A thorough understanding of pharmaceutical and therapeutic products and materials is important for an improved quality of life. By probing the complex behaviors and properties of these systems, new insights can allow for a better understanding of current treatments, improved design and synthesis of new drug products, and the development of new treatments for various health conditions. Often, the impact of these new insights are limited by current technology and instrumentation and by the methods in which existing data is processed. Additionally, current standards for characterization of pharmaceuticals and therapeutics are time-consuming and can delay the timeline in which these products become available to the consumer. By addressing the limitations in current instrumentation and data science methods, faster and improved characterization is possible.<div><br></div><div>Development and improvement in optical instrumentation provides potential solutions to the current limitations of characterization methods by conventional instrumentation. Limitations in speed can be addressed through the use of nonlinear optical (NLO) methods, such as second harmonic generation (SHG) and two-photon excited ultraviolet fluorescence (TPE-UVF) microscopy, or by linear methods such as fluorescence recovery after photobleaching (FRAP). For these methods, a high signal-to-noise ratio (SNR) and a nondestructive nature decrease the overall sample size requirements and collections times of these methods. Furthermore, by combination of these optical techniques with other techniques, such as thermal analysis (e.g. differential scanning calorimetry (DSC)), polarization modulation, or patterned illumination, the collection of more complex and higher quality data is possible while retaining the improved speed of these methods. Thus, this modified instrumentation can allow for improved characterization of properties such as stability, structure, and mobility of pharmaceutical and therapeutic products.<br></div><div><br></div><div>With an increase in data quantity and complexity, improvements to existing methods of analysis, as well as development of new data science methods, is essential. Machine learning (ML) architectures and empirically validated models for the analysis of existing data can provide improved quantification. Using the aforementioned optical instrumentation, auto-calibration of data acquired by SHG microscopy is one such method in which quantification of sample crystallinity is enabled by these ML and empirical models. Additionally, ML approaches utilizing generative adversarial networks (GANs) are able to improve on identification of data tampering in order to retain data security. By use of GANs to tamper with experimentally collected and/or simulated data used in existing spectral classifiers, knowledge of adversarial methods and weakness in spectral classification can be ascertained. Likewise, perturbations in physical illumination can be used to ascertain information on classification of real objects by use of GANs. Use of this knowledge can then be used to prevent further data tampering or by improving identification of data tampering.<br></div>

Particle dispersions provide a promising tool for the engineering of functional materials that exploit self-assembly of complex structures. Dispersion made from magnetic colloidal particles is a great choice; they are biocompatible and remotely controllable among many other advantages. However, their dominating dipolar interaction typically limits structural complexity to linear arrangements. This paper shows how a magnetostatic equilibrium state with noncollinear arrangement of the magnetic moments, as reported for ferromagnetic Janus particles, enables the controlled self-organization of diverse structures in two dimensions via constant and low-frequency external magnetic fields. Branched clusters of staggered chains, compact clusters, linear chains, and dispersed single particles can be formed and interconverted reversibly in a controlled way. The structural diversity is a consequence of both the inhomogeneity and the spatial extension of the magnetization distribution inside the particles. We draw this conclusion from calculations based on a model of spheres with multiple shifted dipoles. The results demonstrate that fundamentally new possibilities for responsive magnetic materials can arise from interactions between particles with a spatially extended, anisotropic magnetization distribution.

