Abstract The main object of this thesis was to research injection mouldable 0–3 type ceramic polymer composites and their dielectric and magnetic properties in the GHz frequency region. The work has been divided into three sections. In the first section, two–phase ceramic polymer composites containing dielectric and magnetic fillers have been investigated and their characteristics analysed by reference to pre–existing mixing rules. The exploitation of these composites in miniaturizing devices, such as antennae, is presented and discussed. The second part describes three phase composites containing different nanosize additives (silver, silicon and alumina fibres) towards improving their dielectric properties. In the third part, some periodical and multilayer structures for ceramic polymer composite layers are proposed. In the case of two–phase ceramic polymer composites, with 37 vol.% of dielectric filler (Barium Strontium Titanate, BST) embedded into a thermoplastic polymer (ER140) matrix, the highest measured relative permittivity was 15 with a dielectric loss value of 0.008 at 1 GHz. With 43 vol.% of magnetic filler (hexaferrite, CO2Z) in ER182 matrix, the highest achieved relative permeability was 1.8 with a magnetic loss value of 0.077 at 1 GHz. Composites with Co2Z filler provide a 77% size reduction, and could thus be used advantageously in antennae. It was found that a 2–6 vol.% nanoaddition in BST–ER140 composites enhanced the relative permittivity drastically with only a minor effect on the dielectric losses. In particular, with only 2 vol.% addition of nanosize silver particles into the BST–ER140 composite, a 52% increase in the relative permittivity was obtained, with no significant change in the dielectric losses (tan δε = 0.004). Vertically and horizontally periodical dielectric composite structures comprising layers of different dielectric properties have been fabricated as well as multilayered structures containing dielectric and magnetic layers. The measurement results indicate that such multimaterial multilayer structures are good candidates for components with reduced dielectric and magnetic losses. / Tiivistelmä Väitöstyön tavoitteena oli tutkia ruiskuvalettavien 0–3 –liitännäisten keraami-polymeerikomposiittien ominaisuuksia erityisesti niiden GHz-taajuusalueen dielektristen ja magneettisten ominaisuuksien kannalta. Työ on jaettu kolmeen osaan. Ensimmäisessä osassa on tutkittu kaksikomponenttisia keraami-polymeerikomposiitteja, joissa täytemateriaali on joko dielektristä tai magneettista materiaalia. Komposiittien ominaisuuksia on analysoitu jo olemassa olevien seosmallinnuskaavojen avulla. Komposiittien hyödyntämistä erilaisten sovellusten, kuten antennien, minityrisoinnissa on myös käsitelty. Toinen osa käsittelee kolmikomponenttisia komposiitteja, joissa lisäaineena on käytetty pieniä määriä nanomateriaaleja (hopea- ja piipartikkelit sekä alumiinioksidikuitu) tarkoituksena parantaa komposiitin dielektrisiä. Kolmannessa osassa on tutkittu periodisia ja monikerroksisia keraami- polymeerikomposiittirakenteita rakenteita. Kaksikomponenttisten keraami-polymeerikomposiittien tapauksessa suurin permittiivisyyden arvo 15 dielektristen häviöiden ollessa 0.008 (mittaustaajuus 1 GHz) saatiin komposiitille, jossa dielektristä täytemateriaalia (Barium Strontium Titanaatti, BST) oli 37 tilavuus-% termoplastisessa polymeerimatriisissa (ER140). Korkein saavutettu permeabiliteetin arvo 1.8 magneettisten häviöiden ollessa 0.077 (mittaustaajuus 1 GHz) saatiin komposiitille, jossa magneettista täyteainetta (hexaferriitti, Co2Z) oli 43 tilavuus-% ER182 -matriisissa. Tämä täyteaine mahdollistaa nykyistä jopa 77 % pienempien antennielementtien kehittämisen. Tukimuksessa todettiin 2–6 tilavuus-% nanomateriaalin lisäyksen BST-ER140 -komposiitteihin kasvattavan permittiivisyyttä merkittävästi juurikaan vaikuttamatta dielektrisiin häviöihin. Erityisesti 2 tilavuus-% hopeananopartikkeleiden lisäys BST-ER140 -komposiitteihin kasvatti permittiivisyyttä 52 % dielektristen häviöiden (tan δε =  0.004) kasvamatta. Työssä on myös tutkittu periodisesti (vertikaali ja horisontaali) koostettuja dielektrisiä komposiittirakenteita, jossa eri kerroksissa on erilaiset dielektriset ominaisuudet sekä monikerrosrakenteita, joissa vuorottelevat dielektriset ja magneettiset kerrokset. Mittaukset osoittivat, että monimateriaaliset monikerrosrakenteet ovat hyviä kandidaatteja komponentteihin, jotka vaativat pieniä dielektrisiä ja magneettisiä häviöitä.

