Neste trabalho, estudamos a fotoassociação de átomos de rubídio no regime de curto alcance. Realizamos espectroscopia por perda de átomos em uma armadilha magneto-óptica de 85Rb usando um laser de fibra de alta potência, o qual possuia largura de linha da ordem de 1MHz e 50W de potência no intervalo de 1060nm a 1070nm. Dois níveis vibracionais do potencial excitado 0u+ foram observados (v=137 e v=138). Além disso, medimos o tempo de vida de uma armadilha óptica de dipolo cruzada. Como esperado, o tempo de vida é menor quando o laser está sintonizado na ressonância. Um modelo teórico prevê a distribuição dessas moléculas nos níveis vibracionais do estado eletrônico fundamental após o processo de fotoassociação. Os resultados, nos sugerem perspectivas para a produção de moléculas de Rb2 no estado vibracional fundamental. / In this work, we studied short-range photoassociation of rubidium atoms. We realize trap-loss spectroscopy in a magneto-optical trap of 85Rb using high power fiber laser, which had around 1MHz linewidth and 50W power at 1060nm to 1070nm interval. Two vibrational levels of the 0u+ excited potential were observed (v=137 e v=138). Besides that, we measured the lifetime of a crossed optical dipole trapped. As expected, the lifetime is shorter when the laser is tuned on resonance. A theoretical model predicts the molecular distribution in the vibrational levels of electronic ground state. The results suggest us perspectives to produce Rb2 molecules in the ground vibrational state.

Armadilhamento duplo de átomos neutros constitui um dos avanços mais recentes no estudo de colisões frias. Obtivemos experimentalmente as taxas de perda devido a interação de espécies alcalinas mistas (Cs/Rb). Utilizamos uma armadilha magneto-óptica mista operando com feixes de alta intensidade permitindo o resfriamento e confinamento das amostras com sucesso. Esse trabalho apresenta-se de forma relevante pois corresponde a primeira etapa para o estudo do processo de formação de moléculas frias heteronucleares. Uma comparação entre duas técnicas de monitoramento dos processos de carga de átomos foi realizada. Os resultados tanto qualitativamente como quantitativamente foram satisfatórios. Determinamos as taxas de perda, de interesse e analisamos essas taxas considerando a proporção entre as massas dos átomos envolvidos e enfocando o efeito causado pela diferença de massa entre eles concluindo assim o objetivo principal dessa dissertação. / Double trapping of neutral atoms is one of the most recent advances in the study of collisions cold. Experimentally obtained the rates of loss due to the interaction of species alkaline mixed (Cs / Rb). We use a magneto-optical trap mixed operating with beams of high intensity allowing the cooling and containment of the samples successfully. This work is so important because it represents the first step to study the process of formation of molecules heteronucleares cold. A comparison between two techniques of monitoring procedures for cargo of atoms was performed. The results both qualitatively and quantitatively were satisfactory. And the rates of loss of interest and analyze the rates considering the ratio between the masses of atoms involved and focusing on the effect caused by the difference of mass between them thus completing the main objective of this dissertation.

Neste trabalho, descrevemos a construção de uma armadilha óptica de dipolo, tipo Quest, para átomos de Rydberg utilizando um laser de CO2 de alta potência. A amostra aprisionada apresenta aproximadamente 3 × 106 átomos de 85Rb numa densidade 4 × 1011 átomos/cm3, em temperaturas da ordem 30 µK. O tempo de vida da armadilha é da ordem de 200 ms. Neste sistema, observamos a fotoionização dos estados de Rydberg devido ao laser de CO2 em 10, 6 µm, contudo fomos incapazes de quantificá-lo. Além disso, medimos o tempo de vida do estado 37D do Rb na armadilha de dipolo, o resultado foi compatível ao encontrado na literatura. Em suma, o sistema esta operante para experimentos mais complexos. / In this work, we describe the implementation of a QUEST dipole trap for Rydberg atoms using a CO2 high power laser. The trapped atomic sample has approximately 3 × 106 85Rb atoms, at a density of 4 × 1011 atoms/cm3 and a temperature of about 30 µK. The trap lifetime is about 200 ms. We observed photoionization of the Rydberg states due to the CO2 laser at 10, 6 µK, however we were unable to quantify it. Furthermore, we measured the 37D state lifetime of the Rb in the dipole trap, the experimental result was in agreement with the literature. In summary, the system is fully operating for more complex experiments.