Ce travail de thèse est dédié à la visualisation par microscopie optique des transitions de phases, thermo- et photo-induites dans des monocristaux à transition de spin. L’étude des cristaux du composé [{Fe(NCSe)(py)2}2(m-bpypz)] a permis de montrer la possibilité de contrôler la dynamique de l’interface HS/BS (haut spin/bas spin) par une irradiation lumineuse appliquée sur toute la surface du cristal ou de manière localisée. Les investigations expérimentales menées sur l’effet de l’intensité de la lumière sur la température de transition ont mis en évidence d’une part l’importance du couplage entre le cristal et le bain thermique, et d’autre part le rôle de la diffusion de la chaleur dans le monocristal. En parallèle, un modèle basé sur une description de type Ginzburg-Landau, a permis de mettre sur pied une description de type réaction diffusion des effets spatio-temporels accompagnant la transition de spin dans un monocristal. Celui-ci a permis d’identifier et de comprendre le rôle des paramètres pertinents entrant en jeu dans le contrôle du mouvement de l’interface HS/BS. Les résultats obtenus sont très encourageants et reproduisent avec une grande fidélité les données expérimentales. Cependant l’origine de l’orientation de l’interface HS/BS observée par microscopie optique dans les cristaux du composé [{Fe(NCSe)(py)2}2(m-bpypz)] était restée mystérieuse. Pour résoudre cette question, nous avons développé un modèle électro-élastique qui tient compte du changement de volume au cours de la transition de spin. Ce dernier nous a conduits à analyser l’effet de la symétrie du réseau cristallin et de la forme du cristal sur l’orientation de l’interface élastique. En l’appliquant au composé [{Fe(NCSe)(py)2}2(m-bpypz)], en tenant compte du caractère anisotrope du changement de la maille élémentaire lors du passage HSBS, nous avons réussi à retrouver quantitativement l’orientation du front observée expérimentalement en microscopie optique. Ceci confirme bien le rôle primordial de l’élasticité dans le comportement des matériaux à transition de spin. Des études sous lumière à très basse température nous ont donné la possibilité de suivre en temps réel, l’effet LIESST (Light Induced Excited Spin State Trapping), la re-laxation coopérative du cristal ainsi que l’instabilité photo-induite LITH (Light Induced Thermal Hysteresis). Un monde fascinant est apparu autour de cette dernière, avec la présence de comportements totalement inédits. Ainsi, et pour la première fois, nous avons mis en évidence l’existence de phénomènes d’auto-organisation et de comportements autocatalytiques du front de transition. Cette physique non-linéaire dénote un comportement actif du cristal, par suite d’une subtile préparation autour d’un état instable. Ces comportements rappellent les structures dissipatives de Turing et ouvrent des perspectives fascinantes pour cette thématique, tant sur le plan expérimental que théorique. / This thesis work is devoted to visualization by optical microscopy of thermo- and photo-induced phase transitions, in switchable spin transition single crystals. The study of crystals of the compound [{Fe (NCSe) (py) 2} 2 (m-bpypz)] showed the possibility to control reversibly the dynamics of the HS/LS interface through a photo-thermal effect generated by an irradiation of the whole crystal or using a spatially localized light spot on the crystal surface. The investigations of the effect of the light intensity on the transition temperature have highlighted the importance of the coupling between the crystal and the thermal bath in these experiments. Concomitantly, we developped a reaction diffusion model allowing to describe and iden-tify the relevant physical parameters involved in the control of the movement of HS/LS interface. The obtained results are very encouraging and reproduce the main features of the experimental data. However the origin of the interface orientation observed by the optical microscopy in the crystal of the compound [{Fe (NCSe) (py) 2} 2 (m-bpypz)] re-mained mysterious, and needed an elastic approach to be handled. At this end, an electro-elastic model including the volume change at the spin transition was developed. By taking into account for the anisotropy of the unit cell deformation at the transition, we were able to reproduce quantitatively the experimental HS/LS interface orientation. This result confirms the crucial role of the lattice symmetry and its elastic properties in the emergence of a stable interface orientation. The last part of the thesis is devoted to the investigation of photo-induced effects at very low temperatures (~10K). There, we visualized for the first time the real time transformation of a single crystal under LIESST (Light Induced Excited Spin State Trapping) effect as well as its subsequent relaxation at higher temperatures. We have also studied the light induced instabilities through investigation on the LITH (Light Induced Thermal Hysteresis) loops. Around the latter, a fascinating world made of nonlinear effects, and patterns formation emerged, recalled the well known Turing structures. These results lead to new horizons that will give access to new theories and original experimental observations that will enrich the topics opening the new avenues to study of nonlinear phenomena in spin crossover solids.

