Continental rifting is an important geodynamic process during which the Earth's outer-most rigid shell undergoes continuous stretching resulting in continental break-up and theformation of new oceanic basins. The East African Rift System, which has two continentalsegments comprising largely of the East African Rift (EAR) to the West and the easternmostsegment Madagascar, is the largest narrow rift on Earth. However, the driving mechanismsof continental rifting remain poorly understood due to a lack of numerical infrastructure tosimulate rifting, the lack of knowledge of the underlying mantle dynamics, and poor knowl-edge of mantle rheology. Here, we use state-of-art computational modeling of the upper660 km of the Earth to: 1) provide a better understanding of mantle flow patterns and themantle rheology beneath Madagascar, 2) to elucidate the main driving forces of observedpresent-day∼E-W opening in the EAR, and 3) to investigate the role of multiple plumesor a superplume in driving surface deformation in the EAR. In chapter 1, we simulate EdgeDriven convection (EDC), constrained by a lithospheric thickness model beneath Madagas-car. The mantle flow associated with the EDC is used to calculate induced olivine aggregates'Lattice Preferred Orientation (LPO), known as seismic anisotropy. The predicted LPO isthen used to calculate synthetic seismic anisotropy, which were compared with observationsacross the island. Through a series of comparisons, we found that asthenospheric flow result-ing from undulations in lithospheric thickness variations is the dominant source of the seismicanisotropy, but fossilized structures from an ancient shear zone may play a role in southern Madagascar. Our results suggest that the rheological conditions needed for the formationof seismic anisotropy, dislocation creep, dominates the upper asthenosphere beneath Mada-gascar and likely other continental regions. In chapter 2, we use a 3D numerical model ofthe lithosphere-asthenosphere system to simulate instantaneous lithospheric deformation inthe EAR and surroundings. We test the hypothesis that the∼E-W extension of the EAR isdriven by large scale forces arising from topography and internal density gradients, known aslithospheric buoyancy forces. We calculate surface deformation solely driven by lithosphericbuoyancy forces and compare them with surface velocity observations. The lithosphericbuoyancy forces are implemented by imposing observed topography at the model surfaceand lateral density variations in the crust and mantle down to a compensation depth of 100km. Our results indicate that the large-scale∼E-W extension across East Africa is driven bylithospheric buoyancy forces, but not along-rift surface motions in deforming zones. In chap-ter 3, we test the hypothesis that the anomalous northward rift-parallel deformation observedin the deforming zones of the EAR is driven by viscous coupling between the lithosphereand deep upwelling mantle material, known as a superplume, flowing northward. We testtwo end-member plume models including a multiple plumes model simulated using high res-olution shear wave tomography-derived thermal anomaly and a superplume model (Africansuperplume) simulated by imposing a northward mantle-wind on the multiple plumes model.Our results suggest that the horizontal tractions from northward mantle flow associated withthe African Superplume is needed to explain observations of rift-parallel surface motions indeforming zones from GNSS/GPS data and northward oriented seismic anisotropy beneaththe EAR. Overall, this work yields a better understanding of the geodynamics of Africa. / Doctor of Philosophy / Continental rifting is an important geodynamic process during which the Earth's outer-most rigid shell undergoes continuous stretching resulting in continental break-up and theformation of new oceanic basins. The East African Rift System, which has two continentalsegments comprising largely of the East African Rift (EAR) to the West and the easternmostsegment Madagascar, is the largest narrow rift on Earth. However, the driving mechanismsof continental rifting remain poorly understood due to a lack of numerical infrastructure tosimulate rifting, the lack of knowledge of the underlying mantle dynamics, and poor knowl-edge of mantle rheology. Here, we use state-of-art computational modeling of the upper660 km of the Earth to: 1) provide a better understanding of mantle flow patterns and themantle rheology beneath Madagascar, 2) to elucidate the main driving forces of observedpresent-day∼E-W opening in the EAR, and 3) to investigate the role of multiple plumesor a superplume in driving surface deformation in the EAR. In chapter 1, we simulate EdgeDriven convection (EDC), constrained by a lithospheric thickness model beneath Madagas-car. The mantle flow associated with the EDC is used to calculate induced olivine aggregates'Lattice Preferred Orientation (LPO), known as seismic anisotropy. The predicted LPO isthen used to calculate synthetic seismic anisotropy, which were compared with observationsacross the island. Through a series of comparisons, we found that asthenospheric flow result-ing from undulations in lithospheric thickness variations is the dominant source of the seismicanisotropy, but fossilized structures from an ancient shear zone may play a role in southern Madagascar. Our results suggest that the rheological conditions needed for the formationof seismic anisotropy, dislocation creep, dominates the upper asthenosphere beneath Mada-gascar and likely other continental regions. In chapter 2, we use a 3D numerical model ofthe lithosphere-asthenosphere system to simulate instantaneous lithospheric deformation inthe EAR and surroundings. We test the hypothesis that the∼E-W extension of the EAR isdriven by large scale forces arising from topography and internal density gradients, known aslithospheric buoyancy forces. We calculate surface deformation solely driven by lithosphericbuoyancy forces and compare them with surface velocity observations. The lithosphericbuoyancy forces are implemented by imposing observed topography at the model surfaceand lateral density variations in the crust and mantle down to a compensation depth of 100km. Our results indicate that the large-scale∼E-W extension across East Africa is driven bylithospheric buoyancy forces, but not along-rift surface motions in deforming zones. In chap-ter 3, we test the hypothesis that the anomalous northward rift-parallel deformation observedin the deforming zones of the EAR is driven by viscous coupling between the lithosphereand deep upwelling mantle material, known as a superplume, flowing northward. We testtwo end-member plume models including a multiple plumes model simulated using high res-olution shear wave tomography-derived thermal anomaly and a superplume model (Africansuperplume) simulated by imposing a northward mantle-wind on the multiple plumes model.Our results suggest that the horizontal tractions from northward mantle flow associated withthe African Superplume is needed to explain observations of rift-parallel surface motions indeforming zones from GNSS/GPS data and northward oriented seismic anisotropy beneaththe EAR. Overall, this work yields a better understanding of the geodynamics of Africa.

