L'effet Hall quantique, qui apparaît dans les gaz d'électrons bidimensionnels soumis à un champ magnétique perpendiculaire et à basses températures, a été un sujet de recherche intense pendant les derniers trente ans, en particulier, à cause des manifestations spectaculaires de la mécanique quantique dans les propriétés de transport à l'échelle macroscopique. Dans cette thèse, on étend l'horizon de la recherche au niveau théorique sur ce sujet en considérant les effets du couplage spin-orbite et l'interaction électron-électron de façon analytique dans ce régime.Dans la première partie de ce manuscrit, on considère l'effet simultané du couplage spin-orbite de type Rashba et l'interaction Zeeman dans le régime de l'effet Hall quantique entier. Pour cela, on étend un formalisme de fonctions de Green basé sur des états de vortex cohérents avec l'objectif d'inclure le couplage entre les degrés de liberté orbitaux et de spin dans les états de dérive électroniques. Puis, comme première application, on montre comment obtenir analytiquement, nonperturbativement et de manière contrôlée des fonctionnelles quantiques (spectre et densité d'états locale) pour des potentiels électrostatiques arbitraires et localement plats. Les fonctionnelles sont ensuite analysées dans différents régimes de températures et comparées aux données expérimentales obtenues à partir des sondes de spectroscopie locales. Comme seconde mise en pratique du formalisme, on étudie en profondeur les propriétés de transport de charge et de spin dans un régime hydrodynamique d'équilibre local (ou quasi-équilibre) et dérive des expressions analytiques qui incorporent les caractères non-relativiste et relativiste des gaz d'électrons avec couplage spin-orbite de type Rashba.Dans la deuxième partie de cette thèse, on s'occupe du problème de traiter analytiquement les fortes interactions électron-électron dans le régime de l'effet Hall quantique fractionnaire. A cette fin, on étudie un problème à deux corps généralisé avec du désordre et des corrélations électroniques, en utilisant une nouvelle représentation d'états de vortex cohérents. Des corrélations à longue portée entre les particules sont incorporées de manière topologique à travers la présence d'une métrique non-Euclidienne. Subséquemment, on montre que ces états de vortex forment bien une base d'un espace de Hilbert élargi, puis on dérive l'équation du mouvement pour la fonction de Green. Enfin, on vérifie la consistance de notre théorie pour tout niveau de Landau de paire et on discute la nécessité d'aller au-delà de la limite semiclassique (à champ magnétique infinie) pour obtenir des gaps dans chaque niveau de énergie. / The quantum Hall effect, appearing in disordered two-dimensional electron gases under strong perpendicular magnetic fields and low temperatures, has been a subject of intense research during the last thirty years due to its very spectacular macroscopic quantum transport properties. In this thesis, we expand the theoretical horizon by analytically considering the effects of spin-orbit coupling and strong electron-electron interaction in these systems.In the first part of the manuscript, we examine the simultaneous effect of Rashba spin-orbit and Zeeman interaction in the integer quantum Hall regime. Under these conditions, we extend a coherent-state vortex Green's function formalism to take into account the coupling between orbital and spin degrees of freedom within the electronic drift states. As a first application of this framework, we analytically compute controlled microscopic nonperturbative quantum functionals, such as the energy spectrum and the local density of states, in arbitrary locally flat electrostatic potential landscapes, which are then analyzed in detail in different temperature regimes and compared to scanning tunnelling experimental data. As a second application, we thoroughly study local equilibrium charge and spin transport properties and derive analytical useful formulas which incorporate the mixed non-relativistic and relativistic character of Rashba-coupled electron gases.In the second part of this thesis, we deal with the problem of analytically incorporating strong electron-electron interactions in the fractional quantum Hall regime. To this purpose, we consider a generalized two-body problem where both disorder and correlations are combined and introduce a new vortex coherent-state representation of the two-body states that naturally include long-range correlations between the electrons. The novelty of this theory is that correlations are topologically built in through the non-Euclidean metric of the Hilbert space. Next, we show that this kind of vortex states form a basis of an enlarged Hilbert space and derive the equation of motion for the Green's function in this representation. Finally, we check the consistency of our approach for any Landau level of the pair and discuss the necessity of going beyond the semiclassical (infinite magnetic field) approximation to obtain energy gaps within each energy level.