Indiana University-Purdue University Indianapolis (IUPUI) / The details of Polarization Modulation Near-Field Scanning Optical Microscopy (PM-NSOM) are presented. How to properly calibrate and align the system is also introduced. A measurement of Muscovite crystal is used to display the capabilities of the setup. Measurements of supported Lβʹ 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) lipid bilayers are presented, emphasizing how it was tooled in exploiting the anisotropic nature of the acyl chains. A discussion of how the effective retardance (ΔS = 2π( n_e-n_o )t/λ) and the direction of the projection of the acyl chains (θ) are measured simultaneously is given, (where t is the thickness of the bilayer and λ is the wavelength of light used). It is shown from ΔS the birefringence (ne-no) of the bilayer is determined, by assuming the acyl chain tilt with respect to the membrane's normal to be ϕ ≈ 32. Time varying experiments show lateral diffusions of ~ 2 x 10-12 cm2/s. Temperature controlled PM-NSOM is shown to be a viable way to determine the main phase transition temperature (Tm) for going from the gel Lβʹ to liquid disorder Lα state of supported DPPC bilayers. A change of ΔS ~ (3.8 +/- 0.3 mrad) at the main phase transition temperature Tm (≈41^o C) is observed. This agrees well with previous values of (ne-no) and translates to an assumed <ϕ> ~ 32^o when T < Tm and 0^o when T > Tm. Evidence of supper heating and supper cooling will be presented, along with a discussion of the fluctuations that occur around Tm. Finally it is shown how physical parameters such as the polarizability are extracted from the data. Values of the transverse (αt) and longitudinal (αl) polarizabilites of the acyl chains are shown to be, αt = 44.2 Å3 and αl = 94.4 Å3, which correspond well with the theoretical values of a single palmitic acid (C16) αt = 25.14 Å3 and αl = 45.8 Å3.

In the past few years, studies regarding new bio-based materials have led to an increased attention in the nanoscale product of cellulose, called nanocellulose. This biodegradable and renewable material has interesting physical, optical and thermal properties. The optical properties could be affected by tuning the nanostructure of the material, which makes it interesting for further investigation. The promising properties of nanocellulose can be useful in many different applications. The aim of this work was therefore to study the optical properties of nanocellulose, and to examine if the material is suitable for spectral design of camouflage or in passive cooling applications. The optical properties of a nanocellulose, specifically cellulose nanofiber (CNF), have been studied. Freestanding CNF films and CNF films deposited on glass substrates were made and characterized by spectroscopy, ellipsometry, BRDF measurements, and optical microscopy. The freestanding samples were examined with different CNF concentrations of 0.52% and 1.0%, and different thicknesses. The samples on glass substrates all had a concentration of 1.0% CNF, but with different amount deposited solution which was either drop or spin coated. The freestanding CNF samples show high transmission in the visual region and relatively high emissivity in the atmospheric windows. This implies that it can be used as an effective material for passive radiative cooling. A thicker sample could also be used to increase the emissivity in the atmospheric windows and improve the ability for passive cooling. The low reflectance, and high emissivity in the atmospheric windows can be promising for use in camouflage applications, according to earlier studies. However, the suitable properties are very dependent on the spectral response of the background. Additional measurements need to be performed and more specified scenarios are necessary to draw any further conclusions.