<p dir="ltr"><i>The high heat fluxes generated in electronic devices must be effectively diffused through </i><i>the semiconductor substrate and packaging layers to avoid local, high-temperature “hotspots” </i><i>that govern long-term device reliability. In particular, advanced semiconductor packaging </i><i>trends toward thin form factor products increase the need for understanding and improving </i><i>in-plane conduction heat spreading in anisotropic materials. Furthermore, predicting thermal </i><i>transport in vertical stacks of thinned and bonded die hinges on accurately characterizing </i><i>unknown buried interfacial thermal resistances. The design of semiconductor thermal packaging </i><i>solutions is hence limited by the functionality and accuracy of metrology available </i><i>for thermal properties characterization of engineered anisotropic heat spreading materials </i><i>and buried interfaces. This work focuses on the development of two separate innovative </i><i>metrology techniques for characterizing in-plane thermal properties of both isotropic and </i><i>anisotropic materials, and the measurement of low thermal interfacial resistances embedded </i><i>in stacks of semiconductor substrates.</i></p><p dir="ltr"><i>In the first portion of this thesis, a new measurement technique is developed for characterizing </i><i>the isotropic and anisotropic in-plane thermal properties of thin films and sheets, </i><i>as an extension of the traditional Ångstrom method and other lock-in thermography techniques. </i><i>The measurement leverages non-contact infrared temperature mapping to quantify </i><i>the thermal response to laser-based periodic heating at the center of a suspended thin film </i><i>sample. This novel data extraction method does not require precise knowledge of the boundary </i><i>conditions. To validate the accuracy of this technique, numerical models are developed </i><i>to generate transient temperature profiles for hypothetical anisotropic materials with known </i><i>properties. The resultant temperature profiles are processed through a fitting algorithm to </i><i>extract the in-plane thermal conductivities, without the knowledge of the input properties </i><i>to the forward model. Across a wide range of in-plane thermal conductivities, these results </i><i>agree well with the input values. The limits of accuracy of this technique are identified based </i><i>on the experimental and sample parameters. Further, numerical simulations demonstrate </i><i>the accuracy of this technique for materials with thermal conductivities from 0.1 to 1000 W </i><i>m</i><i>−1 </i><i>K</i><i>−1</i><i>, and material thicknesses ranging from 0.1 to 10 mm. This technique effectively</i> <i>measures anisotropy ratios up to 1000:1. Data from multiple heating frequencies can be </i><i>combined to fit for a single set of thermal properties (independent of frequency), which improves </i><i>measurement sensitivity as the thermal penetration depth varies across frequencies. </i><i>The post-processing algorithm filters out regions within the laser absorber and heat sink to </i><i>eliminate regions in the sample domain with boundary effects. Based on these guidelines, </i><i>experiments demonstrate the accuracy of this measurement technique for a wide range of </i><i>known isotropic and anisotropic heat spreading materials across a thermal conductivity range </i><i>of 0.3 to 700 W m</i><i>−1 </i><i>K</i><i>−1</i><i>, and in-plane anisotropy ratios of 30:1. These steps contribute </i><i>towards standardization of this measurement technique, enabling the development and characterization </i><i>of engineered heat spreading materials with desired anisotropic properties for </i><i>various applications.</i></p><p dir="ltr"><i>The second portion of this thesis focuses on characterization of thermal resistances across </i><i>“buried” interfaces that are challenging to characterize in situ due to their low relative magnitude </i><i>and embedded depth within a material stack. In particular, we target characterization </i><i>of interfaces that are buried deeper than the thermal penetration depth of available transient </i><i>measurement techniques, such as thermoreflectance, but have low thermal resistances </i><i>that prohibit the use of steady-state techniques, such as the reference bar method, due to </i><i>the very high temperature gradients that would be necessary resolve the resistances, among </i><i>other sample preparation challenges. This work develops a technique for the non-destructive </i><i>characterization of such deeply buried interfaces having thermal contact resistances of the </i><i>order of 0.001 cm</i><i>2</i><i>K/W. Two different embodiments of the measurement approach are first </i><i>assessed before down-selecting to a single experimental implementation. The working principle </i><i>for both embodiments includes a combination of non-contact periodic heating and </i><i>thermal sensing to measure the transient