La plupart des matériaux étudiés en physique de la matière condensée sont à base de fermions massifs vérifiant les relations de dispersion paraboliques usuelles. Récemment, sont apparus un certain nombre de matériaux dotés de relations de dispersion linéaires : le graphène, système purement bidimensionnel et les isolants topologiques, composés tridimensionnels à base de Bismuth où les fermions de Dirac surfaciques coexistent avec les fermions massifs volumiques. À côté de ces deux grandes familles de matériaux de Dirac, on trouve le composé organique α-(BEDT-TTF)2I3, un système quasi-bidimensionnel du point de vue du transport électronique en raison de sa structure cristalline lamellaire et qui présente une phase de Dirac sous forte pression hydrostatique (P>1,5 GPa). Cette phase de Dirac est singulière puisque ses cônes de Dirac sont inclinés, et donc fortement anisotropes, et qu'ils émergent aux côtés d'une bande de porteurs de charge massifs. Ce travail de thèse porte ainsi sur l'étude, à la fois expérimentale et théorique, des effets des spécificités de la phase de Dirac du α-(BEDT-TTF)2I3 sur son transport électronique en régime quantique. Il examine notamment plusieurs modèles théoriques pour tenter d'interpréter les oscillations quantiques apériodiques mesurées dans le composé organique, ainsi que l'impact de l'inclinaison des cônes de Dirac. Les effets de dopage, surfacique et volumique, sur le α-(BEDT-TTF)2I3 sont également discutés. / The physics of most of the materials studied within condensed matter are based on massive fermions which verify the usual parabolic dispersion relations. Recently, a certain number of materials with linear dispersion relation have appeared: graphene, purely bidimensional and topological insulators, tridimensional compounds based on Bismuth where the surfacic Dirac fermions coexist with bulk massive fermions. Alongside these two families of Dirac materials, there is the organic α-(BEDT-TTF)2I3 compound, a quasi-bidimensional system from an electronic transport point of view because of its lamellar crystalline structure and which exhibits a Dirac phase under high hydrostatic pressure (P>1,5 GPa). This Dirac phase is singular: the Dirac cones are tilted, and highly anisotropic, and they emerge with a massive band. This work is then focus on the study, experimentally and theoretically, of the effects of the α-(BEDT-TTF)2I3 Dirac phase specificities on its electronical transport in quantum regime. It examines particularly several theoretical models to understand the aperiodic quantum oscillations measured in the organic compound, and the impact of Dirac cones tilting. Doping effects, surfacic and in the bulk, on the α-(BEDT-TTF)2I3 are also discussed.

This study investigates the complex flow structure generated by riparian emergent vegetation along the edge of floodplain. Detailed velocity and boundary shear stress measurements were carried out for various arrangements of emergent rigid cylindric rods of 3 mm, 6 mm and 9 mm diameters and for three different rod densities. In addition, the impact of foliage on the flow field was assessed during a series of experiments where brushes were used instead of smooth rods. The results of these new experiments are first presented. In addition to the laboratory data, field data was obtained through Acoustic Doppler Current Profiler measurements for two flood events in a stretch of the river Rhône that can be approximated to a straight compound channel with vegetated banks. The analysis of the flow structure highlights the presence of strong secondary circulation and increased vorticity on the river banks. The rods on the edge of the floodplain increase significantly flow resistance, reducing velocity and decreasing boundary shear stress. Flow rate was seen to decrease with increasing vegetative density for all cases except when foliage was added. This suggests that an optimum threshold density, for which a smaller density would lead to an increased flow rate might exist. Wakes trailing downstream of the vegetation stem, planform coherent structures advected between the main channel and the floodplain, and eddying motion in the flow due to enhanced turbulence anisotropy are among the defining patterns observed in the studied compound channel flows with one line of emergent vegetation along the edge of the floodplain. The Shiono and Knight Method (SKM) was modified in order to account for the increased turbulence activity due to the rods. The drag force term was introduced in the same way as in the work of Rameshwaran and Shiono (2007). However, a new term was added to the transverse shear stress term in the form of an Elder formulation, incorporating a friction drag coefficient which can be derived from the experimental data. In this proposed version, the advection term was set to zero. Another version of the SKM, similar to Rameshwaran and Shiono (2007), was also tested with the addition of a local drag friction only applied in the rod region. The proposed SKM version without the advection term was favored as it can be more closely related to the experimental data and to physical processes. Finally, the capabilities of Telemac-2D were tested against the experimental data for various turbulence models. The Large Eddy Simulation turbulence model highlighted some unsteady flow patterns that were observed during experiments, while satisfactorily predicting the lateral velocity and boundary shear stress distributions.

