Thermal and quantum fluctuations of the electromagnetic near field of atoms and macroscopic bodies play a key role in quantum electrodynamics (QED), as in the Lamb shift. They lead, e.g., to atomic level shifts, dispersion interactions (Van der Waals-Casimir-Polder interactions), and state broadening (Purcell effect) because the field is subject to boundary conditions. Such effects can be observed with high precision on the mesoscopic scale which can be accessed in micro-electro-mechanical systems (MEMS) and solid-state-based magnetic microtraps for cold atoms (‘atom chips’). A quantum field theory of atoms (molecules) and photons is adapted to nonequilibrium situations. Atoms and photons are described as fully quantized while macroscopic bodies can be included in terms of classical reflection amplitudes, similar to the scattering approach of cavity QED. The formalism is applied to the study of nonequilibrium two-body potentials. We then investigate the impact of the material properties of metals on the electromagnetic surface noise, with applications to atomic trapping in atom-chip setups and quantum computing, and on the magnetic dipole contribution to the Van der Waals-Casimir-Polder potential in and out of thermal equilibrium. In both cases, the particular properties of superconductors are of high interest. Surface-mode contributions, which dominate the near-field fluctuations, are discussed in the context of the (partial) dynamic atomic dressing after a rapid change of a system parameter and in the Casimir interaction between two conducting plates, where nonequilibrium configurations can give rise to repulsion. / Thermische und Quantenfluktuationen des elektromagnetischen Nahfelds von Atomen und makroskopischen Körpern spielen eine Schlüsselrolle in der Quantenelektrodynamik (QED), wie etwa beim Lamb-Shift. Sie führen z.B. zur Verschiebung atomarer Energieniveaus, Dispersionswechselwirkungen (Van der Waals-Casimir-Polder-Wechselwirkungen) und Zustandsverbreiterungen (Purcell-Effekt), da das Feld Randbedingungen unterliegt. Mikroelektromechanische Systeme (MEMS) und festkörperbasierte magnetische Fallen für kalte Atome (‘Atom-Chips’) ermöglichen den Zugang zu mesoskopischen Skalen, auf denen solche Effekte mit hoher Genauigkeit beobachtet werden können. Eine Quantenfeldtheorie für Atome (Moleküle) und Photonen wird an Nichtgleichgewichtssituationen angepasst. Atome und Photonen werden durch vollständig quantisierte Felder beschrieben, während die Beschreibung makroskopischer Körper, ähnlich wie im Streuformalismus (scattering approach) der Resonator-QED, durch klassische Streuamplituden erfolgt. In diesem Formalismus wird das Nichtgleich- gewichts-Zweiteilchenpotential diskutiert. Anschließend wird der Einfluss der Materialeigenschaften von normalen Metallen auf das elektromagnetische Oberflächenrauschen, das für magnetische Fallen für kalte Atome auf Atom-Chips und für Quantencomputer-Anwendungen von Bedeutung ist, sowie auf den Beitrag des magnetischen Dipolmoments zum Van der Waals-Casimir-Polder-Potential im thermisch- en Gleichgewicht und in Nichtgleichgewichtssituationen untersucht. In beiden Fällen sind die speziellen Eigenschaften von Supraleitern von besonderem Interesse. Beiträge von Oberflächenmoden, die die Feldfluktuationen im Nahfeld dominieren, werden im Kontext des (partiellen) dynamischen Dressing nach einer raschen Änderung eines Systemparameters sowie für die Casimir-Wechselwirkung zweier metallischer Platten diskutiert, zwischen denen in Nichtgleichgewichtssituationen Abstoßung auftreten kann.

