Les nano-antennes optiques constituent un élément clé pour le contrôle et l’intéraction lumière/matière à l’échelle nanométrique. Ces systèmes opèrent dans le domaine de l’optique visible et proche infrarouge. Les propriétés de ces composants sont contrôlées en modifiant la taille, la forme et le matériau utilisé. Ces paramètres sont ajustés par les processus de fabrication de l’antenne. Dans le domaine des radio-fréquences, le tuner permet d’ajuster la fréquence de résonance de l’antenne de façon dynamique. Nous avons dans le cadre de cette thèse voulu adapter ce concept de tuner au domaine de l’optique. Le principe employé consiste à changer la résistance de charge de l’antenne, c’est-à-dire l’indice du milieu électrique environnant. Pour cela, nous avons utilisé un matériau anisotrope constitué de molécules de cristaux liquides. L’indice optique est alors modifié par l ’application d’un champ électrique statique. Le changement des propriétés spectrales ainsi que de diffusion d’une antenne de type dimère sont ici démontrées.Toujours en analogie avec les antennes radio-fréquences, nous avons étudié la propriété de transduction électron-photon dans le cas des antennes optiques. Dans ce but, nous avons considéré deux configurations. La première concerne l’utilisation de nanotubes de carbone placés dans une configuration de transistor à effet de champ. Ces objets émettent de la lumière par une recombinaison de paires électrons-trous dans le domaine des longueurs d’ondes Télécom. La seconde configuration emploie des jonctions tunnels fabriquées par électro-migration. Dans ce cas là, la jonction est assimilée à une antenne à interstice. A cause des faibles dimensions des jonctions (autour de 1 nm), nous nous sommes intéressés à la réponse en optique non linéaire de ses objets. Cette technique permet de localiser la jonction tunnel grâce à une forte exaltation du signal. L’etude des différentes caractérisques de ses jonctions sont ici présentées. Une fois la transduction du signal réalisée par l’antenne radiofréquence, celui-ci est acheminé via une ligne de transmission. A l’ échelle nanométrique, les guides plasmoniques s’avèrent être un type de structure approprié. Dans ce cas, les guides peuvent à la fois servir d’´electrode mais aussi de guide. Dans le cadre de cette thèse, nous avons étudié par microscopie à fuites radiatives, dans l’espace direct et réciproque, la plus simple des géométries : le guide ruban métallique. Nous avons cherché à comprendre, pourquoi ce type de structure présente une largeur de coupure. / Optical nano-antennae are the new class of components to control light/matterinteraction at the nanoscale. These devices are operating in the visible to near infraredpart of the spectrum. The properties of these nano objects are controlled by theform, the size and the material.In the radio frequency domain, the tuner changes dynamically the operatingwavelength of the antenna. In this thesis work, we search to transfer this conceptto the nanoscale. The principle is to change the load impedance of the antenna, i.e.changing the optical index of the dielectric medium around the nano-object. Forthat we used anisotropic liquid cristal molecules. The value of the optical index iscontrolled by applying an external electrical static field. The effects on the spectraland scattering properties are demonstrated on a single dimer nano-antenna.However with the microwave antennae, we were interesting to the electronsphotonstransduction with an optical antenna. In this mind, we studied two differentsconfigurations. The first one concerns the use of carbon nanotubes placedin a field effect transistor configuration. These nano-objects emit light in the Telecomwavelength range by a radiative combination of electrons and holes. the secondconfiguration used planar tunnel junctions made by electromigration. In this case,the junctions are view as an optical gap antenna. Because the gap are very small(around 1 nm), we have studied the nonlinear optical response of these objects. Thisnonlinear optical characterization allows to determined the location of the tunneljunctions by an enhancement of the optical signal. The results about the properties(electrical and optical) of these tunnel junctions are presented.Once the transduction by the radio frequency antenna is achieved, this signalis transporting by a transmission line. By transposition at the nanoscale, the plasmonicswaveguides prove to be the most appropriate structure. In this case, theycould be used as an electrode or a waveguide. In this thesis work, we have studiedby leakage radiation microscopy, in the direct and reciprocal space, the simplestgeometry : plasmonic metal strips. We search to understand why these structureshave a cut-off width.