<p>Spin-imbalanced Fermi gases serve as a testbed for fundamental notions and are efficient table-top emulators of a variety of quantum matter ranging from neutron stars, the quark-gluon plasma, to high critical temperature superconductors. A macroscopic quantum phenomenon which occurs in spin-imbalanced Fermi gases is that of phase separation; in three dimensions, a spin-balanced, fully-paired superfluid core is surrounded by an imbalanced normal-fluid shell, followed by a fully polarized shell. In one-dimension, the behavior is reversed; a balanced phase appears outside a spin-imbalanced core. This thesis details the first density profile measurements and studies on spin-imbalanced quasi-2D Fermi gases, accomplished with high-resolution, rapid sequential spin-imaging. The measured cloud radii and central densities are in disagreement with mean-field Bardeen-Cooper-Schrieffer theory for a 2D system. Data for normal-fluid mixtures are well fit by a simple 2D polaron model of the free energy. Not predicted by the model is an observed phase transition to a spin-balanced central core above a critical polarization.</p> / Dissertation

The flow characteristics in compound channels with and without vegetation on the floodplain were investigated experimentally and numerically in this thesis. Detailed measurements of velocity and boundary shear stress, using a Pitot tube and an acoustic Doppler velocimeter together with a Preston tube, were undertaken to understand the flow characteristics in compound channels. Eight no-rod cases, two emergent-rod cases and two submerged-rod cases were tested. Unsteady large eddies that occur in the shear layer were explored numerically with Large Eddy Simulation (LES) to identify its generation and its effects on the flow behaviors. Mean flow parameters were predicted using the quasi-2D model by considering the shear effect. Usirgg the data of depth-averaged velocity and boundary shear stress, the contributions of shear-generated turbulence and bed-generated turbulence to the Reynolds shear stress were identified, the apparent shear stress was calculated using the modified method of Shiono and Knight (1991) and the depth-averaged secondary current force was then obtained. Large eddies were important to the lateral momentum exchange in shallow non-vegetated compound channels and even in deep vegetated compound channels. In the compound channel with one-line rods at the floodplain edge, the secondary current forces were of opposite signs in the main channel and on the floodplain and the bed shear stress was smaller than the standard two-dimensional value of yHSo due to the vegetation effect, where y,H,So are the specific weight of water, water depth and bed slope respectively. In vegetated compound channels, the velocity patterns were different to those and the discharges were smaller than those in non-vegetated compound channels under similar relative water depth conditions. The anisotropy of turbulence was the main contribution to the generation of secondary currents in non-vegetated and vegetated compound channels, but the Reynolds stress term was more important in the vegetated compound channels. Results of cross spectra showed the mechanisms of the turbulent shear generation near the main channel-floodplain junction are due to large eddies in the non-vegetated compound channel and owing to wakes in the vegetated compound channel. LES results indicated that large eddies caused significant spatial and temporal fluctuations of velocity and water level in the compound channel and the instantaneousv alues of these flow parameters were significantly higher than the mean values. In vegetated compound channels, the flow moved from the main channel to the floodplain and from the floodplain to the main channel alternately. The characteristic frequencies of the large eddy were less than 1Hz which was consistent with the experimental data. The capability of the quasi-2D model to predict the 2D mean flow parameters in compound channels were assessed under different flow conditions and also improved by using the mean wall velocity as the boundary condition and appropriate values of the lateral gradient of the secondary current force. In the vegetated compound channels, new approaches were proposed to treat the drag force in the cases of oneline emergent rods at the floodplain edge and submerged rods on the floodplain.