This thesis was inspired by the discovery of Bi14Rh3I9, the first so-called weak three-dimensional topological insulator (3D-TI) and has been concerned with the topic of TIs in general. Two aspects were tackled to gain a deeper understanding of this new state of matter. On one hand, the expansion of the material’s basis and on the other hand developing a simple model of the structure and analysing it via density-functional theory (DFT) based methods. To discover new materials, a systematic investigation of the metal-rich parts of the bismuth–platinum-metal–iodine phase systems was conducted. It led to six new phases among the bismuth subiodides. Some of which, e.g. Bi14Rh3I9, share a honeycomb network of platinum-metal-centred bismuth-cubes and are the seed of a family of materials with this structural motive. The others show strand-like structures or layered structures with platinum-platinum bonds. The latter were so far unknown amongst bismuth subiodides. The honeycomb network was separately analysed and shown to host the TI properties. Structurally and electronically it can be seen as a “heavy graphene analogue”, which refers to the fact that graphene with hypothetical strong spin-orbit coupling (“heavy graphene”) was the first TI put forward by theoreticians. Apart from DFT-calculations, physical experiments confirmed the TI properties. Angle-resolved photoelectron spectroscopy (ARPES) was used to verify the electronic structure and scanning tunnelling microscopy and spectroscopy (STM and STS) to reveal the protected 1D edge states present at the cleaving surface of this material. As the arrangement of the honeycomb layer varies between the different known and newly discovered materials within this family of structures, this influence was also investigated. All further materials were also characterised by DFT-calculations and physical experiments, e.g. magnetisation and transport measurements. This thesis might give an experimental and theoretical basis for a deeper understanding of the TI state of matter. The 1D edge states on the surface of Bi14Rh3I9 could be a chance to handle spins and therefore propel spintronic research, or they could host Majorana fermions, which could be used as qubits in quantum computing.

For the analysis of the wet pressing process, which was presented in the first part of this paper, a theoretical approach was chosen. This enabled the pre-definition of three quality-related priorities which now will be considered in detail in the second part. For further analysis, real process data, recorded in an early phase of the process implementation, are used. The challenge is that in this process status, the availability of data is limited or the data sets are incomplete. Supported by the theoretical approach, an easier interpretation of the process data, and in case of ambiguous issues, an accelerated decision making is expected. The objective is to show that this combination is suitable for the process analysis in an early production phase.

The wet pressing process represents a new production method for carbon fibre-reinforced plastics components. Due to the low cycle times, it is suitable for use in the automotive industry. Therefore, a sufficient degree of industrialisation needs to be achieved, which is characterised by a stable process. The knowledge about relevant process parameters, their interactions, and influence on the part quality builds the basis of an economic process. This is a major challenge, since in the early stage of process development the available amount of recorded process data is small and the data sets are not complete. As the implementation of time-, material-, and cost-intensive experiments represents no acceptable alternative, a theoretical approach is chosen. This article describes a theoretical procedure to define the critical factors of the wet pressing process with significantly less resource input.