La génération de seconde harmonique magnétique (mSHG pour magnetic Second Harmonic Generation) est un phénomène physique très sensible apparaissant grâce aux brisures de symétrie aux niveaux des surfaces et interfaces des structures métalliques magnétiques. Elle constitue donc un outil puissant pour explorer ce type d'interfaces et des nanostructures. Dans ce travail, nous nous intéressons aux couplages et interactions entre la mSHG et les ondes électromagnétiques pouvant se propager en surface des matériaux. Un intérêt spécifique est porté sur l’ excitation de (i) plasmon polaritons de surfaces (SPP) dans des films métalliques en structures multicouches, (ii) d'anomalies de diffraction (dîtes de Wood) dans des nanostructures métalliques périodiques. Pour étudier l'influence de l'excitation linéaire et non-linéaire des SPP sur la mSHG, l'intensité du signal réfléchi par génération de seconde harmonique (SH) et le contraste magnétique lié à ce signal ont été mesurés par la technique de l'effet Kerr magnéto-optique transverse (MOKE) en fonction de l'angle d'incidence. Via l'utilisation de sources lasers femtosecondes émettant dans le proche infrarouge, domaine spectral où les variations de la dispersion des SPP et du coefficient d'amortissement sont significatives, nous avons pu distinguer les différentes contributions linéaires et non-linéaires aux processus d'excitation. Ce travail de thèse a ainsi permis de montrer que l’accord de phase entre la mSHG et les ondes électromagnétiques de surface peuvent contribuer très efficacement à l'augmentation des signaux SH et de contraste magnétique associé. / Owing to surface and interface sensitivity, the magnetic Second Harmonic Generation (mSHG) represents a useful tool to probe magnetic interfaces and nanostructures. This work investigates the coupling and interaction of the mSHG with electromagnetic waves propagating along the surface. Two types of surface waves have been studied: (i) surface plasmon polaritons (SPP) at surfaces of metallic thin films and multilayers, and (ii) the diffraction anomaly at the surface of periodically arranged metallic nanostructures. To study influence of linear and nonlinear excitation of surface waves on the mSHG, the reflected second harmonic (SH) intensity and the magnetic SH contrast in the transverse magneto-optical geometry were measured as a function of the angle of incidence. The use of different femtosecond light sources in the near-infrared optical range, where the SPP dispersion and damping exhibit significant variations, made it possible to disentangle linear and nonlinear contributions to the excitation of surface waves. In this thesis, it is proven that phase-matching of the mSHG and surface electromagnetic waves can lead to the enhancement of both the SH yield and the nonlinear magneto-optical signal. These results are important for controlling of the nonlinear magneto-optical response and could impact the development of magnetic storage devices, label-free biosensors and nonlinear magneto-optical switches.

This dissertation presents the novel creation of a hybrid D-fiber electro-optic polymer electric field sensor. The sensor is made by removing a portion of the cladding from a D-shaped optical fiber, thus exposing the core to interaction with external stimulus. Then, an electro-optic polymer is deposited, partially replacing the core of the fiber. Next, the polymer is poled to endow it with electro-optic properties. This sensor is packaged in order to restore its mechanical strength. Because D-fiber is not intrinsically compatible with standard optical equipment it is fusion spliced to standard polarization maintaining fiber. Finally the sensor is tested for electro-optic sensitivity. The hybrid D-fiber electric field sensors designed and fabricated in this work meet the requirements of mechanical strength, temporal stability, minimal perturbation of the electric field by the sensor, and a small and flexible cross-sectional area so that it can be embedded into the device under test. A fully packaged hybrid electro-optic polymer D-fiber electric field sensor which is capable of detecting electric fields of 50 V/m at a frequency of 6 GHz is produced. The sensor's electro-optic response is shown to be temporally stable. Additionally, the sensor is physically robust, and physically and electrically non-intrusive. This work also adds a thorough understanding of the design and fabrication of D-fiber waveguides with a polymer material deposited in the core. Several new fabrication techniques are developed and presented. A path to greater electric field sensitivity is outlined for future research.