temperature response of a two-layer stack of materials </i><i>with a bonded interface of unknown thermal resistance. The approaches aim to </i><i>eliminate the preparation requirement of cutting samples to investigate their temperature in </i><i>cross-section. In the first embodiment, the sample stack is heated periodically at the center </i><i>of the sample, and cooled at the periphery, to create a radial temperature gradient. The </i><i>second embodiment involves generating a one-dimensional temperature gradient across the </i><i>stack by periodic heating of one face and steady cooling of the other face. The corresponding </i><i>ing amplitude and phase delay of the temperature responses are used to fit for the thermal </i><i>interfacial resistance, assuming a time-periodic solution for the heat diffusion equation for </i><i>a system with periodic heating. Numerical models developed for both approaches simulate </i><i>the transient temperature profiles across a two-layer bonded silicon stack of known thermal </i><i>properties, and enable an assessment of both approaches. The one-dimensional (1D) gradient </i><i>approach is found to have higher sensitivity and measurable signal compared to the </i><i>radial spreading approach, at the same mean temperature of the sample. </i></p><p dir="ltr"><i>Based on this 1D gradient concept, an experimental facility is developed, which includes </i><i>a IR-transparent heat sink, laser-based heating, and two IR temperature sensors for noncontact </i><i>temperature measurement of both sides of the sample. The unique IR transparent </i><i>heat sink design allows for simultaneous cooling and non-contact temperature measurement </i><i>of the bottom surface of the sample. An inverse fitting method is developed to extract </i><i>the thermal resistances using the steady periodic temperature amplitude and phase delay </i><i>across the thickness of the material. Thermal data generated using numerical simulations, </i><i>along with the data fitting method, is first leveraged to validate the extracted thermal resistance </i><i>values for two-layer material systems with an bonded interface, as well as for the </i><i>thermal conductivity measurement of bulk materials without an interface. The data extraction </i><i>process is shown to accurately extract thermal contact resistances on the order of </i><i>0.0001 cm</i><i>2</i><i>K/W in silicon-based packages for interfaces that are a few millimeters from the </i><i>exposed surface. For bulk materials, this technique demonstrates accuracy in extracting </i><i>the thermal conductivity of a wide range of materials ranging from thermal insulators to </i><i>highly conductive materials, spanning a range of 0.1 to 2000 W m</i><i>−1 </i><i>K</i><i>−1</i><i>. Physical measurements </i><i>of thermal conductivity of bulk silicon nitride and zinc oxide agree well with expected </i><i>reference values, and these measurements also align well with data from independently performed </i><i>experiments on the same materials using an established ASTM D5470 standard, </i><i>thereby validating this new measurement technique experimentally. Two-layer dry-contact </i><i>stacks of these two materials demonstrate the extraction of the thermal resistance across </i><i>interfaces buried up to 2 mm from the exposed surface. This work contributes toward standardization </i><i>of this technique for measurement of thermal resistances with low magnitudes </i><i>and buried depths, which are commonly found in modern electronic packages, ranging from </i><i>near-junction epitaxial semiconductor films to interconnect layers in emerging die-to-die and </i><i>wafer hybrid bonding technologies.</i></p><p dir="ltr"><i>Ultimately, these measurement techniques of in-plane thermal conductivity measurement </i><i>of anisotropic materials and the interfacial contact resistance measurements across buried </i><i>interfaces offer an important contribution to the area of thermal metrology, and advance the </i><i>field of next-generation semiconductor packaging.</i></p>

Diese Arbeit befasst sich mit den optischen Eigenschaften von dünnen GaN-Schichten gewachsen in verschiedenen Orientierungen. Hierbei werden die optischen Eigenschaften von verspannten M- und A-plane sowie unverspannten C-plane GaN-Schichten untersucht und die Ergebnisse im Rahmen von Bandstrukturberechnungen diskutiert. Im Rahmen dieser Arbeit werden die Bandstrukturverschiebungen theoretisch mittels eines k.p-Näherungsansatzes untersucht. Diese Bandverschiebungen beeinflussen sowohl die Übergangsenergien als auch die Oszillatorstärken. Man findet, dass die C-plane Schicht im Falle einer isotropen Verspannung in der Filmebene keine Anisotropie der optischen Polarisation zeigt. In beiden Fällen zeigen die drei Übergänge von den drei oberen Valenzbändern in das untere Leitungsband andere Polarisationseigenschaften als die entsprechenden Übergänge in C-plane GaN-Schichten. Es wird beobachtet, dass für einen bestimmten Wertebereich