In this work, the crystal growth as well as structural and magnetic investigations of several metal trichalcogenides compounds with a general formula M2X2Ch6 are presented. M stands for a main group metal or transition metal, X is an element of the IV or V main group and Ch is a chalcogen. In particular, these compounds are the phosphorus sulfides Fe2P2S6, Ni2P2S6 as well as intermediate compounds of the substitution regime (Fe1-xNix)2P2S6, the quarternary phosphorus sulfides CuCrP2S6 and AgCrP2S6 and the germanium tellurides Cr2Ge2Te6 and In2Ge2Te6. As members of the metal trichalcogenides, all these compounds have a van der Waals layered honeycomb structure in common. This layered structure in combination with their magnetic properties makes these compounds interesting candidate materials for the production of magnetic monolayers by exfoliation from bulk crystals. Crystals of the phosphorus sulfides were grown by the chemical vapor transport technique and, for the growth of the germanium tellurides, the self-flux growth technique was used. Crystals of all phases were extensively characterized regarding their morphology, chemical composition and homogeneity as well as regarding their crystal structure. The structural analysis, especially for Ni2P2S6, yields insight into details of the stacking order and disorder of the corresponding quasi-two-dimensional layers in the bulk. Regarding the magnetic properties, both Fe2P2S6 and Ni2P2S6 order antiferromagnetically but exhibit different magnetic anisotropies (i.e. Ising-like anisotropy for Fe2P2S6 and XYZ anisotropy for Ni2P2S6). In this context, it is surprising to find that compounds in the solid solution regime of (Fe1-xNix)2P2S6 up to x = 0.9 exhibit an anisotropic magnetic behavior that is comparable to Fe2P2S6 and, thus, indicative of Ising-like anisotropy. For CuCrP2S6 and AgCrP2S6, the ordering of the two different transition elements on the honeycomb sites yields more complex magnetic structures. The magnetic Cr3+ atoms in CuCrP2S6 order in a triangular arrangement and form an antiferromagnetic ground state with notable ferromagnetic interactions. AgCrP2S6 exhibits pronounced features of low dimensional magnetism resulting from the (quasi-)one-dimensional stripe-like arrangement of magnetic Cr3+ atoms and no onset of long-range magnetic order is unambiguously observed. Cr2Ge2Te6 exhibits ferromagnetic order and an anisotropic feature in the temperature dependence of the magnetization. Based on the magnetic phase diagrams for two orientations between the magnetic field and the crystallographic directions, the temperature dependence of the magnetocrystalline anisotropy constant as well as the critical exponents of the magnetic phase transition are extracted. Concluding from this, the magnetic interactions in Cr2Ge2Te6 are dominantly of two-dimensional nature and the anisotropy is uniaxial with the before mentioned anisotropic feature resulting from the interplay between magnetocrystalline anisotropy, magnetic field, and temperature. In2Ge2Te6 is diamagnetic as to be expected for a closed-shell system. Additional to the investigations on single crystals, the quasi-binary phase diagram of (Cu1-xAgx)CrP2S6 was investigated for regimes of solid solution behavior based on polycrystalline samples. Accordingly, isostructural substitution is most likely possible in the composition range of (Cu0.25Ag0.75)CrP2S6 to AgCrP2S6, potentially allowing to tune the magnetic interactions of the Cr sublattice indirectly by substitution on the Cu/Ag sublattice.:1. Introduction 1.1. M2X2Ch6 Class of Materials 1.2. Magnetism in Solid State Materials 1.2.1. Diamagnetism 1.2.2. Paramagnetism 1.2.3. Cooperative Magnetism 1.2.4. Magnetic Anisotropy 1.2.5. Magnetism in D < 3 1.2.6. Critical Exponents 2. Methods 2.1. Synthesis and Crystal Growth 2.1.1. Solid State Synthesis 2.1.2. Crystal Growth via the Liquid Phase 2.1.3. Crystal Growth via the Vapor Phase 2.2. X-ray Diffraction 2.2.1. Single Crystal X-ray Diffraction 2.2.2. Powder X-ray Diffraction 2.3. Scanning Electron Microscopy and Energy Dispersive X-ray Spectroscopy 2.3.1. Scanning Electron Microscopy 2.3.2. Energy Dispersive X-ray Spectroscopy 2.4. Magnetometry 2.5. Nuclear Magnetic Resonance Spectroscopy 2.6. Specific Heat Capacity 3. M2P2S6 3.1. Ni2P2S6 3.1.1. Crystal Growth 3.1.2. Characterization 3.1.3. Magnetic Properties 3.1.4. 