[pt] O objetivo deste trabalho foi desenvolver métodos eficientes e reprodutíveis de crescimento de monocamadas de WS2, MoS2 e outras heteroestruturas verticais por deposição química em fase de vapor à pressão atmosférica (APCVD). A monocamada separada destes materiais tem grande importância na fabricação de novos dispositivos óticos e Nano eletrônicos. Dispositivos finos e de baixo custo necessitam temperaturas em torno de 800 graus celsius, o que é um problema para aplicações mencionadas acima. Nesta tese, nós propusemos uma nova rota usando APCVD para crescer monocamadas de MoS2 a 550 graus celsius, usando sódio como catalisador. Nós produzimos monocristais e poli cristais controlando a razão de precursores NaNO3/MoO3 e tempo de crescimento. Usando cálculos de primeiros princípios, mostramos que o sódio atua como centro de nucleação para o processo de síntese. A razão de precursores é crucial para diminuir a energia de formação e a temperatura de síntese. Cálculos de primeiros princípios e experimentos concordam que uma razão ideal é em torno de 0.3, proporcionando uma queda de 250 graus celsius na temperatura de crescimento. Nós investigamos as amostras crescidas por APCVD usando espectroscopia de fotoelétrons induzidos por raios-X, microscopia de força atômica, espectroscopia Raman, fotoluminescência e mediadas de transporte. Dicalcogenetos de metais de transição (TMD) dispostos em poucas camadas permitem-nos criar materiais e estudar novos fenômenos físicos. A sequência de empilhamento dos TMDs pode modificar suas propriedades opticas e elétricas. Também sintetizamos poucas camadas de MoS2 e WS2 usando APCVD. Duas e três camadas de WS2, MoS2 e suas heteroestruturas verticais foram caracterizadas através de geração de segundo harmônico (SHG). SHG mostra que as bicamadas crescidas com ângulos de rotação relativos de 0 grau e 60 graus possuem diferentes fases de empilhamento. O SHG do empilhamento bicamada com ângulo relativo de 0 graus aumentos, enquanto para amostras com empilhamento de 60 graus foi zerado. Este comportamento do SHG sugere que duas camadas de MoS2 ou WS2, quando empilhados a 0 graus não possuem simetria de inversão para 3R(AB) entre as camadas inferiores e superiores, enquanto as camadas de 60 graus possuem simetria de inversão (centrossimétricas) e possuem empilhamento na forma 2H(AA). Finalmente, dispositivos foram fabricados em amostras de boa qualidade para a investigação de sua performance elétrica. Os dispositivos mostram comportamento típico tipo-n e sua mobilidade foi estimada a partir das curvas de transporte. A dependência dos modos Raman das nossas amostras de heteroestruturas também foi estudada. Aplicando uma tensão nos dispositivos, o modo A1 mostrou um desvio para o azul e um novo modo surge em 410 cm-1, atribuídos defeitos (D) no cristal. / [en] The aim of this work was to develop reliable and repeatable methods for growing high-quality monolayer MoS2, WS2, and their vertical heterostructure by atmospheric pressure chemical vapor deposition (APCVD) technique. The monolayer of these materials have vital importance in the fabrication of new optical and nanoelectronic devices. Thin and low-cost devices have increased the demand for new synthesis processes. Usually, the synthesis requires temperatures around 800 Celsius degrees, which is an issue for applications mentioned above. In this thesis, we propose a new route using the APCVD technique to grow monolayers of MoS2 at 550 Celsius degrees mediated by sodium as a catalyst. We have produced single crystals and polycrystals by controlling the NaNO3/MoO3 precursor s ratio and growth time. Using first-principles calculations, we find out that sodium is the nucleation site of the growth process. The precursor s ratio is crucial to