Dissertations / Theses on the topic 'Two Bose-Einstein condensates'

This thesis reports the experimental study of two-component Bose-Einstein condensates with tunable interactions, which are exploited as a platform to perform quantum simulation of many-body quantum systems. To perform this experiments, we have implemented an atomic source consisting on a glass cell 2D MOT vacuum chamber and a high resolution optical system to image and manipulate the atoms. Furthermore, we develop and characterize a polarization phase contrast technique which is able to probe optically dense atomic mixtures at intermediate and high magnetic fields in open transitions. This technique has been used to either probe the total column density of a two-component atomic cloud or the difference in column density between both components. We report on the first observation of composite quantum liquid droplets in an incoherent mixture with residual mean field attraction. Strikingly, this novel phase is stabilized due to the repulsive beyond mean field corrections in a weakly interacting system. Moreover, we have characterized the liquid to gas phase transition which occurs for small atom numbers. Additionally, we have compared two different self-bound states in a quasi-1D geometry with incoherent mixtures: quantum droplets and bright solitons. Depending on the atom number and interaction strengths both states can be smoothly connected through a crossover or be distinct entities separated by a transition. We have measured its composition, its phase diagram and mapped out the soliton to droplet transition. Finally, we report on a technique to modify the elastic and inelastic interactions in a two-component Bose-Einstein condensate with very unequal and competing interactions under the presence of strong coherent coupling. This technique provides a wide flexibility and has allowed us to observe bright solitons in quasi-1D in a coherently coupled dressed state. We exploit the fast temporal control of the effective interactions to quench them into the attractive regime and study the resulting modulational instability which develops into a bright soliton train.
Aquesta tesi descriu l'estudi experimental d'una mescla de dos condensats de Bose-Einstein amb interaccions ajustables. Aquest sistema és utilitzat com una plataforma per a estudiar sistemes quàntics formats per moltes partícules a partir de la simulació quàntica. Per a fer aquests experiments, he construït una font atòmica formada per una trampa magneto-òptica en 2D que s'implementa en una cambra de buit feta de vidre. A més a més, he desenvolupat i caracteritzat una tècnica d'imatge de contrast de fase basada en la rotació de la polarització de la llum. Aquesta tècnica està preparada per fer imatges de mescles atòmiques a camps magnètics intermedis i alts amb una gran densitat òptica i amb transicions òptiques obertes. Hem utilitzat la tècnica per a mesurar la densitat integrada total en l'eix òptic així com la diferència entre ambdues components. Es descriu la primera observació de gotes líquides quàntiques compostes per dues components incoherents amb una atracció residual en l'aproximació de camp mitjà. Sorprenentment, aquesta nova fase està estabilitzada a causa de la repulsió generada per les correccions de l'energia més enllà de l'aproximació de camp mitjà en un sistema amb interaccions dèbils. També hem caracteritzat la transició de fase líquid-gas que succeeix quan el sistema té un nombre d'àtoms reduït. A més a més, hem comparat dos estats autoconfinats de diferent natura en una geometria quasi-1D amb una mescla d'àtoms incoherents: les gotes quàntiques i els solitons brillants. Segons el nombre d'àtoms i la força de les interaccions aquests estats poden estar connectats o bé suaument o bé per una transició de fase. Hem mesurat la seva composició, el diagrama de fases i hem traçat el mapa de transició entre solitons i gotes en funció del camp magnètic i nombre d'àtoms. Finalment, es descriu una tècnica per a modificar les interaccions elàstiques i inelàstiques en un condensat de Bose-Einstein format per dues components, amb interaccions diferents i en competició, coherentment acoblades. Aquesta tècnica ens proveeix d'una gran flexibilitat per a modificar les interaccions i ens ha permès observar solitons brillants en quasi-1D en un estat vestit per l'acoblament coherent. Hem utilitzat l'habilitat per a modificar temporalment les interaccions per a canviar-les bruscament cap al règim atractiu i estudiar la inestabilitat dels modes que es manifesta amb la formació d'un tren de solitons brillants.