This thesis is a blend of neutron transport theory and numerical analysis. We start with the study of the problem of the Mika/Case eigenexpansion used in the solution process of the homogeneous one-speed Boltzmann neutron transport equation with anisotropic scattering for plane symmetry. The anisotropic scattering is expressed as a finite Legendre series in which the coefficients are the ``scattering coefficients'. This eigenexpansion consists of a discrete spectrum of eigenvalues with its corresponding eigenfunctions and the continuous spectrum [-1,+1] with its corresponding eigendistributions. In the general case where the anisotropic scattering can be of any (finite) order, multiple discrete eigenvalues exist and these have to be located to have the complete spectrum. We have devised a stable and robust method that locates all these discrete eigenvalues. The method is a two-step process: first the number of discrete eigenvalues is calculated and this is followed by the calculation of the discrete eigenvalues themselves, now being able to count them down and make sure none are forgotten. <p><p>During our numerical experiments, we came across what we called near-singular eigenvalues: discrete eigenvalues that are located extremely close to the continuum and hence lead to near-singular behaviour in the eigenfunction. Our solution method has been adapted and allows for the automatic detection of such a near-singular eigenvalue. <p><p>For the elements of the continuous spectrum [-1,+1], there is no non-zero function satisfying the associated eigenequation but there is a non-zero distribution that does satisfy it. It is not feasible to compute a distribution as such but one can evaluate integrals in which this distribution appears. The continuum part of the eigenexpansion can hence only be characterised by its (angular) moments. Accurate and fast numerical quadrature is needed to evaluate these integrals. Several quadrature methods have been evaluated on a representative test function. <p><p><p>The eigenexpansion was proved to be orthogonal and complete and hence can be used to represent the infinite medium Green's function. The latter is the building block of the Boundary Sources Method, an integral solution method for the neutron transport equation. Using angular and angular/spatial moments of the Green's function, it is possible to solve with high accuracy slab problems. We have written a one-dimensional slab code implementing this Boundary Sources Method allowing for media with arbitrary order anisotropic scattering. Our results are very good and the code can be considered as a benchmark code for others. <p><p><p>As a final application, we have used our code to study the discrete spectrum of a well-known scattering kernel in radiative transfer, the Henyey-Greenstein kernel. This kernel has one free parameter which is used to fit the kernel to experimental data. Since the kernel is a continuous function, a finite Legendre approximation needs to be adopted. Depending on the free parameter, the approximation order and the number of secondaries per collision, the number of discrete eigenvalues ranges from two to thirty and even more. Bounds for the minimum approximation order are derived for different requirements on the approximation: non-negativity, an absolute and relative error tolerance. <p> / Doctorat en sciences appliquées / info:eu-repo/semantics/nonPublished

L'objectif de cette thèse est de simuler l'histoire temporelle de la réponse d'un bâtiment de grande hauteur sous sollicitation sismique et de proposer des méthodologies simplifiées qui reproduisent correctement une telle réponse. Initialement, un modèle tridimensionnel par éléments finis est produit afin de valider sa fiabilité pour simuler le comportement réel du bâtiment pendant les mouvements du sol, enregistrés à l'aide d'accéléromètres. Il est proposé d'améliorer la précision du modèle numérique en imposant de multiples excitations, compte-tenu des effets de basculement et de la variabilité spatiale sur la sollicitation d'entrée. L'utilisation de fonctions de Green empiriques est proposée pour simuler la réponse sismique directement à partir d'enregistrements d'événements passés, sans avoir besoin de dessins de construction ni d'étalonnage des paramètres mécaniques. Une méthode de sommation stochastique, déjà utilisée pour prédire les mouvements du sol, est adoptée pour générer des signaux synthétiques à des hauteurs différentes du bâtiment, par extension du chemin de propagation des ondes du sol à la structure. Une représentation simplifiée du bâtiment comme une poutre homogène Timoshenko est proposée pour simuler la réponse sismique directement à partir des enregistrements des vibrations ambiantes. Des paramètres mécaniques équivalents sont identifiés à l'aide de l'interférométrie par déconvolution en termes de dispersion des ondes, de fréquences naturelles et de rapport de vitesse des ondes de cisaillement et de compression dans le milieu / The aim of this thesis is to simulate the time history response of a high rise building under seismic excitation and provide simplified methodologies that properly reproduce such response. Firstly, a detailed three-dimensional finite element model is produced to validate its reliability to simulate the real behavior of the building during ground motions, recorded using accelerometers. It is proposed to improve the accuracy of the numerical model by imposing multiple excitations, considering rocking effect and spatial variability on the input motion. The use of empirical Green's functions is proposed to simulate the seismic response directly from past event records, without the need of construction drawings and mechanical parameters calibration. A stochastic summation scheme, already used to predict ground motions, is adopted to generate synthetic signals at different heights of the building, extending the wave propagation path from the ground to the structure. A simplified representation of the building as a homogeneous Timoshenko beam is proposed to simulate the seismic response directly from ambient vibration records. Equivalent mechanical parameters are identified using deconvolution interferometry in terms of wave dispersion, natural frequencies and shear to compressional wave

We prove exponential decay for a fractional power of the Green's function for some correlated Anderson models using the fractional moment method.