decrease the energy formation and the synthesis temperature. Firstprinciples calculations and experiments agree with the ideal precursor s rate of 0.3 and with the decrease of the synthesis temperature of 250 Celsius degrees. We investigated the CVD grown sample with X-ray photoelectron spectroscopy, atomic force microscopy, Raman spectroscopy, photoluminescence spectroscopy, and transport experiments. Few layers of TMDs allow us to create new materials and find new physical phenomena. The stacking sequence in few-layer TMDs can significantly impact on their electrical and optical properties.We also synthesized few layers of MoS2 and WS2 via APCVD. Two and three layers of MoS2, WS2, and their vertical heterostructures were characterized by second harmonic generation (SHG). The SHG shows that the layers in bilayers grow with 0 degrees or 60 degrees has different phase stacking. The SHG from 0 degrees stacked bilayer has increased when compared to monolayer, while the generated signal from bilayer with 60 degrees stacking is zero. This behavior of SHG suggests that the two layers of MoS2 or WS2 when stacked at 0 degrees have no inversion symmetry to 3R(AB) phase stacking between the top layer and the bottom layer. While when stacked with 60 degrees has inversion symmetry (Centrosymmetric) and have 2H(AA0) phase stacking. Finally, the devices were fabricated on good quality samples to investigate their electrical performance. The fabricated devices show typical n-type behavior and mobility was estimated by measuring transport curves. The dependence of Raman modes of our heterostructure device with electron doping was also studied. By applying a voltage across our device the A1 mode shows blueshift and a new mode emerges at ~ 410 cm-1, which is attributed to the defects (D) in the crystal.

Durch neue Ansätze zur Charakterisierung molekularer und nanokristalliner Materialien spiegelt die vorliegende Arbeit die Synergie von linearer Optik über Ultrakurzzeitphysik zur nichtlinearen Optik wider. Angefangen mit der linearen diffusen Reflektanz (Remission) zur Bestimmung des spektralen Reflexionsvermögens von Pulverpartikeln, erlaubt die hier gezeigte alternative Herangehensweise (s. Kapitel 2) nicht nur ein vereinfachtes Messen der Remission zur Analyse von Materialzusammensetzungen, Verunreinigungen und Co-Dotierungen, sondern eröffnet zudem über Monte-Carlo Simulationen, kombiniert mit der Kubelka-Munk Theorie und der Mie Streuung, auch den Zugang zu dem ansonsten experimentell unzugänglichen Absorptionskoeffizienten von nicht-transluzenten Proben. Die präsentierten Mess- und Simulationsergebnisse an Pulvertabletten aus Rutil-Titandioxid (TiO2) und Cer-dotierten Yttrium Aluminium Granat (YAG:Ce3+) sind mit den bisherigen in der Literatur vorliegenden Ergebnissen konsistent oder zumindest vergleichbar. Auch lassen sich nach Modifikation der Kubelka-Munk Funktion die Bandkanten-Energien Eg der mikro- und nanokristallinen Pulverproben mittels so genannter Tauc Plots verifizieren. Basierend auf einer starken Temperatur- und Konzentrationsabhängigkeit lassen sich die Emissionsspektren der oben genannten YAG:Ce3+-Leuchtstoffe aufgrund von Überlappung oder Verschiebung der energetischen Grundniveaus 2F5/2 und 2F7/2 variieren (s. Kapitel 3). Während sich bei Tieftemperaturen um 19K die doppelbandige Natur der Leuchtstoffe zeigt, verbreitern sich die Emissionsbanden bei Raumtemperatur zu einer Einzelbande, womit eine spektral sehr breite Fluoreszenz einhergeht. Mathematische Entfaltungen dieser Spektren zeigen jeweils den prozentualen Beitrag der Relaxation aus dem untersten angeregten Zustand 5d1 in einen der beiden Grundzustände 2F5/2 und 2F7/2 und ebenso den Einfluss der Temperatur und Cer-Konzentration. Tatsächlich führen die