Contact mechanical study of layered structures is useful to various fields of engineering, such as - mechanical engineering, civil engineering, materials engineering and biomechanics. Thin hard film coating on a compliant substrate used in cutting tool industry is an example of a layered structure. The protective coating saves the substrate from fracture and wear. However, due to film material brittleness, fracture in the films is of concern. We have developed an analytical model for a film-substrate bilayer system under normal contact loading, which helps us to obtain the stress distribution in the film and fracture behaviour. Our contact model is based on Hankel’s Transform technique, where we assume a Hertzian pressure boundary condition. At each depth of penetration of the indenter in the film-substrate system, we estimate effective modulus of the system based on Gao’s approach. We have validated our analysis by surface strain measurements and photoelastic stress study in the film on a substrate. Experimental observations from literatures show the dependence of different fracture modes in a thin hard film with columnar structure on film thickness and substrate plasticity. We perform fracture analysis, a parametric study of the fracture modes in the film under contact loading. When the film thickness is small and the substrate is relatively hard (e.g. tool steel), the film and the substrate deform conformally under contact loading and the columns of TiN slide against each other into the substrate. On the other hand, when the film is thicker and the substrate is soft (e.g. mild steel or aluminium), the strain mismatch between the film and substrate acts as an added traction at the interface and drives cracks, such as radial tensile stress driven bending cracks that start from the interface at the center of indentation; maximum shear stress driven inclined shear crack that starts inside the film and propagate at an angle to the indentation axis and tensile stress driven edge crack that starts from the free surface outside the contact. We can draw a fracture map based on these calculations which provides a guide to select film thickness depending on the substrate hardness, so that the benign mode of damage, i.e., columnar shear occurs in the film. Apart from generating the fracture map, we can obtain rationale for different fracture phenomenon in the film by studying the indentation stress field. Principal tensile stresses, responsible for driving edge cracks from the free surface outside the contact, become compressive as one approaches the substrate if the substrate is compliant. The cracks therefore do not penetrate deep into the film rather curve away from the axis of indentation. At the transition zone from one mode of damage to other in the fracture map, different modes of fracture may co-exist. The whole column may not shear, rather the shear can start from somewhere in the middle of the film, where the shear stress is maximum and it can end without reaching the interface. The indentation energy is then dissipated in other forms of damage. The contact analysis is further applied to TiN /AlTiN multilayered films having similar elastic properties. Experimental observations suggest that with decreasing layer thickness the fracture resistance of the multilayers increase and some plastic yielding occurs at the top layers of the film. However no substantial change in strain capacity (Hardness/ Young’s Modulus) of the film is observed. Hence we attribute the increase of fracture resistance of multilayers to film plasticity and mimic it by reducing the modulus of the film. The analysis validates the propensity of edge cracking and transgranular cracking as they decrease with increasing number of layers in a multilayer. We next extend our bilayer analysis to a more general trilayer problem where the moduli of the layers vary by several orders. The test system here is a mica-glue-glass system which is used in surface force apparatus experiments. Gao’s trilayer analysis is used to fit the experimental data obtained from surface force apparatus experiments, where a glass sphere indents the trilayer. The parallel spring model used in Gao’s approximation is found to be inadequate to rationalize the experimental data. We have modified Gao’s formulations by reducing the problem to a bilayer problem where the layers are the first layer (in contact) and an equivalent layer which has properties determined by a rule of mixture of the properties of all the layers excluding the top layer set out as a set of springs in series. The modified formulations give a better fit to the experimental data and it is validated from nanoindentation experiments on the same system. The formulation is used to obtain the compression of the glue, which contributes significantly to the deformation of the trilayer system in the SFA experiments. Thus, the analysis can be used to deconvolute the influence of glue in the actual mechanical response of the system in an SFA experiment, which has so far been neglected.

This thesis was inspired by the discovery of Bi14Rh3I9, the first so-called weak three-dimensional topological insulator (3D-TI) and has been concerned with the topic of TIs in general. Two aspects were tackled to gain a deeper understanding of this new state of matter. On one hand, the expansion of the material’s basis and on the other hand developing a simple model of the structure and analysing it via density-functional theory (DFT) based methods. To discover new materials, a systematic investigation of the metal-rich parts of the bismuth–platinum-metal–iodine phase systems was conducted. It led to six new phases among the bismuth subiodides. Some of which, e.g. Bi14Rh3I9, share a honeycomb network of platinum-metal-centred bismuth-cubes and are the seed of a family of materials with this structural motive. The others show strand-like structures or layered structures with platinum-platinum bonds. The latter were so far unknown amongst bismuth subiodides. The honeycomb network was separately analysed and shown to host the TI properties. Structurally and electronically it can be seen as a “heavy graphene analogue”, which refers to the fact that graphene with hypothetical strong spin-orbit coupling (“heavy graphene”) was the first TI put forward by theoreticians. Apart from DFT-calculations, physical experiments confirmed the TI properties. Angle-resolved photoelectron spectroscopy (ARPES) was used to verify the electronic structure and scanning tunnelling microscopy and spectroscopy (STM and STS) to reveal the protected 1D edge states present at the cleaving surface of this material. As the arrangement of the honeycomb layer varies between the different known and newly discovered materials within this family of structures, this influence was also investigated. All further materials were also characterised by DFT-calculations and physical experiments, e.g. magnetisation and transport measurements. This thesis might give an experimental and theoretical basis for a deeper understanding of the TI state of matter. The 1D edge states on the surface of Bi14Rh3I9 could be a chance to handle spins and therefore propel spintronic research, or they could host Majorana fermions, which could be used as qubits in quantum computing.