The Arlanda area is a construction intensive area facing problems with risk of leaching of arsenic (As) from the bedrock to surface- and groundwater. Construction projects in the area have had problems with high levels of As in the bedrock and the risk of leaching increases through processing of aggregates and blasting of the bedrock. Additionally, there are high concentrations of As in potable water and elevated concentrations are correlated with occurrences of metasedimentary rock, but may also be related to other rock types. The existing geological information of the area was collected in the 1960´s and modern petrographic information as well as modelling of P-T and redox conditions are needed to understand the As mineralogy of the bedrock. Methods used in this project include field work, optical microscopy, electron microprobe analyses, geothermometry calculations, pseudosection modelling in Perple_X and geochemical modelling in PHREEQC. The results indicate that the As-rich bedrock domain include rocks of both igneous and sedimentary origin. As-bearing minerals löllingite and arsenopyrite were found in the matrix of two of the metasedimentary rock samples, while no As-minerals were found in metavolcanic samples. P-T estimates from several geothermobarometry models all suggest amphibolite facies metamorphism for the area, with pressure of 3.0-5.5 kbar and temperature of 490-640 °C. Simple modelling of equilibration of löllingite and arsenopyrite in pure water indicate that As(III) is the dominating oxidation state of As and that the molality of As increases with increasing T and decreasing pH. The results of this thesis provide new information on the petrography and P-T conditions for metamorphism of As-bearingsupracrustal rocks in the Arlanda area, but future research is needed to be able to predict the spatial occurrence of As in the bedrock. / Arlandaområdet är ett av de mest expansiva områdena i Sverige där en stor mängd infrastrukturprojekt är planerade under de närmaste 5-20 åren. Tidigare byggnadsprojekt i området har dock stött på problem med höga bakgrundshalter av arsenik (As) i berggrunden och det finns även en risk för urlakning av As från berggrunden till både yt-och grundvatten. Denna risk ökar under byggnadsarbeten i och med till exempel sprängning av berg. Ytterligare ett problem är att det i området runtomkring Arlanda ofta är höga halter av arsenik i dricksvattenbrunnar. Från data över As-halter i bergborrade brunnar har man kunnat se att höga halter av As ofta förekommer i metasedimentära bergarter, men även kan uppträda i andra bergarter. Den tillgängliga geologiska informationen över området är insamlad på 60-talet och ny petrografisk information, samt modellering av tryck- och temperaturförhållanden är nödvändig för att förstå förekomst av As i berggrunden. Målet med detta projekt är att med hjälp av fältarbete, optisk- och elektronmikroskopering, samt termodynamisk modellering få djupare kunskap kring ytbergarterna i området och utvärdera förekomsten av arsenik i dessa. Under vilka tryck- och temperaturförhållanden som de metamorfa bergarterna omvandlats studeras genom beräkningar från mineralsammansättningar samt modellering i programmet Perple_X. Resultatet från projektet visar att bergarter i As-anrikade zoner är av både magmatiskt och sedimentärt ursprung. Arsenikmineralen löllingit och arsenikkis dokumenterades endast i bergarter av sedimentärt ursprung. Bergarternas kemiska sammansättning tyder också på att de högsta As-halterna finns i de metasedimentära bergarterna. Modellering i PHREEQC visar att As(III) är den dominerande formen av As när löllingit och arsenikkis reagerar med vatten. Tryck- och temperaturberäkningar samt tryck- och termodynamisk modellering tyder på metamorfos under amfibolitfacies, med tryck omkring 3.0-5.5 kbar och temperatur omkring 490-640 °C. Resultaten från detta projekt ger ny information om de metamorfa bergarterna i Arlanda området och förekomst av As i dessa. Vidare studier är nödvändiga för att kunnaförutse i vilken form och i vilka bergarter As förekommer.