Let us consider the singularly perturbed model problem Lu := -epsilon laplace u-bu_x+cu = f with homogeneous Dirichlet boundary conditions on the unit-square (0,1)^2. Assuming that b > 0 is of order one, the small perturbation parameter 0 < epsilon << 1 causes boundary layers in the solution. In order to solve above problem numerically, it is beneficial to resolve these layers. On properly layer-adapted meshes we can apply finite element methods and observe convergence. We will consider standard Galerkin and stabilised FEM applied to above problem. Therein the polynomial order p will be usually greater then two, i.e. we will consider higher-order methods. Most of the analysis presented here is done in the standard energy norm. Nevertheless, the question arises: Is this the right norm for this kind of problem, especially if characteristic layers occur? We will address this question by looking into a balanced norm. Finally, a-posteriori error analysis is an important tool to construct adapted meshes iteratively by solving discrete problems, estimating the error and adjusting the mesh accordingly. We will present estimates on the Green’s function associated with L, that can be used to derive pointwise error estimators.

Die verlässliche Vorhersage der Wärmeentzugsleistungen als auch der Soletemperaturen in den Sonden sind wichtig für deren Auslegung und Betriebsoptimierung. Es ist ebenso wichtig für die Auslegung und Optimierung der Anlagen im versorgten Gebäude. In der vorliegenden Dissertation wurde versucht, durch eine mathematische Weiterentwicklung von Greenschen Funktionen (g-Funktionen) eine präzisere Lösung für Temperaturverteilung im Erdreich infolge des von einer oder mehreren Sonden verursachten Wärmeentzuges mit verschiedenen Randbedingungen im geologischen Untergrund zu erreichen. Hierzu wurden sechs „neue“ g-Funktionen entwickelt, die vertikal variable Wärmeentzüge einzelner Sonden und Sondenfelder, eine Asymmetrie des Wärmeentzuges der Sonde, den Einfluss einer zusätzlichen Grundwasserströmung und den realen, geschichteten Untergrund berücksichtigen. Die mathematischen Modelle des Erdreichs wurden mit Modellen für die Soleströmung und Wärmeübergabe in der Hinterfüllung der Sonde gekoppelt und anschließend auf ein praktisches Betriebsbeispiel angewendet. Die Arbeit enthält ebenfalls umfangreiche Sichtung existierender Modelle sowie deren Anwendung und vergleichende Bewertung der teilweise komplexen Modellansätze.:Formelzeichen und Abkürzungen 1 Einführung 2 Energiequellen und Aufbau der Erdwärmeübertrager 2.1 Quellen der geothermalen Energie 2.2 Aufbau der Erdwärmeübertrager 2.3 Betriebsverhalten von Erdwärmesonden 2.4 Auslegung der Sonden 3 Vorhandene Modelle 3.1 Soleströmung 3.2 Wärmeübergang in den Rohren der Sonde 3.3 Wärmeleitung in der Hinterfüllung 3.4 Erdreichmodellierung – numerisch 3.5 Erdreichmodellierung mit g-Funktionen 4 Weiterentwicklung der analytischen Modelle 5 Anwendungsbeispiele 185 5.1 Ein praktisches Beispiel 5.2 Auswirkung auf die Jahresarbeitszahl 6 Zusammenfassung Literatur A Ableitung der Bohrlochwiderstände B Ableitung der Funktionen für Randbedingungen C Eidesstattliche Erklärung / The design of the ground heat exchangers (GHE) systems demands the precise prediction of their heat output and the brine temperature. The same information is needed for design and optimization of the HVAC systems coupled to GHEs. In the thesis at hand the Green’s functions (g-Functions) have been used to develop the more accurate solutions for the temperature distribution in soil resulting from the heat extraction from one GHE or a field of GHEs. These solutions consist of six novel g-functions that take account of the vertical variation of the extracted heat flux in one GHE or field of GHEs, of the horizontal ground water flow and of the horizontal variation of the soil properties. The models for prediction of the soil temperature have been coupled with models for brine flow and heat transfer in the GHE’s grout and eventually applied to the simulation of the real world