No presente trabalho, estudamos o comportamento de um Condensado de Bose-Einstein contendo um vórtice tipo linha aprisionado, e durante o vôo livre. Desta maneira foi feito a analise da velocidade de expansão do aspect ratio da nuvem para três formatos de armadilhas, as quais são potenciais harmônicos sem rotação, incluindo a comparação entre a velocidade de expansão do raio da nuvem e do núcleo do vórtice. Vimos que a precessão do vórtice pode independer de um potencial com rotação, sendo diretamente relacionada com a densidade da nuvem atômica. Ao supor um Condensado com um vórtice não-fundamental e estável obtemos uma possível descrição do aspect ratio da nuvem, como uma aproximação para uma rede de vórtices; utilizando apenas de um método semi-analítico. / In this work, we have studied the behavior of a Bose-Einstein Condensate contend a line vortex at trap, and while the free flight. In this way it was analysed the expansion speed of clouds aspect ratio into three kind of traps, which are non-rotating harmonic potentials, including the comparation between velocity of the radius and the vortex core under expansion. We have seem the vortexs precession may be independent of a rotating potential, thus it is directly associated with the density profile of atomic cloud. By assuming a Condensate within a stable non-funtamental vortex we obtain a possible description of aspect ratio of cloud, like an approach for a lattice vortex; using only a semi-analytic method.

Neste trabalho apresentamos a construção de um novo sistema experimental para aprisionamento de átomos e moléculas. Trata-se de uma armadilha de dipolo cruzada totalmente óptica, formada por um laser de fibra com 40 W de potência com comprimento de onda em 1064 nm. Nesse sistema foi demonstrado o aprisionamento de átomos Rb e K e moléculas Rb2. Realizamos dois experimentos distintos neste se novo sistema: No primeiro, estudamos a evolução temporal de amostras dos isótopos 85Rb e 87Rb na armadilha de dipolo cruzada. Pudemos medir pela primeira vez o processo de mudança de estrutura hiperfina em átomos sem a presença de luz ressonante, e observamos a fotoassociação dos átomos pelo laser da armadilha de dipolo. E no segundo, desenvolvemos uma técnica que permite o estudo rápido e direto do decaimento no número de moléculas de Rb2 na armadilha. Com essa técnica, observamos também o comportamento dessas moléculas na presença de átomos preparados em um determinado estado hiperfino do estado fundamental. Estes resultados juntamente com um desenvolvimento teórico, nos sugerem novas perspectivas rumo a produção de um sistema que possa produzir e aprisionar moléculas KRb no estado fundamental 1Σ+ (v = 0). / In this work, we present the construction of a new experimental system for trapping atoms and molecules. It is an all optical crossed dipole trap, formed by a fiber laser with 40 W of power at 1064 nm. In this system, we have trapped K and Rb atoms as well as Rb2 molecules. We have carried out two experiments in this new system. In the first, we studied the temporal evolution of atomic samples of different isotopes, 85Rb and 87Rb, in the crossed trap dipole. We were able to measure for the first time the hyperfine-changing collisions of atoms in the absence of resonant light, and we have observed photoassociation of atoms by the dipole trap laser beam. In the other experiment, we have developed a technique that allows us to study the trapped molecule population decay in the trap. It was also observed the molecule population decay in the presence of atoms prepared in a given hyperfine state of the ground state. These results together with a theoretical development may suggest us new perspectives towards the production of a system that can produce and trap KRb molecules in the ground state 1Σ+ (v = 0).

Dans les systèmes quantiques unidimensionnels, le rôle des fluctuations et des interactions est plus important et les théories utilisées à plus haute dimension ne peuvent plus être employées. Le point de départ pour décrire la plupart des systèmes unidimensionnels est la théorie du liquide de Luttinger. Bien que cette théorie décrive de nombreux phénomènes avec succès, elle a aussi ses limites. Par exemple, elle ne peut décrire que la limite de basse énergie d'un system unidimensionnel, elle échoue aussi lorsqu'il s'agit de décrire la désintégration des excitations du système. Dans cette thèse, nous étudions principalement deux types de problème en une dimension. Le premier est l'interaction effective entre des impuretés dans un liquide de bosons tandis que le deuxième est la désintégrations des quasi-particules dans un mélange bosons-fermions. Dans les deux cas, décrire le système comme un liquide de Luttinger n'est pas suffisant. Afin de pallier à cela, nous développons plusieurs approches pour ces systèmes unidimensionnels qui prennent en compte les différentes anharmonicités nécessaires afin de capturer les mécanismes importants en jeu dans ces problèmes. / In one-dimensional quantum systems, the role of fluctuations and interactions is enhanced and theories used in higher- dimensional systems cannot be employed anymore to describe such strongly-correlated systems. The starting point to describe most one-dimensional systems is the Luttinger liquid theory. Even though this theory is successful to describe many phenomena, it has its shortcomings. For example, it can only treat the low-energy limit of one-dimensional systems and fails to describe the decay of excitations. In this thesis, we mainly study two kinds of problems in one dimension. The first one is the effective interaction between impurities in a Bose liquid whereas the second one is the decay of quasiparticles in a Bose-Fermi mixture. In both cases, the description of the system in terms of a Luttinger liquid is not sufficient. To overcome this, we develop different approaches for these one-dimensional systems to account for the various anharmonicities which are necessary to capture the relevant physics of these problems.