L’imagerie biomédicale d’élastographie, visant à cartographier les propriétés mécaniques des tissus mous, est explorée à travers des approches multiphysiques et multimodales regroupant la microscopie optique d’une part et l’imagerie par résonance magnétique associée à la stimulation électrique d’autre part. Tout d’abord, une méthode de génération d’ondes élastiques, nécessaires aux expériences d’élastographie par résonance magnétique (ERM), suivant une approche de stimulation in situ est présentée. Cette dernière repose sur l’induction de forces de Lorentz, sources de mouvement, dans un matériau soumis à une stimulation électrique et exposé au champ magnétique d’un système d’imagerie par résonance magnétique (IRM). Un dispositif expérimental d’ERM par force de Lorentz est proposé et testé avec des fantômes de gélatine de différentes rigidités. Le champ ondulatoire mesuré est démontré provenir de la force de Lorentz établie au sein des échantillons et a permis la reconstruction d’images de rigidité au moyen d’un algorithme d’inversion habituellement appliqué au traitement de données cliniques. La faible amplitude des déplacements capturés suggère toutefois que les déformations induites seraient difficilement mesurables par ERM dans des conditions de stimulation électrique sûres. Si cette caractéristique questionne la faisabilité de l’ERM par force de Lorentz, elle ouvre la voie à l’application simultanée de l’ERM conventionnelle et de la stimulation électrique dans une même région d’intérêt, permettant l’analyse de la réponse biomécanique de tissus biologiques à une stimulation électrique. Cet aspect est abordé à travers une étude numérique de stimulation transcrânienne par courant alternatif associée à l’ERM dans un modèle 3D de cerveau de souris. L’impact des forces de Lorentz, inhérentes à cette combinaison, sur les reconstructions de viscoélasticité est étudié via un algorithme d’inversion non-linéaire par sous-zones. Un volet d’imagerie de la conductivité ohmique par résonance magnétique est incorporé aux simulations de façon à approximer la distribution de courant électrique induit par stimulation. L’union de ces différentes approches pourrait être pertinente dans le cadre de la caractérisation du cerveau et révéler davantage de mécanismes physiologiques ensemble qu’individuellement. Dans un second temps, l’évaluation de la viscoélasticité des tissus biologiques est abordée à l’échelle de la cellule grâce à la micro-élastographie optique. Cette approche repose également sur la génération, la mesure et l’analyse d’ondes élastiques harmoniques dans le milieu sondé et est appliquée à des ovocytes de souris d’un diamètre avoisinant 85 µm. Les déformations locales sont mesurées dans le plan des images expérimentales acquises à une fréquence de 200 kHz et sont traitées par un modèle de déplacements 3D exploitant la symétrie planaire des ovocytes imagés. La reconstruction de cartes de viscoélasticité est assurée par l’algorithme itératif d’inversion non-linéaire par sous-zones, emprunté à l’élastographie par résonance magnétique. Les images de module de stockage produites démontrent un niveau de précision supérieur aux images obtenues par inversion directe, sur la base de différentiabilité des structures internes de l’ovocyte. La génération inédite d’images du module de perte dans de telles cellules et la robustesse de l’ensemble de cette approche sont des indicateurs encourageant d’une éventuelle applicabilité future aux procédures de fécondation in vitro. / Biomedical elastography imaging, aiming at mapping the mechanical properties of soft tissues, is explored through multiphysical and multimodal approaches combining optical microscopy on one hand and magnetic resonance imaging associated with electrical stimulation on the other hand. First, a method for generating elastic waves, necessary for magnetic resonance elastography (MRE) experiments, following an in situ actuation approach is presented. The latter is based on the induction of Lorentz forces, sources of motion, in a material subjected to an electrical stimulation and exposed to the magnetic field of a magnetic resonance imaging (MRI) system. An experimental set-up for Lorentz force MRE is proposed and tested with gelatin phantoms of different stiffness. The measured wave field is shown to originate from the Lorentz force established within the samples and allowed the reconstruction of stiffness images using an inversion algorithm typically applied to clinical data processing. The small amplitude of the captured displacements, however, suggests that the induced deformations would be difficult to measure by MRE under safe electrical stimulation conditions. If this characteristic questions the feasibility of Lorentz force MRE, it opens the way to the simultaneous application of conventional MRE and electrical stimulation in the same region of interest, allowing the analysis of the biomechanical response of biological tissues to electrical stimulation. This aspect is addressed through a numerical study of transcranial alternating current stimulation associated with MRE in a 3D mouse brain model. The impact of Lorentz forces, inherent to this combination, on viscoelasticity reconstructions is studied via a nonlinear subzone inversion algorithm. A magnetic resonance imaging component of the ohmic conductivity is incorporated into the simulations in order to approximate the electrical current distribution induced by stimulation. The union of these different approaches could be relevant for the characterization of the brain and may reveal more physiological mechanisms together than individually. In a second step, the evaluation of the viscoelasticity of biological tissues is approached at the cell level using optical microelastography. This approach is also based on the generation, measurement and analysis of harmonic elastic waves in the probed medium and is applied to mouse oocytes with a diameter of about 85 µm. Local deformations are measured in the plane of the experimental images acquired at a frequency of 200 kHz and are processed by a 3D displacement model exploiting the planar symmetry of the imaged oocytes. Viscoelasticity maps are reconstructed using the iterative subzone nonlinear inversion algorithm borrowed from magnetic resonance elastography. The storage modulus images produced demonstrate a higher level of accuracy than images obtained by direct inversion, based on the differentiability of the internal structures of the oocyte. The novel generation of loss modulus images in such cells and the robustness of the overall approach are encouraging indicators of potential future applicability to in vitro fertilization procedures.