object. Additionally, the thesis contains broad review of the known models and their applications as well as the comparative analysis of the complex modelling assumptions.:Formelzeichen und Abkürzungen 1 Einführung 2 Energiequellen und Aufbau der Erdwärmeübertrager 2.1 Quellen der geothermalen Energie 2.2 Aufbau der Erdwärmeübertrager 2.3 Betriebsverhalten von Erdwärmesonden 2.4 Auslegung der Sonden 3 Vorhandene Modelle 3.1 Soleströmung 3.2 Wärmeübergang in den Rohren der Sonde 3.3 Wärmeleitung in der Hinterfüllung 3.4 Erdreichmodellierung – numerisch 3.5 Erdreichmodellierung mit g-Funktionen 4 Weiterentwicklung der analytischen Modelle 5 Anwendungsbeispiele 185 5.1 Ein praktisches Beispiel 5.2 Auswirkung auf die Jahresarbeitszahl 6 Zusammenfassung Literatur A Ableitung der Bohrlochwiderstände B Ableitung der Funktionen für Randbedingungen C Eidesstattliche Erklärung

Carbon-based conductors like carbon nanotubes (CNTs) and graphene nanoribbons (GNRs) have many properties, which make them relevant for potential electronic applications. Among them are high conductances and tunable band gap sizes. These properties make CNTs and GNRs useful in many circumstances, e.g. as channel material in transistors or transparent electrodes in solar cells. Plenty of literature can be found on the topic of single linear CNTs/GNRs. Some applications however require a large network of these conductors. In addition, a single conductor has only a small impact on the network conductance, which reduces the need to control the properties of each individual nanotube/-ribbon. This leads to networks being easier to apply. In this work, the conductance of large networks of GNRs is calculated using the quantum-transport formalism (QT). This has not been done before in literature. In order to apply QT to such a large amount of atoms, the recursive Green's function formalism is used. For this the networks are devided into subcells, which are represented by tight-binding matrices. Similar networks are also examined using two different nodal analysis (NA) approaches, where the nanoribbons are treated as ohmic conductors. For NA with one-dimensional conductors, major discrepancies are found in regards to the QT model. However, networks consisting of two-dimensional conductors (NA-2D) have many properties similar to the QT networks. A recipe to approximate the QT results with NA-2D is presented.:1. Introduction 2. Theoretical Principles 2.1 Carbon-based Conductors 2.1.1 Structure and Properties 2.1.2 Networks 2.2 Tight-Binding Model 2.3 Quantum Transport 2.3.1 Introduction 2.3.2 Level Broadening 2.3.3 Current Flow 2.3.4 Transmission 2.4 Nodal Analysis 3. Implementation 3.1 Quantum Tranport 3.1.1 Network Generation 3.1.2 Density-Functional based Tight-Binding Method 3.1.3 Recursive Green's Function Algorithm 3.1.4 Conductance 3.2 Nodal Analysis 3.2.1 One-dimensional Conductors 3.2.2 Two-dimensional Conductors 4. Results 4.1 Quantum Transport 4.1.1 Band Structures and Fermi Energies 4.1.2 Ideal Transmission and Consistency Tests 4.1.3 Percolation 4.1.4 Transmission 4.1.5 Conductance 4.1.6 Power Law Scaling 4.1.7 Size Dependence and Confinement Effects 4.1.8 Calculation Time 4.2 Nodal Analysis 4.2.1 One-dimensional Conductors 4.2.2 Two-dimensional Conductors 4.2.3 Calculation Time 4.3 Approximating QT with NA 4.3.1 Optimal Parameters 4.3.2 Percolation 4.3.3 Conductance 4.3.4 Power Law Scaling 5. Conclusions / Graphenbasierte Leiter wie Kohlenstoff-Nanoröhrchen (engl. 'carbon nanotubes', CNTs) oder Graphen-Nanobänder (engl. 