We examine the energy cascades and quantum vortex structures in two-dimensional quantum turbulence through a special unitary time evolution algorithm. An early attempt at using the Lattice Boltzmann Method proved successful in correctly representing some features of the Nonlinear Schrodinger System (NLS), such as the phase shift following the one-dimensional soliton-soliton collision, as well as the two-dimentional modulation instability. However, to accurately evaluate NLS, the implicit Euler method is required to resolve the time evolution, which is computationally expensive. A more accurate and efficient method, the Quantum Lattice Gas model is employed to simulate the quantum turbulence governed by the Gross-Pitaevskii equation, an equaiton that describes the evolution of the ground state wave function for a Bose-Einstein condensate (BEC). It is discovered that when the ratio of the internal energy to the kinetic energy is below 0.05, an unexpected short Poincare recurrence occurs independent of the initial profile of the wave function. It is demonstrated that this short recurrence is destroyed as the internal energy is strengthened. to compare the two-dimensional quantum turbulence with its classical counterpart, the incompressible energy spectra of quantum turbulence is analyzed. However, the result reveals no sign of dual cascades which is a hallmark of the classical incompressible two-dimensional fluid (inverse energy cascade to large scales with a direct cascade of enstrophy to small scales). It is the spectra of the compressible energy that can exhibits multiple cascades, but this is strongly dependent on the initial condition.

Bose-Einstein condensates (BECs) of ultra-cold atoms have been subjects of a large research effort, that started a century ago as a purely theoretical subject and is now, since the invention of evaporative cooling thirty years ago, a rich research topic with many experimental apparatuses around the world. A deep knowledge of its underlying physics has been now acquired, for example on the thermodynamics of the gas, superfluidity, topological excitations and many-body physics. However, many topics are still open for investigation, thanks to the flexibility and the high degree of control of these systems. During the course of my PhD, I developed and realized a new experimental apparatus for the realization of coherently-coupled mixtures of sodium BECs. The highly stable and low-noise magnetic environment of this apparatus enables the experimental investigation of a previously inaccessible regime, where the energy of the coupling becomes comparable to the energy of spin excitations of the mixture. With this apparatus, I concluded two experimental investigations: I produced and investigated non-dispersive spin-waves in an two-component BEC and I experimentally observed the quantum spin-torque effect on a elongated bosonic Josephson junction.The research activity in multi-component BECs of alkali atoms begun shortly after the first realization of a condensate, thanks to the low energy splitting between the internal sub-states of the electronic ground state. These internal states can be coherently coupled with an external electromagnetic field and can interact via mutual mean-field interaction, generating interestinc effects such as ground states with different magnetic ordering depending on their interaction constants, density as well as spin dynamics and internal Josephson effects. The research interest on mixtures of sodium atoms sparks from the peculiar characteristic of the system: in the $ket{F = 1, m_F = pm 1}$ states, the interaction constants are such that the ground state has anti-ferromagnetic ordering and the system is perfectly symmetric for exchanges of the two species. In these peculiar system, density- and spin-excitations have very different energetic cost, with the latter being much less energetic, and can be completely decoupled. Moreover, spin-excitations, that are connected to excitations in the relative-phase between the components, change drastically in nature when a coupling of comparable energy is added between the states. The presence of the coupling effectively locks the relative-phase in the bulk and spin excitations become localized. While extensive theoretical predictions on the spin dynamics of this system has been already performed, experimental confirmation was still lacking because of the high sensitivity to external forces (due to the very low energy of the spin excitations) and the impossibility of realizing a low-energy coupling between these states in the presence of environmental magnetic noise. During my PhD, I realized an experimental apparatus where magnetic noises are suppressed by five orders of magnitude using a multi-layer magnetic shield made of an high-permeability metal alloy (μ-metal), that encases the science chamber. In this apparatus, I developed a protocol, compatible with the technical limitations of the magnetic shield, to produce BECs in a spin-insensitive optical trapping potential. I then characterized the residual magnetic