der Verspannung in der Filmebene diese Übergänge nahezu vollständig x-,z- bzw. y-artig polarisiert sind. Die verwendeten Schichten wurden auch mittels Transmissionspektroskopie untersucht. Im Falle der M-plane GaN-Schichten können zwei fundamentale Übergänge identifiziert werden, wobei der elektrische Feldvektor E des einfallenden Lichtes einmal parallel (z-Polarisation) und einmal senkrecht (x-Polarisation) auf der c-Achse steht. Die M-plane GaN-Schicht besitzt unterschiedliche Dielektrizitätskonstanten für z-Polarisation und x-Polarisation, welche zu zusätzlichem Dichroismus und Doppelbrechung führen. Als Resultat findet eine Filterung der Polarisation für einfallendes, linear polarisiertes Licht statt. Die elektrische Feldkomponente mit x-Polarisation wird stärker absorbiert als die Komponente mit z-Polarisation. Diese Polarisationsfilterung äußert sich für schmalbandiges Licht in Form einer Drehung der Polarisationsebene in Richtung der c-Achse, wobei ein maximaler Rotationswinkel von 40 Grad gefunden wurde. / In this work, we focus on the optical response of GaN thin films grown along various orientations. The optical properties of strained M- and A- and unstrained C-plane GaN thin films are investigated, and the results are explained with help of band-structure calculations. We calculate the strain-induced band-structure modification using the k.p perturbation approach. The valence-band (VB) states are modified affecting both the transition energies as well as the oscillator strengths. We observe that C-plane GaN does not show any in-plane polarization anisotropy, when an isotropic in-plane strain is applied. For the case of M- and A-plane GaN, one expects to see an in-plane polarization anisotropy even for the unstrained case. Additionally, the in-plane strain significantly changes the band structure and the symmetry of the VB states. The three transitions, involving electrons in the conduction band (CB) and holes in the top three VBs, will exhibit a very different polarization characteristic than the ones for C-plane GaN. These transitions are predominantly x, z, and y polarized, respectively, for a certain range of in-plane strain values, present in our samples. For M-plane GaN thin films, two fundamental transitions can be identified, which occur when the electric field vector E is perpendicular (x-polarization) and parallel c (z-polarization). These transitions give rise to a transmittance spectrum separated by 50 meV at room temperature with respect to each other. This result in a polarization filtering of an incident linearly polarized light beam after transmission, because the electric field component with x-polarization is more strongly absorbed than with z-polarization. This filtering manifests as a rotation of the polarization vector toward the c axis and can be as large as 40 degrees for an initial angle of 60 degrees, for our samples.

Knochen und Muskel sind die wichtigsten Gewebe im muskuloskelettalen System welche dem Körper die Bewegungen möglich machen. Beide Gewebetypen sind hochgradig strukturierter Extrazellulärmatrix zugrundegelegt, welche die mechanischen und biologischen Funktionen bestimmen. In dieser Studie wurden die räumliche Verteilung der anisotropen elastischen Eigenschaften und der Gewebemineralisation im humanen kortikalen Femur untersucht mit akustischer Mikroskopie und Synchrotron-µCT. Die homogenisierten elastischen Eigenschaften wurden aus einer Kombination der Porosität und der Gewebeelastizitätsmatrix mit Hilfe eines asymptotischen Homogenisierungsmodells ermittelt. Der Einfluss der Gewebemineralisierung und der Strukturparameter auf die mikroskopischen und mesoskopischen elastischen Koeffizienten wurde unter Berücksichtigung der anatomischen Position des Femurschaftes untersucht. Es wurde ein Modell entwickelt, mit welchem der intramuskuläre Fettgehalt des porcinen musculus longissimus nichtinvasiv mittels quantitativem Ultraschall und dessen spektraler Analyze des Echosignals bestimmt werden kann. Muskelspezifische Parameter wie Dämpfung, spectral slope, midband fit, apparent integrated backscatter und cepstrale Paramter wurden aus den RF-Signalen extrahiert. Die Einflüsse der Muskelkomposition und Strukturparameter auf die spektralen Ultraschallparameter wurden untersucht. Die akustischer Parameter werden durch die Muskelfaserorientierung beeinflusst und weisen höhere Werte parallel zur Faserlängsrichtung als senkrecht zur Faserorientierung auf. Die in dieser Studie gewonnenen detaillierten und lokal bestimmten Knochendaten können möglicherweise als Eingabeparameter für numerische 3D FE-Simulationen. Darüber hinaus kann die Untersuchung von Veränderungen der lokalen Gewebeanisotropie neue Einsichten in Studien über Knochenumbildung geben. Diese auf Gewebeebene bestimmten Daten von Muskelgewebe können in numerischen Simulationen von akustischer Rückstreuung genutzt werden um diagnostische Methoden und Geräte zu verbessern. / Bone and muscle are the most important