'graphene nanoribbons', GNRs) haben viele Eigenschaften, die sie für potenzielle elektronische Anwendungen interessant machen. Darunter sind hohe Leitfähigkeiten und einstellbare Bandlückengrößen. Dadurch sind CNTs und GNRs in vielen Bereichen nützlich, z.B. als Kanalmaterial in Transistoren oder als transparente Elektroden in Solarzellen. Es gibt viel Literatur über einzelne, lineare CNTs/GNRs. Einige Anwendungen benötigen jedoch ein großes Netzwerk dieser Leiter. Zusätzlich hat ein einzelner Leiter wenig Einfluss auf die Leitfähigkeit des Netzwerks, wodurch die Eigenschaften der einzelnen Nanoröhrchen/-streifen weniger streng kontrolliert werden müssen. Dies führt dazu, dass es einfacher ist Netzwerke zu nutzen. In dieser Arbeit wird die Leitfähigkeit von großen GNR-Netzwerken mittels Quantentransport (QT) berechnet. Dies wurde in der Literatur noch nicht getan. Um QT auf eine so große Menge an Atomen anzuwenden wird der rekursive Greenfunktions-Formalismus benutzt. Dazu werden die Netzwerke in Unterzellen unterteilt, die durch Tight-Binding-Matrizen dargestellt werden. Ähnliche Netzwerke werden auch mit zwei Versionen der Knotenanalyse (engl. 'nodal analysis', NA) untersucht, welche die Nanobänder wie ohmische Leiter behandelt. Die Ergebnisse der NA mit eindimensionalen Leitern weisen deutliche Unterschiede zu den mit QT erzielten Ergebnissen auf. Wenn jedoch zweidimensionale Leiter in NA verwendet werden (NA-2D) gibt es viele parallelen zu den QT Ergebnissen. Zuletzt wird ein Vorgehen präsentiert, mit dem QT Resultate durch NA-2D Rechnungen genähert werden können.:1. Introduction 2. Theoretical Principles 2.1 Carbon-based Conductors 2.1.1 Structure and Properties 2.1.2 Networks 2.2 Tight-Binding Model 2.3 Quantum Transport 2.3.1 Introduction 2.3.2 Level Broadening 2.3.3 Current Flow 2.3.4 Transmission 2.4 Nodal Analysis 3. Implementation 3.1 Quantum Tranport 3.1.1 Network Generation 3.1.2 Density-Functional based Tight-Binding Method 3.1.3 Recursive Green's Function Algorithm 3.1.4 Conductance 3.2 Nodal Analysis 3.2.1 One-dimensional Conductors 3.2.2 Two-dimensional Conductors 4. Results 4.1 Quantum Transport 4.1.1 Band Structures and Fermi Energies 4.1.2 Ideal Transmission and Consistency Tests 4.1.3 Percolation 4.1.4 Transmission 4.1.5 Conductance 4.1.6 Power Law Scaling 4.1.7 Size Dependence and Confinement Effects 4.1.8 Calculation Time 4.2 Nodal Analysis 4.2.1 One-dimensional Conductors 4.2.2 Two-dimensional Conductors 4.2.3 Calculation Time 4.3 Approximating QT with NA 4.3.1 Optimal Parameters 4.3.2 Percolation 4.3.3 Conductance 4.3.4 Power Law Scaling 5. Conclusions

<p>Dipole-dipole interactions are ubiquitous fundamental physical phenomena that govern physical effects such as Casimir Forces, van der Waals forces, collective Lamb shifts, cooperative decay, and resonance energy transfer. These interactions are associated with real and virtual photon exchange between the interacting emitters. Such interactions are crucial in realizing quantum memories, novel super-radiant light sources, and light-harvesting devices. Owing to this, the control and modification of dipole-dipole interactions have been a longstanding theme. The electromagnetic environment plays a crucial role in enhancing the range and strength of the interactions. This work focuses on modifying the nanophotonic environment near interacting emitters to enhance dipole-dipole interactions instead of spontaneous emission. To this end, we focus on engineering the nanophotonic environment to enhance the strength and range of dipole-dipole interactions between an ensemble of emitters. We explore ordered and disordered nanophotonic structures. We experimentally demonstrate long-range dipole-dipole interactions mediated by surface lattice resonances in a periodic plasmonic nanoparticle lattice. Further, the modified electromagnetic environment reduces the apparent dimensionality of the interacting system compared to non-resonant in-homogeneous and homogeneous environments. We also develop a spectral domain inverse design technique for the accelerated discovery of disordered metamaterials with unique spectral features. </p> <p>Further, we explore the novel regimes of light localization at near-zero-index in such disordered media. The disordered near-zero-index medium reveals enhanced localization and near-field chirality. This work paves the way to engineer the electromagnetic nanophotonic environment to realize enhanced long-range dipole-dipole interactions.</p>

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