noise and found it compatible with the requirements for observing spin-dynamics effects. Finally, I realized a system and a set of protocols for the manipulation of the internal state of the sample allowing arbitrary preparation of the sample while maintaining the long coherence times necessary to observe the spin dynamics, that have been used in the subsequent experimental observations. The first experimental result discussed in this thesis, is the production of magnetic solitons and the observation of their dynamic in a trapped sample. Waves in general spread during their propagation in a medium, however this tendency can be counterbalanced by a self-focusing effect if dispersion of the wave is non-linear, generating non-dispersive and long-lived wavepackets commonly named solitons. These have been found in many fields of physics, such as fluid dynamics, plasma physics, non-linear optics and cold-atoms BECs, attracting interest because of their ability to transport information or energy unaltered over long distances, as they are robust against the interaction with in-homogeneities in the medium. Of these systems, cold-atoms can be widely manipulated to generated different kinds of solitons, both in single and in multi-components systems. A new kind of them, named magnetic solitons, has been predicted in a balanced mixture of BECs of sodium in $ket{F = 1, m_F = pm 1}$, however experimental observation was still lacking. I deterministically produced magnetic solitons via phase engineering of the condensate using a spin-sensitive optical potential. I then developed a tomographic imaging technique to semi-concurrently measure the densities of both components and the discontinuities in their relative phase, allowing for the reconstruction of all the relevant quantities of the spinor wavefunction. This allowed to observe the dispersionless dynamics of the solitons as they perform multiple oscillation in the trapped sample in a timescale of the order of the second. Moreover, I engineered collisions between different kinds of magnetic solitons and observed their robustness to mutual interaction. The second experimental results presented in this thesis is the observation of the breaking of magnetic hetero-structures in BECs due to the quantum spin torque effect, an effect with strong analogies with electronic spins traveling through magnetic devices. Spins in magnetic material precess around the axis of the effective magnetic field, and their dynamics must take into account the external field as well as non-linear magnetization and the inhomogeneity of the material. These effects are commonly described by the Landau-Lifshitz equation and have been mainly studied for electronic spins in magnetic hetero-structures, where the inhomogeneity in the material at the interfaces enhances the exchange effects between spins. For homogeneous materials, this description reduces to the Josephson system, a closely related effect that is more known in cold-atoms systems. The Josephson effect arises when a macroscopic number of interacting bosonic particles are distributed in two possible states, weakly tunnel-coupled together, with the average energy of particles occupying each of the states depending on the occupation number itself. In these conditions, the dynamics of the system depends on the difference in occupation numbers, the relative phase between the states and the self-interaction to tunneling ratio, giving raise to macroscopic quantum effects such as oscillating AC and DC Josephson currents and self-trapping. While these phenomena has been historically studied in junctions between superconducting systems, they can be also realized with cold-atoms systems, allowing the study of Josephson junctions with finite dimensions and in regimes that are hard to reach for superconducting systems. In this thesis, I realized a magnetic hetero-structure in a two-component elongated BECs thanks to the simultaneous presence of self-trapped (ferromagnetic) and oscillating (paramagnetic) regions in the sample. While the dynamics at short times is correctly described by the Josephson effects, at the interface between the regions the particle nature of the gas creates a strong exchange effect, named the quantum spin torque, that produces magnetic excitations that spread trough the sample and break the local Josephson behaviour. I experimentally studied the spread and nature of these magnetic excitations, while numerical simulations confirmed the dominant role played by the quantum spin torque effect. The structure of this thesis is the following: in the first chapter is given a review of theoretical concepts and existing literature. In the second chapter is described the experimental apparatus and the protocols developed to prepare the ultra-cold atoms sample. In the third chapter is presented the experimental observation of magnetic solitons. In the fourth chapter is presented the experimental investigation of the quantum spin torque effect in magnetic heterostructures. The last chapter is devoted to conclusions and outlook of this work.