Near-field optical microscopy allows the nondestructive examination of surfaces with a spatial resolution far below the diffraction limit of Abbe. In fact, the resolution of this kind of microscope is not at all dependent on the wavelength, but is typically in the range of 10 to 100 nanometers. On this scale, many materials are anisotropic, even though they might appear isotropic on the macroscopic length scale. In the present work, the previously never studied interaction between a scattering-type near-field probe and an anisotropic sample is examined theoretically as well as experimentally. In the theoretical part of the work, the analytical dipole model, which is well known for isotropic samples, is extended to anisotropic samples. On isotropic samples one observes an optical contrast between different materials, whereas on anisotropic samples one expects an additional contrast between areas with different orientations of the same dielectric tensor. The calculations show that this anisotropy contrast is strong enough to be observed if the sample is excited close to a polariton resonance. The experimental setup allows the optical examination in the visible and in the infrared wavelength regimes. For the latter, a free-electron laser was used as a precisely tunable light source for resonant excitation. The basic atomic force microscope provides a unique combination of different scanning probe microscopy methods that are indispensable in order to avoid artifacts in the measurement of the near-field signal and the resulting anisotropy contrast. Basic studies of the anisotropy contrast were performed on the ferroelectric single crystals barium titanate and lithium niobate. On lithium niobate, we examined the spectral dependence of the near-field signal close to the phonon resonance of the sample as well as its dependence on the tip-sample distance, the polarization of the incident light, and the orientation of the sample. On barium titanate, analogous measurements were performed and, additionally, areas with different types of domains were imaged and the near-field optical contrast due to the anisotropy of the sample was directly measured. The experimental results of the work agree with the theoretical predictions. A near-field optical contrast due to the anisotropy of the sample can be measured and allows areas with different orientations of the dielectric tensor to be distinguished optically. The contrast results from variations of the dielectric tensor components both parallel and perpendicular to the sample surface. The presented method allows the optical examination of anisotropies of a sample with ultrahigh resolution, and promises applications in many fields of research, such as materials science, information technology, biology, and nanooptics. / Die optische Nahfeldmikroskopie ermöglicht die zerstörungsfreie optische Unter- suchung von Oberflächen mit einer räumlichen Auflösung weit unterhalb des klas- sischen Beugungslimits von Abbe. Die Auflösung dieser Art von Mikroskopie ist unabhängig von der verwendeten Wellenlänge und liegt typischerweise im Bereich von 10-100 Nanometern. Auf dieser Längenskala zeigen viele Materialien optisch anisotropes Verhalten, auch wenn sie makroskopisch isotrop erscheinen. In der vorliegenden Arbeit wird die bisher noch nicht bestimmte Wechselwirkung einer streuenden Nahfeldsonde mit einer anisotropen Probe sowohl theoretisch als auch experimentell untersucht. Im theoretischen Teil wird das für isotrope Proben bekannte analytische Dipol- modell auf anisotrope Materialien erweitert. Während fÄur isotrope Proben ein reiner Materialkontrast beobachtet wird, ist auf anisotropen Proben zusätzlich ein Kontrast zwischen Bereichen mit unterschiedlicher Orientierung des Dielektrizitätstensors zu erwarten. Die Berechnungen zeigen, dass dieser