tissues in the musculoskeletal system that gives the ability to move the body. Both tissues have the highly oriented underlying extracellular matrix structure for performing mechanical and biological functions. In this study, the spatial distribution of anisotropic elastic properties and tissue mineralization within a human femoral cortical bone shaft were investigated using scanning acoustic microscopy and synchrotron radiation µCT. The homogenized meoscopic elastic properties were determined by a combination of porosity and tissue elastic matrix using a asymptotic homogenization model. The impact on tissue mineralization and structural parameters of the microscopic and mesocopic elastic coefficients was analyzed with respect to the anatomical location of the femoral shaft. A model was developed to estimate intramuscular fat of porcine musculus longissimus non-invasively using a quantitative ultrasonic device by spectral analysis of ultrasonic echo signals. Muscle specific acoustic parameters, i.e. attenuation, spectral slope, midband fit, apparent integrated backscatter, and cepstral parameters were extracted from the measured RF echoes. The impact of muscle composition and structural properties on ultrasonic spectral parameters was analyzed. The ultrasound propagating parameters were affected by the muscle fiber orientation. The most dominant direction dependency was found for the attenuation. The detailed locally assessed bone data in this study may serve as a real-life input for numerical 3D FE simulation models. Moreover, the assessment of changes of local tissue anisotropy may provide new insights into the bone remodelling studies. The data provided at tissue level and investigated ultrasound backscattering from muscle tissue, can be used in numerical simulation FE models for acoustical backscattering from muscle for the further improvement of diagnostic methods and equipment.

Die Magnetresonanzelastographie (MRE) stellt ein nichtinvasives Verfahren dar, welches die Bestimmung der in vivo Scherelastizität weicher Gewebe ermöglicht. Im Rahmen diese Arbeit wurden Methoden zur Bestimmung isotroper und anisotroper Scherelastizitäten anhand von MRE Wellenbildern entwickelt und evaluiert. Alle in dieser Arbeit vorgestellten Methoden basieren auf planarer MRE, d.h. auf der Aufnahme einer einzelnen Auslenkungskomponente innerhalb der Bildschicht. Dadurch wird die MRE erheblich beschleunigt. Allerdings stellen sich dadurch auch besondere Anforderungen an die Datenauswertung zur Bestimmung aussagekräftiger elastischer Kenngrößen. Anhand von planaren MRE-Experimenten an Gewebephantomen und menschlicher Skelettmuskulatur sowie mittels numerischer Simulation wird gezeigt, dass bei Beachtung weniger experimenteller Randbedingungen und einer darauf abgestimmten Datenauswertung, korrekte Elastizitäten ermittelt werden können. Ein besonderer Schwerpunkt der Arbeit liegt in der Analyse experimenteller Einflüsse wie Bildrauschen und -auflösung auf die ermittelten elastischen Kenngrößen. Des Weiteren werden Methoden zur Bestimmung anisotroper Elastizitäten sowie zur Analyse von Streueffekten im MRE-Wellenbild vorgestellt. Die behandelten Einflüsse auf die Amplituden und Wellenlängen im MRE-Bild, werden vergleichend diskutiert und zusammengefasst, um ein einfaches Verfahrensprotokoll zur Analyse experimenteller in vivo MRE-Daten zu entwickeln. Alle in dieser Arbeit verwendeten Methoden und Programme sind im Anhang zusammengefasst und auf Anforderung erhältlich. / Magnetic resonance elastography (MRE) is a noninvasive method that allows the determination of in vivo shear elasticity of soft tissues. In this thesis methods for the determination of isotropic and anisotropic shear elasticities from MRE wave data were developed and evaluated. All methods presented in this work are based on planar MRE, i.e. they are based on the measurement of a single displacement component in the image plane. This way measurement time in MRE is greatly reduced. However, this imposes specific requirements on data evaluation in order to determine significant elastic constants. On the basis of planar MRE experiments on tissue mimicking gels, human skeletal muscle and numerical simulations it is demonstrated that correct shear elasticities can be determined, taking into account a small set of experimental boundary conditions as well as the employment of complementary data evaluation strategies. This thesis is particularly focussed on the analysis of noise and image resolution on the determined elastic constants. Moreover, methods for determining anisotropic elasticity and analyzing shear wave scattering effects on MRE wave data are introduced. The investigated influences on wave amplitudes and wave lengths are compared and discussed to develop a simple measurement protocol for the evaluation of in vivo MRE data. All methods employed in this work are summarized in the appendix along with the corresponding computer code, which is available on demand.