In this Thesis we study steady state solutions and dynamical evolutions of two– component atomic Bose–Einstein Condensates. We initially investigate the equilibrium properties of condensate mixtures in harmonic trapping potentials at zero temperature. Subsequently we simulate the coupled growth of these condensates by inclusion of damping terms. Finally, we investigate the evolution of coupled Bose gases via the so-called classical–field method. A recent experiment [D. J. McCarron et al., Phys. Rev. A, 84, 011603(R) (2011)] achieved Bose–Einstein Condensation of a two–species 87Rb–133Cs phase segregated mixture in harmonic trapping potentials. Depending on relative atom numbers of the two species, three distinct regimes of density distributions were observed. For these experimental parameters, we investigate the corresponding time–independent ground state solutions through numerical simulations of the coupled Gross–Pitaevskii equations. By including experimentally relevant shifts between the traps, we observe a range of structures including ‘ball and shell’ formations and axially/radially separated states. These are found to be very sensitive to the trap shifts. For all three experimental regimes, our numerical simulations reveal good qualitative agreement. The observed experimental profiles cannot be guaranteed to be fully equilibrated. This, coupled with the rapid sympathetic cooling of the experimental system, leads to a situation where growth may play a determining factor in the density structures formed. To investigate this further, we introduce phenomenological damping to describe the associated condensate growth/decay, revealing a range of transient structures. However, such a model always predicts the predominance of one condensate species over longer evolution times. Work undertaken by collaborators with the more elaborate Stochastic Projected Gross–Pitaevskii equations, which can describe condensate formation by coupling to a heat bath, predicts the spontaneous formation of dark–bright solitons. Motivated by this, we show how the presence of solitons can affect the condensate distribution, thus highlighting the overall dynamical role in the emerging patterns. Finally, we use classical field methods to analyse the evolution of non trapped Bose gases from strongly nonequilibrium initial distributions. The contrast between miscible (overlapping) and immiscible (phase segregated) components gives rise to important distinctions for condensate fractions and the formation of domains and vortices. In addition, splitting the particles of a single component thermalised state into two components is investigated. We then study the effects of suddenly quenching the strength of the interspecies interactions. Under suitable conditions, this quench generates isotropic vortex tangles. While this tangle subsequently decays over time, we propose how a repeat sequence of quenches at regular intervals could be employed to drive the tangle, thereby potentially providing a novel route to the generation of quantum turbulence.

Bose-Einstein condensates (BECs), with their superfluid behavior, quantized vortices, and high-level of control over trap geometry and other system parameters provide a compelling environment for studies of quantum fluid dynamics. Recently there has been an influx of theoretical and numerical progress in understanding the superfluid dynamics associated with two-dimensional quantum turbulence, with expectations that complementary experiments will soon be realized. In this dissertation I present progress in the development of an experimental toolkit that will enable such experimental studies of two-dimensional quantum turbulence. My approach to developing this toolkit has been twofold: first, efforts aimed at the development of experimental techniques for generating large disordered vortex distributions within a BEC; and second, efforts directed towards the design, implementation, and characterization of a quantum vortex microscope. Quantum turbulence in a superfluid is generally regarded as a disordered tangle of quantized vortices in three dimensions, or a disordered planar distribution of quantized vortices in two dimensions. However, not all vortex distributions, even large disordered ones, are expected to exhibit robust signatures of quantum turbulence. Identification and development of techniques for controlled forcing or initialization of turbulent vortex distributions is now underway. In this dissertation, I will discuss experimental techniques that were examined during the course of my dissertation research, namely generation of large disordered distributions of vortices, and progress towards injecting clusters of vortices into a BEC. Complimentary to vortex generation is the need to image these vortex distributions. The nondeterministic nature of quantum turbulence and other far-from-equilibrium superfluid dynamics requires the development of new imaging techniques that allow one to obtain information about vortex dynamics from a single BEC. To this end, the first vortex microscope constructed as part of my dissertation research enabled the first in situ images of quantized vortices in a single-component BEC, obtained without prior expansion. I have further developed and characterized a second vortex microscope, which has enabled the acquisition of multiple in situ images of a lattice of vortex cores, as well as the acquisition of single in situ images of vortex cores in a BEC confined in a weak hybrid trap. In this dissertation, I will discuss the state-of-the-art of imaging vortices and other superfluid phenomena in the University of Arizona BEC lab, as indicated by the examined performance of the quantum vortex microscope.