Anisotropiekontrast messbar ist, wenn die Probe nahe einer Polaritonresonanz angeregt wird. Der verwendete experimentelle Aufbau ermöglicht die optische Untersuchung von Materialien im sichtbaren sowie im infraroten Wellenlängenbereich, wobei zur re- sonanten Anregung ein Freie-Elektronen-Laser verwendet wurde. Das dem Nahfeld- mikroskop zugrunde liegende Rasterkraftmikroskop bietet eine einzigartige Kombi- nation verschiedener Rastersondenmikroskopie-Methoden und ermöglicht neben der Untersuchung von komplementären Probeneigenschaften auch die Unterdrückung von mechanisch und elektrisch induzierten Fehlkontrasten im optischen Signal. An den ferroelektrischen Einkristallen Lithiumniobat und Bariumtitanat wurde der anisotrope Nahfeldkontrast im infraroten WellenlÄangenbereich untersucht. An eindomÄanigem Lithiumniobat wurden das spektrale Verhalten des Nahfeldsignals sowie dessen charakteristische Abhängigkeit von Polarisation, Abstand und Proben- orientierung grundlegend untersucht. Auf Bariumtitanat, einem mehrdomänigen Kristall, wurden analoge Messungen durchgeführt und zusätzlich Gebiete mit ver- schiedenen Domänensorten abgebildet, wobei ein direkter nachfeldoptischer Kon- trast aufgrund der Anisotropie der Probe nachgewiesen werden konnte. Die experimentellen Ergebnisse dieser Arbeit stimmen mit den theoretischen Vorhersagen überein. Ein durch die optische Anisotropie der Probe induzierter Nahfeldkontrast ist messbar und erlaubt die optische Unterscheidung von Gebie- ten mit unterschiedlicher Orientierung des Dielektriziätstensors, wobei eine Än- derung desselben sowohl parallel als auch senkrecht zur Probenoberfläche messbar ist. Diese Methode erlaubt die hochauflösende optische Untersuchung von lokalen Anisotropien, was in zahlreichen Gebieten der Materialwissenschaft, Speichertech- nik, Biologie und Nanooptik von Interesse ist.

Near-field optical microscopy allows the nondestructive examination of surfaces with a spatial resolution far below the diffraction limit of Abbe. In fact, the resolution of this kind of microscope is not at all dependent on the wavelength, but is typically in the range of 10 to 100 nanometers. On this scale, many materials are anisotropic, even though they might appear isotropic on the macroscopic length scale. In the present work, the previously never studied interaction between a scattering-type near-field probe and an anisotropic sample is examined theoretically as well as experimentally. In the theoretical part of the work, the analytical dipole model, which is well known for isotropic samples, is extended to anisotropic samples. On isotropic samples one observes an optical contrast between different materials, whereas on anisotropic samples one expects an additional contrast between areas with different orientations of the same dielectric tensor. The calculations show that this anisotropy contrast is strong enough to be observed if the sample is excited close to a polariton resonance. The experimental setup allows the optical examination in the visible and in the infrared wavelength regimes. For the latter, a free-electron laser was used as a precisely tunable light source for resonant excitation. The basic atomic force microscope provides a unique combination of different scanning probe microscopy methods that are indispensable in order to avoid artifacts in the measurement of the near-field signal and the resulting anisotropy contrast. Basic studies of the anisotropy contrast were performed on the ferroelectric single crystals barium titanate and lithium niobate. On lithium niobate, we examined the spectral dependence of the near-field signal close to the phonon resonance of the sample as well as its dependence on the tip-sample distance, the polarization of the incident light, and the orientation of the sample. On barium