Depuis quelques temps, les physiciens théoriciens de la matière condensée sont confrontés à un problème majeur : la puissance de calcul nécessaire pour simuler numériquement et étudier certains systèmes à N corps est insuffisante. Comme le contrôle et l’utilisation des systèmes d’atomes ultra-froids se sont développés de manière importante,principalement durant les deux dernières décennies, nous sommes peut-être en mesure d eproposer une solution alternative : utiliser des atomes ultra-froids piégés dans des réseaux optiques en tant que simulateur quantique. En effet, la physique des électrons se déplaçant sur la structure cristalline d’un solide, ainsi que celle des atomes piégés dans des réseaux optiques, sont toutes les deux décrites par le même modèle de Fermi-Hubbard, qui est une présentation simplifiée du comportement des fermions sur un réseau périodique. Les simulateurs quantiques peuvent donc simuler des propriétés électriques des matériaux, telle sque la conductivité ou le comportement isolant, et potentiellement aussi des propriété smagnétiques telles que l’ordre antiferromagnétique.L’expérience AUFRONS, sur laquelle j’ai travaillé pendant mon doctorat, a pour but d’étudie rla physique des fermions fortement corrélés, avec un simulateur quantique basé sur l’utilisation d’atomes ultra-froids de rubidium 87 et de potassium 40, piégés dans le potentiel nanostructuré des réseaux optiques bidimensionnels, générés en champ proche. Pour détecter la distribution atomique à d’aussi courtes distances, nous avons développé une technique d’imagerie novatrice, qui nous permettra de contourner la limite de diffraction. Une fois terminé, notre système d’imagerie pourrait potentiellement détecter et identifier des sites individuels du réseau optique sub-longueur d’onde.Dans ce manuscrit, je décris le travail que j’ai effectué pour construire l’expérience AUFRONS,ainsi que l’étude de faisabilité que j’ai réalisée pour la technique d’imagerie à super-résolution. / For some time now, theoretical physicists in condensed matter face a majorproblem: the computing power needed to numerically simulate and study some interactingmany-body systems is insufficient. As the control and use of ultracold atomic systems hasexperimented a significant development in recent years, an alternative to this problem is to usecold atoms trapped in optical lattices as a quantum simulator. Indeed, the physics of electronsmoving on a crystalline structure of a solid, and the one of trapped atoms in optical lattices areboth described by the same model, the Fermi-Hubbard model, which is a simplifiedrepresentation of fermions moving on a periodic lattice. The quantum simulators can thusreproduce the electrical properties of materials such as conductivity or insulating behavior, andpotentially also the magnetic ones such as antiferromagnetism.The AUFRONS experiment, in which I worked during my PhD, aims at building a quantumsimulator based on cooled atoms of 87Rb and 40K trapped in near field nanostructured opticalpotentials. In order to detect the atom distribution at such small distances, we have developedan innovative imaging technique for getting around the diffraction limit. This imaging systemcould potentially allow us to detect single-site trapped atoms in a sub-wavelength lattice.In this thesis, I introduce the work I have done for building the AUFRONS experiment, as wellas the feasability study that I did for the super-resolution imaging technique.