Made available in DSpace on 2015-05-14T12:14:08Z (GMT). No. of bitstreams: 1 arquivototal.pdf: 2614177 bytes, checksum: 64cd8eee6f69230497da81e691be96a2 (MD5) Previous issue date: 2005-11-24 / Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - CAPES / Interactions with surfaces modify internal and external liberty degrees of atoms next to these surfaces. The dominant long range interaction (which extends itselfs to about an atomic transition wavelength is the van der Waals interaction, usually attractive. Firstly, this thesis treats C3 coefficient, which is characteristic of this interaction and depends on the type of surface and temperature. Other theme is determination of this coefficient using a spectroscopic technique (Selective Reflection) in the atomic cesium system (6S1=2 - 8P3=2 transition) on a dielectric surface. This interaction allows the long range excitation transfer (Förster effect) from atom to the dispersive dielectric surface. Considering small distances (atomic dimensions), interaction becomes repulsive because of electronic orbital overlap between the atom and surface components. The sum of these two kinds of interaction (far and close range) results in a potential well, with discrete energy levels. Next, are presented results of simulations on optic transfer from free atoms to atom-surface bounded states. The radiation sources used on the experiments to evidence atom-surface effects described in the first part of this thesis are resonant diode lasers, with spectral characteristics that must be modified on the laboratory to became useful tools to perform high resolution experiments. The Part II treats diode lasers, beginning from stabilization techniques description and going to a new technique developed on the laboratory during doctoral work, where the laser frequency is controlled by an coupled optical orthogonal feedback with atomic transition to diode. Other effects related to this stabilization technique, as the bi-stability phenomena, are described and interpreted on the last chapter. / Interações dos átomos com superfícies modificam os graus de liberdade internos e externos desses átomos quando próximos a elas. A interação dominante de longo alcance (até a ordem do comprimento de onda das transições atômicas) é a interação de van derWaals, geralmente atrativa. Nesta tese é abordado o coeficiente C3, característico dessa interação e dependente da superfície e temperatura, determinado através do uso de uma técnica espectroscópica (Reflexão Seletiva). Trata-se também da transferência de excitação de longo alcance (efeito Förster) do átomo para a superfície. A curtas distâncias (dimensões atômicas), a interação torna-se repulsiva, devido à sobreposição dos orbitais eletrônicos do átomo incidente e dos constituintes da superfície. A soma das contribuições de curto e de longo alcance resulta em um poço de potencial com níveis discretos de energia que são simulados em uma transferência ótica para esses estados ligados. As fontes de radiação utilizadas nas experiências da primeira parte desta tese são lasers de diodo ressonantes, cujas características espectrais precisam ser modificadas no laboratório para eles se tornarem ferramentas adequadas para a realização de tais experiências de espectroscopia de alta resolução. A Parte II da tese trata de diodos lasers, iniciando com a descrição de técnicas de estabilização e chegando a uma nova técnica desenvolvida no laboratório durante este trabalho de doutorado, onde a freqüência do laser é controlada através de um retorno ótico com polarização ortogonal no diodo acoplado à transição atômica. Outros efeitos relacionados a essa técnica de estabilização, como o fenômeno de bi-estabilidade, são descritos e interpretados no último capítulo desta tese.

Les vapeurs atomiques confinées dans des cellules nanométriques constituent une plateforme intéressante pour la réalisation de senseurs atomiques. Dans cette thèse, nous étudions l’interaction entre la lumière et un ensemble d’atomes d’alcalins dans une telle cellule. Nous nous concentrons sur les phénomènes qui pourraient modifier la réponse optique du système et ainsi affecter la sensibilité du senseur. Premièrement, nous étudions la réponse non locale à la lumière induite par le mouvement des atomes dans la vapeur thermique. Quand la distance de relaxation des atomes excède la taille de la cellule, la réponse optique dépend de la taille du système. En transmission, nous avons montré que cela entraine une modification des propriétés de la vapeur avec une période égale à la longueur d’onde de la transition optique. Nous avons ensuite montré que lorsque la densité augmente, la réponse redevient locale. De plus, dans ce régime dense, l’interaction dipôle-dipôle résonnante engendre des déplacements de fréquences collectifs pour des ensembles sub-longueur d’onde. Nous avons démontré que ces shifts sont induits par la cavité formée par la cellule, clarifiant ainsi un débat de plus de 40 ans. Pour ce faire, nous avons développé un modèle pour extraire les effets de la densité déconvolués de ceux de la cavité. Proche des surfaces, la réponse optique des atomes est aussi impactée par l’interaction de van der Waals. Nous avons introduit une nouvelle méthode pour extraire avec précision la force de cette interaction. Nous avons également construit une nouvelle génération de nano-cellules super-polies en verre et enfin comparé les propriétés spectrales en transmission et spectroscopie hors d’axe. / Alkali vapors confined in nano-scale cells are promising tools for future integrated atom-based sensor. In this thesis, we investigate the interaction between light and an ensemble of atoms confined in a nano-geometry. We focus on the different processes that can modify the optical response of the atomic ensemble and possibly affect the sensitivity of a sensor based on that technology. First, we study the non-local response of atoms to a light excitation due the atomic motion in thermal vapors. When the distance over which the atoms relaxes is larger than the size of the cell, the optical response depends on the size of the system. We have observed that for transmission spectroscopy, this leads to a periodic modification of the optical response with a period equal to the wavelength of the optical transition. Subsequently we showed that when the density of atom increases, the atomic response becomes local again. In this dense regime, the resonant dipole-dipole interaction in a sub-wavelength geometry leads to collective frequency shifts of the spectral lines. We demonstrate that these shifts were induced by the cavity formed by the cell walls, hence clarifying a long-standing issue. We developed a model to extract the density shifts deconvolved from the cavity effects. Close to a surface, the optical response is also affected by the van der Waals atom-surface interaction. We introduced a new method to extract precisely the strength of this interaction. We also developed a new generation of super-polished glass nano-cells and we presented promising spectroscopic signals. Finally, using these cells, we have compared transmission and off-axis spectroscopic techniques.