experimentellen Ergebnisse der vorliegenden Arbeit zu der Erkenntnis, dass eine der vier untersuchten YAG:Ce3+-Proben eine erhöhte Cer-Konzentration aufweisen muss. Anders als bei den schwach konzentrierten YAG:Ce3+-Proben ist die spektrale Doppelbande des stark konzentrierten Leuchtstoffs selbst bei 19K nur zu erahnen, während der Beitrag des 5d1 --> 2F7/2 Übergangs auf die Gesamtfluoreszenz retrograd zum 5d1 --> 2F5/2 Übergang mit steigender Temperatur sogar abnimmt. Im direkten Anschluss an die spektrale Vermessung der Proben folgen zeitaufgelöste Lebensdauermessungen zur Bestimmung der Nachleuchtdauern dieser Leuchtstoffe mittels Pikosekunden-Laserpulsen (ps-Pulse) (s. Kapitel 3.3). Auch hier stellen sich Unterschiede zwischen den genannten YAG:Ce3+-Proben heraus und untermauern erneut die Annahme unterschiedlicher Cer-Konzentrationen: Während die Nachleuchtdauer der niedrig konzentrierten Leuchtstoffe von der Temperatur nahezu unberührt bleibt, zeigt sich eine bemerkenswerte Temperaturabhängigkeit des 5d1 --> 2F5/2 Übergangs beim YAG:Ce3+ mit hohem Cer-Gehalt. Auf Basis sämtlicher experimenteller Erkenntnisse und einer ausgiebigen Literaturrecherche kann schließlich eine Fremddotierung der Leuchtstoff-Proben nahezu vollständig ausgeschlossen und ein Energieschema für die vorliegenden YAG:Ce3+-Leuchtstoffe mit den wichtigsten optischen Übergängen erstellt werden. In Hinblick auf potentielle holographische Applikationen wie der optischen Datenspeicherung oder Echtzeit-Holographie erweisen sich die in Polydimethylsiloxan eingebetteten photoschaltbaren Ruthenium-Sulfoxide aufgrund der äußerst geringen Beugungseffizienz von < 10−2 als nicht pragmatisch für die Praxis (s. Kapitel 4). Vergleichbare photoschaltbare Materialien, wie zum Beispiel Natriumnitrosylprussiat, erreichen hingegen Effizienzen von bis zu 100 %. Dennoch zeichnen sich die in Publikation 2 (s. Anhang A.2) vorgestellten Resultate an OSO-PDMS durch ihre äußerst hohe Qualität aus. Sowohl die dynamische Hologramm-Entstehung als auch die Rocking-Kurve folgen den physikalischen Theorien einwandfrei und lassen sich mit den bekannten mathematischen Anpassungen exakt wiedergeben, womit sich entsprechend intrinsische Größen ableiten lassen. Zudem beeindruckt der experimentelle Aufbau mit der präzisen Messung der oftmals nicht detektierbaren Nebenmaxima der gezeigten Rocking-Kurve sowie des Winkel-Multiplexings. Bemerkenswert ist außerdem aus physikalischer Sicht der immense Unterschied zwischen cw- und fs-Holographie. Hier deuten sich nichtlineare Effekte an, die zu der Erkenntnis führen, dass sich die bekannten Theorien mit cw-Lasern nicht ohne Weiteres deckungsgleich auf die Holographie mit ultrakurzen Laserpulsen anwenden lassen. Ein möglicher Erklärungsansatz ist in Kapitel 4.1 beschrieben. Einen praktischen Zweck zur Nutzung nichtlinearer Effekte erfüllt die vorgestellte Messmethode zur Unterscheidung polarer und nicht-polarer Materialien mittels intensiver fs- Puls-Anregung von sogenannten harmonischen (Upconversion-)Nanopartikeln (s. Kapitel 5). Denn anders als die zu Beginn behandelten Leuchtstoffe, weisen die harmonischen Nanopartikel eine starke Anti-Stokes Verschiebung durch Frequenzkonversion zweier oder dreier Photonen zu einem energiereicheren (kurzwelligen) Photon auf. Diese als SHG (second harmonic generation) und THG (third harmonic generation) bekannte Lichtemission wird spektral vermessen, wobei die zu Beginn der Arbeit beschriebenen linearen diffusen Reflektanzmessungen den zu erwartenden Spektralbereich ohne nennenswerte Absorption eingrenzen. Die eigens definierte Gütezahl fR, bestehend aus dem integrierten SHG- und THG-Emissionsspektrum einer Probe, kategorisiert dann die polare (fR > 1) oder nicht-polare (fR << 1) Natur des Materials.