titanate, analogous measurements were performed and, additionally, areas with different types of domains were imaged and the near-field optical contrast due to the anisotropy of the sample was directly measured. The experimental results of the work agree with the theoretical predictions. A near-field optical contrast due to the anisotropy of the sample can be measured and allows areas with different orientations of the dielectric tensor to be distinguished optically. The contrast results from variations of the dielectric tensor components both parallel and perpendicular to the sample surface. The presented method allows the optical examination of anisotropies of a sample with ultrahigh resolution, and promises applications in many fields of research, such as materials science, information technology, biology, and nanooptics. / Die optische Nahfeldmikroskopie ermöglicht die zerstörungsfreie optische Unter- suchung von Oberflächen mit einer räumlichen Auflösung weit unterhalb des klas- sischen Beugungslimits von Abbe. Die Auflösung dieser Art von Mikroskopie ist unabhängig von der verwendeten Wellenlänge und liegt typischerweise im Bereich von 10-100 Nanometern. Auf dieser Längenskala zeigen viele Materialien optisch anisotropes Verhalten, auch wenn sie makroskopisch isotrop erscheinen. In der vorliegenden Arbeit wird die bisher noch nicht bestimmte Wechselwirkung einer streuenden Nahfeldsonde mit einer anisotropen Probe sowohl theoretisch als auch experimentell untersucht. Im theoretischen Teil wird das für isotrope Proben bekannte analytische Dipol- modell auf anisotrope Materialien erweitert. Während fÄur isotrope Proben ein reiner Materialkontrast beobachtet wird, ist auf anisotropen Proben zusätzlich ein Kontrast zwischen Bereichen mit unterschiedlicher Orientierung des Dielektrizitätstensors zu erwarten. Die Berechnungen zeigen, dass dieser Anisotropiekontrast messbar ist, wenn die Probe nahe einer Polaritonresonanz angeregt wird. Der verwendete experimentelle Aufbau ermöglicht die optische Untersuchung von Materialien im sichtbaren sowie im infraroten Wellenlängenbereich, wobei zur re- sonanten Anregung ein Freie-Elektronen-Laser verwendet wurde. Das dem Nahfeld- mikroskop zugrunde liegende Rasterkraftmikroskop bietet eine einzigartige Kombi- nation verschiedener Rastersondenmikroskopie-Methoden und ermöglicht neben der Untersuchung von komplementären Probeneigenschaften auch die Unterdrückung von mechanisch und elektrisch induzierten Fehlkontrasten im optischen Signal. An den ferroelektrischen Einkristallen Lithiumniobat und Bariumtitanat wurde der anisotrope Nahfeldkontrast im infraroten WellenlÄangenbereich untersucht. An eindomÄanigem Lithiumniobat wurden das spektrale Verhalten des Nahfeldsignals sowie dessen charakteristische Abhängigkeit von Polarisation, Abstand und Proben- orientierung grundlegend untersucht. Auf Bariumtitanat, einem mehrdomänigen Kristall, wurden analoge Messungen durchgeführt und zusätzlich Gebiete mit ver- schiedenen Domänensorten abgebildet, wobei ein direkter nachfeldoptischer Kon- trast aufgrund der Anisotropie der Probe nachgewiesen werden konnte. Die experimentellen Ergebnisse dieser Arbeit stimmen mit den theoretischen Vorhersagen überein. Ein durch die optische Anisotropie der Probe induzierter Nahfeldkontrast ist messbar und erlaubt die optische Unterscheidung von Gebie- ten mit unterschiedlicher Orientierung des Dielektriziätstensors, wobei eine Än- derung desselben sowohl parallel als auch senkrecht zur Probenoberfläche messbar ist. Diese Methode erlaubt die hochauflösende optische Untersuchung von lokalen Anisotropien, was in zahlreichen Gebieten der Materialwissenschaft, Speichertech- nik, Biologie und Nanooptik von Interesse ist.

Mémoire numérisé par la Division de la gestion de documents et des archives de l'Université de Montréal.