Over the last two decades, great progress has been made in the understanding of multiferroic materials, ones where multiple long-range orders simultaneously exist. However, much of the research has focused on bulk systems. If these materials are to be incorporated into devices, they would not be in bulk form, but would be miniaturized, such as in nanoparticle form. Accordingly, a better understanding of multiferroic nanoparticles is necessary. This manuscript examines the multiferroic phase diagram of multiferroic nanoparticles related to system size and surface-induced magnetic anisotropy. There is a particular focus on bismuth ferrite, the room-temperature antiferromagnetic-ferroelectric multiferroic. Theoretical results will be presented which show that at certain sizes, a bistability develops in the cycloidal wavevector. This implies bistability in the ferroelectric and magnetic moments of the nanoparticles. This novel magnetoelectric bistability may be of use in the creation of an electrically-written, magnetically-read memory element. / Graduate

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Spin-torque transfer (STT) effects have brought spintronics ever closer to practical electronic applications, such as MRAM and active broadband microwave spin-torque oscillator (STO), and have emerged as an increasingly attractive field of research in spin dynamics. Utilizing materials with perpendicular magnetic anisotropy (PMA) in such applications offers several great advantages such as low-current, low-field operation combined with high thermal stability. The exchange coupling that a PMA thin film exerts on an adjacent in-plane magnetic anisotropy (IMA) layer can tilt the IMA magnetization direction out of plane, thus creating a stack with an effective tilted magnetic anisotropy. The tilt angle can be engineered via both intrinsic material parameters, such as the PMA and the saturation magnetization, and extrinsic parameters, such as the layer thicknesses.       STOs can be fabricated in one of a number of forms—as a nanocontact opening on a mesa from a deposited pseudospin-valve (PSV) structure, or as a nanopillar etching from magnetic tunneling junction (MTJ)—composed of highly reproducible PMA or predetermined tilted magnetic anisotropy layers.       All-perpendicular CoFeB MTJ STOs showed high-frequency microwave generation with extremely high current tunability, all achieved at low applied biases. Spin-torque ferromagnetic resonance (ST-FMR) measurements and analysis revealed the bias dependence of spin-torque components, thus promise great potential for direct gate-voltage controlled STOs.       In all-perpendicular PSV STOs, magnetic droplets were observed underneath the nanocontact area at a low drive current and low applied field. Furthermore, preliminary results for microwave auto-oscillation and droplet solitons were obtained from tilted-polarizer PSV STOs. These are promising and would be worth investigating in further studies of STT driven spin dynamics. / Effekter av spinnvridmoment (STT) har fört spinntroniken allt närmare praktiska elektroniska tillämpningar, såsom MRAM och den spinntroniska mikrovågsoscillatorn (STO), och har blivit ett allt mer attraktivt forskningsområde inom spinndynamik. Användning av material med vinkelrät magnetisk anisotropi (PMA) i sådana tillämpningar erbjuder flera stora fördelar, såsom låg strömförbrukning och funktion vid låga fält i kombination med hög termisk stabilitet. Den utbyteskoppling (”exchange bias”) en PMA-tunnfilm utövar på ett intilliggande skikt med magnetisk anisotropi i planet (IMA) kan få IMA-magnetiseringsriktningen att vridas ut ur planet, vilket ger en materialstack med en effektivt sett lutande magnetisk anisotropi. Lutningsvinkeln kan manipuleras med både inre materialparametrar, såsom PMA och mättningsmagnetisering, och yttre parametrar, såsom skikttjocklekarna. STO:er kan tillverkas som flera olika typer - som en nanokontaktsöppning på en s.k. mesa av en deponerad pseudospinnventilstruktur (PSV) eller som en nanotråd etsad ur en magnetisk tunnlingsövergång (MTJ) –och bestå av mycket reproducerbar PMA eller av skikt med