31P-NMR Spectroscopy 3.1.5. Stacking (Dis-)Order in Ni2P2S6 3.2. (Fe1-xNix)2P2S6 3.2.1. Synthesis and Crystal Growth 3.2.2. Characterization 3.2.3. Evolution of Magnetic Properties 3.3. Summary and Outlook 4. M1+CrP2S6 4.1. CuCrP2S6 4.1.1. Crystal Growth 4.1.2. Characterization 4.1.3. Magnetic Properties 4.2. AgCrP2S6 4.2.1. Crystal Growth 4.2.2. Characterization 4.2.3. Magnetic Properties 4.3. Polycrystalline (Cu1-xAgx)CrP2S6 4.3.1. Synthesis 4.3.2. Phase Analysis 4.4. Summary and Outlook 5. M2(Ge,Si)2Te6 5.1. Cr2Ge2Te6 5.1.1. Crystal Growth 5.1.2. Characterization 5.1.3. Magnetic Properties 5.1.4. Analysis of the Critical Behavior 5.2. In2Ge2Te6 5.2.1. Crystal Growth 5.2.2. Characterization 5.2.3. Magnetic Properties 5.2.4. Specific Heat 5.3. Summary and Outlook 6. Conclusion Bibliography List of Publications Acknowledgements Eidesstattliche Erklärung A. Appendix A.1. Scanning Electron Microscopic Images A.1.1. (Fe1-xNix)2P2S6 A.2. scXRD A.2.1. (Fe1-xNix)2P2S6 / In dieser Arbeit werden die Kristallzüchtung sowie strukturelle und magnetische Untersuchungen an mehreren Metalltrichalkogenid-Verbindungen mit der allgemeinen Summenformel M2X2Ch6 vorgestellt. M steht für ein Hauptgruppen- oder Übergangsmetall, X ist ein Element der IV- oder V-Hauptgruppe und Ch ein Chalkogen. Insbesondere handelt es sich bei diesen Verbindungen um die Phosphorsulfide Fe2P2S6, Ni2P2S6 sowie um Verbindungen der Substitutionsreihe (Fe1-xNix)2P2S6, die quaternären Phosphorsulfide CuCrP2S6 und AgCrP2S6 sowie die Germaniumtelluride Cr2Ge2Te6 und In2Ge2Te6. Als Mitglieder der Metalltrichalkogenide haben alle diese Verbindungen eine van-der-Waals-Schichtstruktur mit Honigwabenmotiv gemein. Diese Schichtstruktur in Kombination mit ihren magnetischen Eigenschaften macht diese Verbindungen zu interessanten Kandidaten für die Herstellung von magnetischen Monolagen durch Exfoliation aus Volumenkristallen. Kristalle der Phosphorsulfide wurden mit der chemischen Dampfphasentransporttechnik gezüchtet und für die Züchtung der Germaniumtelluride wurde die Selbstflusstechnik verwendet. Die Kristalle aller Phasen wurden sowohl hinsichtlich ihrer Morphologie, chemischen Zusammensetzung und Homogenität als auch hinsichtlich ihrer Kristallstruktur umfassend charakterisiert. Die Strukturanalyse, insbesondere für Ni2P2S6, gibt Aufschluss über Details der Stapelordnung und -unordnung der entsprechenden quasizweidimensionalen Schichten im Volumen. Bezüglich der magnetischen Eigenschaften ordnen sowohl Fe2P2S6 als auch Ni2P2S6 antiferromagnetisch, zeigen aber unterschiedliche magnetische Anisotropien (d.h. Ising-artige Anisotropie für Fe2P2S6 und XYZ-Anisotropie für Ni2P2S6). In diesem Zusammenhang ist es überraschend, dass Verbindungen im Mischkristallregime von (Fe1-xNix)2P2S6 bis x = 0.9 ein anisotropes magnetisches Verhalten zeigen, das mit dem von Fe2P2S6 vergleichbar ist und daher auf Ising-artige Anisotropie hindeutet. Bei CuCrP2S6 und AgCrP2S6 führt die Anordnung der beiden unterschiedlichen Übergangselemente auf den Gitterplätzen der Wabenstruktur zu komplexeren magnetischen Strukturen. Die magnetischen Cr3+ Atome in CuCrP2S6 ordnen sich in einer Dreiecksanordnung an und bilden einen antiferromagnetischen Grundzustand mit ausgeprägten ferromagnetischen Wechselwirkungen. AgCrP2S6 weist deutliche Merkmale von niederdimensionalem Magnetismus auf, welche aus der (quasi-)eindimensionalen, streifenartigen Anordnung der magnetischen Cr3+ Atome resultieren, und das Einsetzen von langreichweitiger magnetischer Ordnung kann nicht eindeutig beobachtet werden. Cr2Ge2Te6 weist ferromagnetische Ordnung und einen anisotropen Verlauf der Temperaturabhängigkeit der Magnetisierung auf. Anhand von magnetischen Phasendiagrammen für zwei Orientierungen zwischen Magnetfeld und kristallographischen Richtungen wurden die Temperaturabhängigkeit der magnetokristallinen Anisotropiekonstante sowie die kritischen Exponenten des magnetischen Phasenübergangs extrahiert. Hieraus ergibt sich, dass die magnetischen Wechselwirkungen in Cr2Ge2Te6 überwiegend zweidimensionaler Natur sind und die Anisotropie uniaxial ist, wobei der zuvor erwähnte anisotrope Verlauf aus dem Zusammenspiel von magnetokristalliner Anisotropie, Magnetfeld und Temperatur resultiert. In2Ge2Te6 ist diamagnetisch, wie es für ein System mit geschlossener Schale zu erwarten ist. Zusätzlich zu den Untersuchungen an Einkristallen wurde das quasibinäre Phasendiagramm von (Cu1-xAgx)CrP2S6 anhand von polykristallinen Proben auf Bereiche mit Mischkristallverhalten hin untersucht. Folglich ist eine isostrukturelle Substitution höchstwahrscheinlich im Zusammensetzungsbereich von (Cu0.25Ag0.75)CrP2S6 bis AgCrP2S6 möglich, was es erlauben könnte, die magnetischen Wechselwirkungen des Cr-Untergitters indirekt durch Substitution auf dem Cu/Ag-Untergitter zu beeinflussen.:1. Introduction 1.1. M2X2Ch6 Class of Materials 1.2. Magnetism in Solid State Materials 1.2.1. Diamagnetism 1.2.2. Paramagnetism 1.2.3. Cooperative Magnetism 1.2.4. Magnetic Anisotropy 1.2.5. Magnetism in D < 3 1.2.6. Critical Exponents 2. Methods 2.1. Synthesis and Crystal Growth 2.1.1. Solid State Synthesis 2.1.2. Crystal Growth via the Liquid Phase 2.1.3. Crystal Growth via the Vapor Phase 2.2. X-ray Diffraction 2.2.1. Single Crystal X-ray Diffraction 2.2.2. Powder X-ray Diffraction 2.3. Scanning Electron Microscopy and Energy Dispersive X-ray Spectroscopy 2.3.1. Scanning Electron Microscopy 2.3.2. Energy Dispersive X-ray Spectroscopy 2.4. Magnetometry 2.5. Nuclear Magnetic Resonance Spectroscopy 2.6. Specific Heat Capacity 3. M2P2S6 3.1. Ni2P2S6 3.1.1. Crystal Growth 3.1.2. Characterization 3.1.3. Magnetic Properties 3.1.4. 31P-NMR Spectroscopy 3.1.5. Stacking (Dis-)Order in Ni2P2S6 3.2. (Fe1-xNix)2P2S6 3.2.1. Synthesis and Crystal Growth 3.2.2. Characterization 3.2.3. Evolution of Magnetic Properties 3.3. Summary and Outlook 4. M1+CrP2S6 4.1. CuCrP2S6 4.1.1. Crystal Growth 4.1.2. Characterization 4.1.3. Magnetic Properties 4.2. AgCrP2S6 4.2.1. Crystal Growth 4.2.2. Characterization 4.2.3. Magnetic Properties 4.3. Polycrystalline (Cu1-xAgx)CrP2S6 4.3.1. Synthesis 4.3.2. Phase Analysis 4.4. Summary and Outlook 5. M2(Ge,Si)2Te6 5.1. Cr2Ge2Te6 5.1.1. Crystal Growth 5.1.2. Characterization 5.1.3. Magnetic Properties 5.1.4. Analysis of the Critical Behavior 5.2. In2Ge2Te6 5.2.1. Crystal Growth 5.2.2. Characterization 5.2.3. Magnetic Properties 5.2.4. Specific Heat 5.3. Summary and Outlook 6. Conclusion Bibliography List of Publications Acknowledgements Eidesstattliche Erklärung A. Appendix A.1. Scanning Electron Microscopic Images A.1.1. (Fe1-xNix)2P2S6 A.2. scXRD A.2.1. (Fe1-xNix)2P2S6

Les écoulement confinés soumis à un fort champ magnétique vertical et les écoulements en rotation autour d'un axe vertical présentent au moins deux caractéristiques communes marquantes : d'une part, le champ de vitesse est quasi-bidimensionnel loin des parois, et d'autre part, une couche limite de structure simple se développe le long des parois perpendiculaires à la direction du champ magnétique (couche de Hartmann) ou à l'axe de rotation (couche d'Ekman). Nous présentons ici une étude de ces propriétés remarquables dans des cas où les autres forces qui agissent sur l'écoulement (inertie, viscosité,...) ne sont