Cette thèse de doctorat en co-tutelle a été centrée sur des expériences d’optique quantique faisant intervenir de grands ensembles atomiques. L’étude de l’interaction entre la lumière et la matière et l’augmentation de leur couplage dans ces systèmes sont des étapes fondamentales pour le développement et l’amélioration de protocoles de génération, de stockage et de manipulation d’information quantique. Le travail de thèse exposé ici traite en particulier de l’évolution des techniques de préparation d’ensembles atomiques denses, des protocoles de lumière arrêtée et de lumière stationnaire développés et étudiés expérimentalement. Les ensembles d’atomes froids préparés par refroidissement laser dans les deux réalisations expérimentales ont été portés jusqu’à des épaisseurs optiques de plusieurs centaines, à des températures d’une dizaine de microkelvin. De plus, l’adressage de ces ensembles dans des configurations symétriques ont permis l’étude de protocoles basés sur le renversement temporel de la conversion de lumière en excitations atomiques collectives. Ces améliorations ont mené au stockage de bits quantiques par transparence induite électromagnétiquement, et de lumière cohérente par symétrie temporelle dans une mémoire Raman, tous deux à des record d’efficacité, à de plus de 50%. Ce travail a également conduit à l’étude expérimentale de la lumière stationnaire et de nouveaux protocoles en découlant. / This cotutelle PhD thesis revolves around quantum optics experiments which involve large atomic ensembles. The study of light-matter interaction and its enhancement are crucial steps in the development and progress of quantum information generation, storage and processing protocols. The work presented here focuses on the evolution of large atomic ensemble preparation techniques, on the development and experimental investigation of stopped and stationary light protocols. Laser-cooled atomic ensembles in both experimental realisations have been brought to optical depths of a few hundreds, at temperatures of tens of microkelvin. Moreover, addressing these ensembles in symmetric configurations has enabled the study of protocols based on the temporal reversal of the mapping of light to collective atomic excitations. These enhancements have led to the storage of qubits based on electromagnetically-induced transparency, and the optical storage in a backward-retrieval Raman scheme, both demonstrating efficiency records, above 50%. This work has also led to the experimental investigation of stationary light and new protocols based on it.

This dissertation presents the implementation of a technique to generate atomic Fock states of Lithium 6 with ultra-high fidelity, called laser culling. Fock states, atomic states with a definite number of particles, are a mandatory step for studying few-body quantum phenomena such as quantum tunneling, quantum entanglement, and serve as building blocks for quantum simulators. The creation of ultra-high fidelity Fock states begins with a degenerate Fermi gas in an optical dipole trap. Being fermions, lithium-6 atoms fill the energy levels of the dipole trap with 2 atoms per energy level. Introducing a magnetic field gradient creates a linear potential that tilts the potential produced by the optical dipole trap. The initially bound energy levels become quasi-bound states, each with a different lifetime. By exploiting the difference between these lifetimes, one can generate a single pair of atoms in the ground state of the trap with fidelities that can exceed 99.9%. This dissertation first presents the details of the design and construction of an apparatus for laser culling, and then reports on the progress made towards the creation of atomic Fock states with ultra-high fidelity. / text

In this thesis we study the physics of quantum many-body systems confined to one-dimensional geometries. The work was motivated by the recent success of experimentalists in developing atom traps, capable of restricting the motion of the individual atoms to a single spatial dimension. Specifically, we look at aspects of the one-dimensional Bose gas including; excitation spectrum, correlation functions, and dynamical behaviour. In Chapter \ref{ch:excitation1D} we consider the Lieb-Liniger model of interacting bosons in one-dimension. We numerically solve the equations arising from the Bethe ansatz solution for the exact many-body wave function in a finite-size system of up to twenty particles for attractive interactions. We discuss novel features of the solutions, including deviations from the well-known string solutions due to finite size effects. We present excited state string solutions in the limit of strong interactions and discuss their physical interpretation, as well as the characteristics of the quantum phase transition that occurs as a function of interaction strength in the mean-field limit. Our results are compared to those obtained via exact diagonalization of the Hamiltonian in a truncated basis. In Chapter \ref{ch:g2} we analytically calculate the spatial nonlocal pair correlation function for an interacting uniform one dimensional Bose gas at finite temperature and propose an experimental method to measure nonlocal correlations. Our results span six different physical realms, including the weakly and strongly interacting regimes. We show explicitly that the characteristic correlation lengths are given by one of four length scales: the thermal de Broglie wavelength, the mean interparticle separation, the healing length, or the phase coherence length. In all regimes, we identify the profound role of interactions and find that under certain conditions the pair correlation may develop a global maximum at a finite interparticle separation due to the competition between repulsive interactions and thermal effects. In Chapter \ref{ch:casimirdrag} we study the drag force below the critical velocity for obstacles moving in a superfluid. The absence of drag is well established in the context of the mean-field Gross-Pitaevskii theory. We calculate the next order correction due to quantum and thermal fluctuations and find a non-zero force acting on a delta-function impurity moving through a quasi-one-dimensional Bose-Einstein condensate at all subcritical velocities and at all temperatures. The force occurs due to an imbalance in the Doppler shifts of reflected quantum fluctuations from either side of the impurity. Our calculation is based on a consistent extension of Bogoliubov theory to second order in the interaction strength, and finds new analytic solutions to the Bogoliubov-de Gennes equations for a gray soliton. In Chapter \ref{ch:solitons} we study the effect of quantum noise on the stability of a soliton. We find the soliton solutions exactly define the reflectionless potentials of the Bogoliubov-de Gennes equations. This results in complete stability of the solitons in a purely one dimensional system. We look at the modifications to the density profile of a black soliton due to quantum fluctuations.