på förhand bestämt lutning av dess magnetiska anisotropi. MTJ-STO:er av CoFeB med helt vinkelrät anisotropi visar högfrekvent mikrovågsgenerering med extremt stort frekvensomfång hos strömstyrningen, detta vid låg biasering. Mätning och analys av spinnvridmoments-ferromagnetisk resonans (ST-FMR) avslöjade ett biasberoende hos spinnvridmomentskomponenter, vilket indikerar en stor potential för direkt gate-spänningsstyrda STO:er. I helt vinkelräta PSV-STO:er observerades magnetiska droppar under nanokontaktområdet vid låg drivström och lågt pålagt fält. Dessutom erhölls preliminära resultat av mikrovågssjälvsvängning och av s.k. ”droplet solitons” hos PSV-STO:er med lutande polarisator. Dessa är lovande och skulle vara värda att undersökas i ytterligare studier av STT-driven spinndynamik. / <p>QC 20160829</p>

Les bactériocines de classe IIa présentent une activité antimicrobienne résultant d'un mécanisme d'action ciblant les membranes des bactéries à Gram positif. Cette activité est modulée par différentes caractéristiques des surfaces bactériennes. Les propriétés physico-chimiques de surface de dix-huit souches bactériennes ont été déterminées afin d'étudier le lien entre ces propriétés et les phénotypes de résistance/sensibilité à Cbn BM1. Les résultats obtenus indiquent une grande diversité des propriétés physico-chimiques des surfaces analysées, sans cependant permettre d’établir un lien entre celles-ci et le phénotype de sensibilité/résistance à CbnBM1. Les mécanismes d'action de Cbn BM1 ont ensuite été étudiés sur Carnobacterium maltaromaticum DSM20730 et Listeria monocytogenes EGDe. L'atteinte de l'intégrité physique des membranes plasmiques par l'action de Cbn BM1 montre une hétérogénéité de réponse des populations bactériennes. Ce résultat a été confirmé par microscopie de force atomique in vivo à haute résolution. L'interaction de Cbn BM1 avec les membranes a été mise en évidence par mesure de l'anisotropie de fluorescence. Cette approche a révélé que Cbn BM1 présente des degrés de pénétration différents dans la membrane de C. maltaromaticum DSM20730 par rapport à L. monocytogenes EGDe. L'action de Cbn BM1 conduit cependant, pour les deux souches, à la modification de la force protomotrice membranaire. Ces différentes approches retenues pour l'étude des mécanismes d'action ont révélé que C. maltaromaticum DSM20730 et L. monocytogenes EGDe présentent une sensibilité à Cbn BM1 uniquement lorsque les cellules sont en phase exponentielle de croissance. / The antimicrobial activity of class IIa bacteriocins toward Gram positive bacteria relies on their membrane targeting mechanisms of action. These mechanisms are modulated by the bacterial surface properties. The physico-chemical surface properties of eighteen bacterial strains were determined to link these properties to the resistance/sensitivity to Cbn BM1 of the bacterial strains. In this way, two approaches were undertaken : the microbial adhesion to solvents and electrophoretic mobility measurements. The results show a large diversity of the determined properties among the strains but without establishing a direct link between the surface properties and the resistance/sensitivity phenotypes. Mechanisms of action of the bacteriocin Cbn BM1 on Carnobacterium maltaromaticum DSM20730 and Listeria monocytogenes EGDe were determined. Syto9® and propidium iodide allowed to show the heterogeneity of the bacterial populations toward the alteration of the membrane integrity. The interaction of Cbn BM1 with the bacterial membrane was studied by monitoring the fluorescence anisotropy of DPH and TMA-DPH. The results highlight a difference between the mechanism of action of Cbn BM1 on C. maltaromaticum DSM20730 and on L. monocytogenes EGDe. However, a treatment by Cbn BM1 leads to a perturbation of the component of the proton-motive force of the membrane for both strains. These approaches revealed that these bacterial strains exhibit a sensitivity to Cbn BM1 only when treated in log growth phase. Modification of nano-mechanical properties of C. maltaromaticum DSM20730 after a treatment by Cbn BM1 were assessed by an atomic force microscopy approach.

