assemblies, which deviate from idealized model systems, must be established one assembly at a time. This thesis demonstrates previously unknown and sensitive relationships between the SPRs and these geometric parameters through systematic single particle experiments of self-assembled ring superstructures, nanorod dimers, individual nanorods populating different size regimes, and short linear chains of Au NPs through single particle spectroscopy. Dark-field scattering of self-assembled ring superstructures of 40 nm Au NPs reveals new plasmon modes that are redshifted from the single NP SPR by hundreds of nanometers, highly polarized along the axis of alignment, and indifferent to irregularities in the NP arrangement. SPRs of Au nanorod dimers, however, are dramatically altered by NP size heterogeneity, reduced symmetry, and metallic contact, consistent with previous studies of small assemblies. Broad band single particle extinction measurements of individual Au nanorods and short chains of 200-1000 nm long demonstrate the importance of the overall dimensions of an NP or an assembly of NPs. Finally, extinction measurements of these chains provide a compelling comparison to chemical polymers via the redshifting of the lowest energy SPR, tolerance to disorder, and the influence of the repeat unit. This result extends already well-defined analogies between plasmonic assemblies and chemical molecules to the ‘plasmonic polymer’. The findings presented in this thesis bring deeper and more detailed understanding to the tunable optical properties of real NP assemblies.

No description available.