Optics are a powerful probe of chemical structure that can often be linked to theoretical predictions, providing robustness as a measurement tool. Not only do optical interactions like second harmonic generation (SHG), single and two-photon excited fluorescence (TPEF), and infrared absorption provide chemical specificity at the molecular and macromolecular scale, but the ability to image enables mapping heterogeneous behavior across complex systems such as biological tissue. This thesis will discuss nonlinear and linear optics, leveraging theoretical predictions to provide frameworks for interpreting analytical measurement. In turn, the causal mechanistic understanding provided by these frameworks will enable structurally specific quantitative tools with a special emphasis on application in biological imaging. The thesis will begin with an introduction to 2nd order nonlinear optics and the polarization analysis thereof, covering both the Jones framework for polarization analysis and the design of experiment. Novel experimental architectures aimed at reducing 1/f noise in polarization analysis will be discussed, leveraging both rapid modulation in time through electro-optic modulators (Chapter 2), as well as fixed-optic spatial modulation approaches (Chapter 3). In addition, challenges in polarization-dependent imaging within turbid systems will be addressed with the discussion of a theoretical framework to model SHG occurring from unpolarized light (Chapter 4). The application of this framework to thick tissue imaging for analysis of collagen local structure can provide a method for characterizing changes in tissue morphology associated with some common cancers (Chapter 5). In addition to discussion of nonlinear optical phenomena, a novel mechanism for electric dipole allowed fluorescence-detected circular dichroism will be introduced (Chapter 6). Tackling challenges associated with label-free chemically specific imaging, the construction of a novel infrared hyperspectral microscope for chemical classification in complex mixtures will be presented (Chapter 7). The thesis will conclude with a discussion of the inherent disadvantages in taking the traditional paradigm of modeling and measuring chemistry separately and provide the multi-agent consensus equilibrium (MACE) framework as an alternative to the classic meet-in-the-middle approach (Chapter 8). Spanning topics from pure theoretical descriptions of light-matter interaction to full experimental work, this thesis aims to unify these two fronts. <br>

Broadband spectral content is required to support ultrashort pulses. However this broadband content is subject to dispersion and hence the pulse duration of corresponding ultrashort pulses may be stretched accordingly. I used a commercially-available adaptive ultrashort pulse shaper featuring multiphoton intrapulse interference phase scan technology to characterise and compensate for the dispersion of the optical system in situ and conducted experimental and theoretical studies in various inter-linked topics relating to the light-matter interaction. Firstly, I examined the role of broadband ultrashort pulses in novel light-matter interacting systems involving optically co-trapped particle systems in which inter-particle light scattering occurs between optically-bound particles. Secondly, I delivered dispersion-compensated broadband ultrashort pulses in a dispersive microscope system to investigate the role of pulse duration in a biological light-matter interaction involving laser-induced cell membrane permeabilisation through linear and nonlinear optical absorption. Finally, I examined some of the propagation characteristics of broadband ultrashort pulse propagation using a computer-controlled spatial light modulator. The propagation characteristics of ultrashort pulses is of paramount importance for defining the light-matter interaction in systems. The ability to control ultrashort pulse propagation by using adaptive dispersion compensation enables chirp-free ultrashort pulses to be used in experiments requiring the shortest possible pulses for a specified spectral bandwidth. Ultrashort pulsed beams may be configured to provide high peak intensities over long propagation lengths, for example, using novel beam shapes such as Bessel-type beams, which has applications in biological light-matter interactions including phototransfection based on laser-induced cell membrane permeabilisation. The need for precise positioning of the beam focus on the cell membrane becomes less strenuous by virtue of the spatial properties of the Bessel beam. Dispersion compensation can be used to control the temporal properties of ultrashort pulses thus permitting, for example, a high peak intensity to be maintained along the length of a Bessel beam, thereby reducing the pulse energy required to permeabilise the cell membrane and potentially reduce damage therein.