The work presented in this thesis has two parts. The first part deals with methodological developments in the area of solid-state NMR, relevant to the study of partially ordered systems. Liquid crystals are best examples of such partially ordered systems and they are easily oriented by the magnetic field used for the NMR study. They provide spectra rich in information useful for the study of structure and dynamic s of the oriented molecule. Dipolar couplings and anisotropic chemical shifts are relatively easy to obtain for these systems. However, the methodologies used for extracting the required information are constantly undergoing change, with newer ideas being used for optimal use of the technique and increasing the sensitivity of the methodology. In this thesis, existing methods used for obtaining dipolar couplings from oriented liquid crystalline samples are examined in detail and conditions for optimal use of the methods are investigated. Different approaches for enhancing the sensitivity of the techniques are also proposed. Estimation of chemical shift anisotropy of carbons for a molecule that is used as a building block for several mesogens has been obtained and its utility for estimating the order parameters of the system have been examined. The second part of the thesis deals with the application of solid state NMR methods to the study of a number of novel liquid crystalline systems and for the estimation of dynamics, order and orientation of the mesogenic molecules in the magnetic field. Chapter-2 deals with a detailed and systematic study to improve the sensitivity of cross-polarization based separated local field (SLF) NMR spectroscopy techniques such as PISEMA(Polarization Inversion Spin Exchange at the Magic Angle) and PDLF(Pro-ton Detected Local Field). The chapter has been further divided into three sections. Section-A describes the optimization procedure for cross-polarization period for reducing zero-frequency peaks in SLF experiments. Polarization Inversion(PI) is one of the important components of PISEMA and plays a crucial role in enhancing the dipolar cross-peaks and suppressing the axial-peaks. Shortening this period has the advantage of less r.f. power input into the system, thus less susceptibility to sample heating. Therefore it is crucial to arrive at the optimum condition for which maximum sensitivity and resolution are obtained. A detailed experimental investigation of the role of the initial po1arization period has been carried out for two different samples of static oriented liquid crystalline material at two different temperatures and a contact time of 2ms has been found to be optimal for such samples. Insection-B of this chapter, the initial preparation period of the experiment is considered as a possible means of increasing the sensitivity of the experiment. Thus the use of cross-polarization via the dipolar bath by the use of a diabatic demagnetization in the rotating frame(ADRF-CP) has been proposed to be incorporated into PISEMA. To understand the CP dynamics, magnetization in double-and zero-quantum reservoirs of an ensemble of spin-1/2 nuclei and their role in determining the sensitivity the experiments have been theoretically examined. Experimentally, a modification incorporating ADRF-CP is shown to result in enhancement of signal-to-noise by as much as 90% in the case of rigid single crystals of a model peptide and up to 50% in non-rigid, partially ordered liquid crystalline systems. In section-C another useful SLF technique known as PDLF spectroscopy has also been examined. In this case a sweep of one of the r.f. amplitudes(RAMP-CP),rather than ADRF is found to work well. The reason for the different behaviours has been discussed. Chapter-3 highlights two experimental approaches used to extract the chemical shift anisotropy(CSA) tensor information from rotating solids. Section-A is devoted to the measurement of the CSA values of thiophene by using MAS side band analysis, by extracting the principal values from the intensities of just a few spinning side bands. Experiments have been performed on thiophene-2 carboxylic acid and thiophene-3 carboxylic acid samples and the carbon CSA values have been obtained. In section-B, CSA values of carbons of the core unit of the liquid crystal4- hexyloxybenzoic acid (HBA) have been obtained by using the recoupling pulse sequence SUPER(Separation of Undistorted Powder patterns by Effortless Recoupling).HBA belongs to an important class of thermotropic liquid crystals which are structurally simple and often used as starting materials for many novel mesogens. As this molecule could serve as an ideal model compound, high resolution13C NMR studies of HBA in solution, solid and liquid crystalline phases have been also undertaken. The CSA values obtained from the 2D SUPER experiment showed good agreement to those computed by DFT calculations. The CSA values were used for obtaining the order parameter of the system at different temperatures. These matched well the order parameter obtained from the 13C-1 H dipolar couplings in the nematic phase determined by SLF spectroscopy at various temperatures. A knowledge of the CSA of the carbons is thus very useful, as they can be used for gaining knowledge about the system from the chemical shifts obtained from a simple 1D spectrum. In chapter-4, 1-and 2-dimensional13CNMR techniques have been utilized to obtain extensive information about some novel mesogenic molecules. Four molecules of different structure and topology have been taken up for study. These molecules have the following features. Mesogen-1 has a terminal hydroxyl group. Such systems with further modification can result in mesogenic monomers for side chain liquid crystalline polymers. Mesogen-2 has a dimethyl amino group at one end and has three phenyl groups connected by appropriate linking units that form the core. In the third case, mesogen-3, the terminal hydroxyl group of mesogen-1 is replaced with a hydrogen such that13C-1 H dipolar couplings provide directly information on molecular ordering and orientation. In the fourth case, mesogen-4, the core is built with four phenyl rings. Here the fourth ring is linked to other three rings via a flexible chain unit. In each of these cases the 2DSLFNMR experiments have been carried out where13C-1 H dipolar couplings as well as13C chemical shifts were used for obtaining the order parameters of various segments of the molecule. The data provide useful insight into the phase behaviour, ordering and orientation of the molecules. Chapter-5 discusses the applications of the natural abundance 13CNMR techniques to thiophene based mesogens, that have the potential for use in molecular electronics material. Typically, these molecules consist of phenyl rings appropriately connected by linking units with thiophene. Different core units as well as different linking units to thiophene have been considered. The six mesogens thus obtained have been investigated in detail using 1D and 2D NMR methods.13C-1 H dipolar couplings have been used to obtain ordering information, that show interesting correlation to the molecular orientation and dynamics.