plus négligeables devant la force de Laplace ou de Coriolis. Il est montré que la combinaison des couplages verticaux et horizontaux conduit d'une part, à une dépendance quadratique du champ de vitesse en fonction de la verticale (effet tonneau), et d'autre part à la présence de jet dans les couches de Hartmann ou d'Ekman. Une loi de paroi analytique pour diverses configurations des couches de Hartmann est construite (présence d'effets inertiels, présence d'une composante horizontale du champ magnétique, parois conductrices...) dans le but d'éviter le maillage fin que requiert le calcul numérique direct d'une telle couche. Les propriétés remarquables des écoulements quasi-2D sont ensuite utilisées pour construire trois modèles 2D différents, à partir de la moyenne verticale des équations du mouvement. Ces modèles simples, ne reposent que sur les hypothèses physiques et ne nécessitent en particulier aucun étalonnage numérique. Le modèle PSM2000 pour les écoulements MHD avec inertie et sous fort champ vertical conduit à des résultats très proches de l'expérience et met notamment en évidence le fait que le pompage d'Ekman dans les couches de Hartmann se traduit approximativement par une diffusion du champ de vorticité le long des lignes de courant de l'écoulement moyen. Un modèle analogue, mais sans effets inertiels et avec un champ non homogène et instationnaire permet en premier lieu de déterminer dans quel cas les couches de Hartmann contrôlent l'écoulement global et en second lieu, d'étudier la possibilité de contrôler un écoulement d'acier liquide par un champ glissant dans un procédé de coulée continue. Finalement, un modèle quasi-géostrophique modifié fournit une base théorique pour l'étude du comportement des couches parallèles lors des expériences de Spin-Up et Spin-Down d'une cuve tournante.

This thesis describes investigations into the properties of -phase BEDT-TTF charge transfer salts. Charge transfer salts are mainly studied as they are very useful test beds for fundamental physics due to the tuneability of their proper- ties and ground states. The effects of temperature and pressure on such systems have been studied, as these allow access to a wide range of different states and properties. Transport properties of these systems have been studied to obtain information about the Fermi surface and effective mass, and the effect of deuter- ation and also change of pressure media will be discussed. The interaction of infrared radiation with these systems has also been investigated and simultaneous pressure and temperature measurements will be presented, something not greatly studied due to the large technical challenges. The techniques and approaches for overcoming these are also discussed. Chapter 1 provides an introduction to the organic materials themselves with particular emphasis on the actual compounds studied. Chapter 2 provides the necessary theoretical background for studying organic charge transfer salts using magnetic quantum oscillations and their infrared re- ectivity. Chapter 3 covers the experimental techniques and also discusses some of the challenges encountered and their solutions to aid others working in this area. Chapter 4 describes an investigation into the transport properties of - (ET)2Cu(SCN)2 by studying Shubnikov-de Haas oscillations using both deuter- ated and normal samples and using two different pressure media, and comparing it to work done using a third. Chapter 5 presents an investigation into the pressure dependence of selected phonon modes in -(ET)2Cu(SCN)2 using infrared radiation on a deuterated sam- ple. Chapter 6 presents what is believed to be the first pressure and temperature dependent infrared study of an organic molecular material. In this case the or- ganic molecular material is d8--(ET)2Cu[N(CN)2]Br, but the techniques should be readily transferable to other materials.