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

Исследовано поглощение мощности электромагнитного поля тканями головы человека в микроволновом диапазоне. Расчет электрического поля в тканях головы, индуцированного элементарной антенной, основано на применении функций Грина слоистых сред. Два вида излучателей, таких как полуволновый диполь и петлевая антенна сравниваются с точки зрения глубины проникновения электромагнитной энергии. Рассчитана мощность, поглощаемая в различных слоях модели головы человека. В заключении сделан вывод о преимуществе применения криволинейных токов, таких, как формируемых плоской спиралью. Рассмотрено влияние проводящего экрана на эффективность излучения антенны. Полученные результаты предполагается использовать при разработке эффективных сенсоров для микроволновой радиометрии мозга. / The power absorbed by human head tissues in the microwave range is investigated. Calculation of the electric field induced in the head tissues by antenna probe is based on the use of the Green’s functions of the stratified media. Two types of emitters such as a half-wave dipole and a loop antenna are compared in terms of the depth of electromagnetic energy penetration. The power absorbed by different layers of the human head model is calculated. The conclusion is made on the best efficiency of antenna with an annular current, such as a flat helix. The effect of the conducting screen on the efficiency of the antenna is studied. The data were obtained for designing effective field sensors for the microwave radiometry of the brain.

Seafloor compliance is a non-intrusive geophysical method sensitive to the shear modulus of the sediments below the seafloor. A compliance analysis requires the computation of the frequency dependent transfer function between the vertical stress, produced at the seafloor by the ultra low frequency passive source-infra-gravity waves, and the resulting displacement, related to velocity through the frequency. The displacement of the ocean floor is dependent on the elastic structure of the sediments and the compliance function is tuned to different depths, i.e., a change in the elastic parameters at a given depth is sensed by the compliance function at a particular frequency. In a gas hydrate system, the magnitude of the stiffness is a measure of the quantity of gas hydrates present. Gas hydrates contain immense stores of greenhouse gases making them relevant to climate change science, and represent an important potential alternative source of energy. Bullseye Vent is a gas hydrate system located in an area that has been intensively studied for over 2 decades and research results suggest that this system is evolving over time. A partnership with NEPTUNE Canada allowed for the investigation of this possible evolution. This thesis describes a compliance experiment configured for NEPTUNE Canada’s seafloor observatory and its failure. It also describes the use of 203 days of simultaneously logged pressure and velocity time-series data, measured by a Scripps differential pressure gauge, and a Güralp CMG-1T broadband seismometer on NEPTUNE Canada’s seismic station, respectively, to evaluate variations in sediment stiffness near Bullseye. The evaluation resulted in a (- 4.49 x10-3± 3.52 x 10-3) % change of the transfer function of 3rd October, 2010 and represents a 2.88% decrease in the stiffness of the sediments over the period. This thesis also outlines a new algorithm for calculating the static compliance of isotropic layered sediments.

Seafloor compliance is a non-intrusive geophysical method sensitive to the shear modulus of the sediments below the seafloor. A compliance analysis requires the computation of the frequency dependent transfer function between the vertical stress, produced at the seafloor by the ultra low frequency passive source-infra-gravity waves, and the resulting displacement, related to velocity through the frequency. The displacement of the ocean floor is dependent on the elastic structure of the sediments and the compliance function is tuned to different depths, i.e., a change in the elastic parameters at a given depth is sensed by the compliance function at a particular frequency. In a gas hydrate system, the magnitude of the stiffness is a measure of the quantity of gas hydrates present. Gas hydrates contain immense stores of greenhouse gases making them relevant to climate change science, and represent an important potential alternative source of energy. Bullseye Vent is a gas hydrate system located in an area that has been intensively studied for over 2 decades and research results suggest that this system is evolving over time. A partnership with NEPTUNE Canada allowed for the investigation of this possible evolution. This thesis describes a compliance experiment configured for NEPTUNE Canada’s seafloor observatory and its failure. It also describes the use of 203 days of simultaneously logged pressure and velocity time-series data, measured by a Scripps differential pressure gauge, and a Güralp CMG-1T broadband seismometer on NEPTUNE Canada’s seismic station, respectively, to evaluate variations in sediment stiffness near Bullseye. The evaluation resulted in a (- 4.49 x10-3± 3.52 x 10-3) % change of the transfer function of 3rd October, 2010 and represents a 2.88% decrease in the stiffness of the sediments over the period. This thesis also outlines a new algorithm for calculating the static compliance of isotropic layered sediments.