Nesta dissertação nós revisamos a teoria básica que descreve a junção Josephson bosônica para uma e duas espécies partindo do modelo de Bose-Hubbard. Em seguida explicamos como é possível gerar campos de calibe artificiais em um sistema de átomos neutros, como é o caso do condensado de Bose-Einstein. Finalmente, utilizando os conhecimentos teóricos desenvolvidos anteriormente nós buscamos os estados estacionários de um sistema de pseudospin 1/2 submetido a um campo de calibre não-Abeliano artificial, que torna a dinâmica da junção muito mais complexa e rica. Nós também exploramos um novo desbalanceamento de população que surge no sistema, devido a presença do campo de calibre, com características similares as do Macroscopic Quantum Self-Trapping.
In this dissertation we review the basic theory that describes the bosonic Josephson junction for one and two species using the Bose-Hubbard model. Afterwards, we explain how it is possible to generate artificial gauge fields for neutral atoms, like a Bose-Einstein condensate. Finally, using this theoretical background we search for stationary states of a pseudospin 1/2 system subject to a non-Abelian artificial gauge field which turns the dynamic of the junction much more complex and rich. We also explore a possible new populational imbalance that appears on the system due to the presence of the gauge field, with similar features as the Macroscopic Quantum Self-Trapping.

Investigamos o sistema formado por dois condensados aprisionados em estados hiperfinos diferentes do Rubídio, num potencial em forma de charuto, ou seja, num sistema físico real e quase-unidimensional. É investigada a dependência das soluções das equações de Gross-Pitaevski com a separação entre as armadilhas, bem como com o parâmetro de acoplamento de Josephson, para três valores diferentes do número total de átomos aprisionados. Para alguns conjuntos de parâmetros constatamos a existência de estados metaestáveis. O observável que escolhemos para caracterizar tal sistema físico foi a separação média entre os pacotes, pois os dois ramos de soluções encontramos correspondem a soluções mais juntas ou mais separadas espacialmente.
We study the system formed by two coupled condensates of different Rubidium hyperfine states trapped in a cigar shaped potential, that is, a real quasi one-dimensional system. The dependency of the solution of the Gross-Pitaevski equations is investigated as a function of trap displacement and Josephson coupling parameter for three different values of the total trapped atoms number. For some sets of parameters we report the existence of metastable states. The observable we chose to characterize this system was the mean separation between the packages, because we found two branches which correspond to closer or more separated solutions.

Les propriétés thermodynamiques ainsi que l'évolution temporelle des systèmes bidimensionnels sont nettement différentes de celles de systèmes à trois dimensions. Ce travail de thèse présente des expériences réalisées avec des gaz ultrafroids uniformes de bosons en interaction faible, et confinés à deux dimensions d'espace. Ces expériences permettent de mettre en lumière certains traits caractéristiques de l'équilibre thermique et de la dynamique hors équilibre des systèmes à deux dimensions. Un expérimentateur travaillant avec des atomes froids possède une boîte à outils très fournie : la géométrie, la température, l'état interne des atomes sont très bien contrôlés, et de nombreuses méthodes permettant d'étudier leurs propriétés sont disponibles. En particulier, nous travaillons avec des gaz de densité uniforme dont la géométrie peut être choisie à volonté. Je décris l'installation expérimentale et les outils à notre disposition dans une première partie. Dans une deuxième partie, je présente une série d'expériences concernant la transition de phase Berezinskii-Kosterlitz-Thouless d'un gaz de Bose bidimensionnel. Il s'agit d'une transition de phase topologique pour laquelle le système présente un ordre à quasi-longue portée en dessous de la température critique. Nous avons développé deux méthodes expérimentales pour sonder cet ordre à quasi-longue portée. Dans une troisième et dernière partie, je détaille les symétries qui sous-tendent la dynamique d'un gaz proche d'une température nulle dans un piège harmonique. Ces symétries sont les symétries cachées de l'équation de Schrödinger non-linéaire, qui décrit plusieurs autres systèmes physiques. Nous avons testé ces symétries expérimentalement, et nous avons également observé des formes dont l'évolution est périodique dans un potentiel harmonique en présence de non-linéarités. Ces formes géométriques pourraient constituer un nouveau type de solutions périodiques de cette équation non-linéaire
The thermodynamic properties and the dynamical behaviour of two-dimensional systems differ notably from the ones in three dimensions. This work presents experiments performed with ultracold clouds of uniform weakly interacting bosons confined in two dimensions of space. These experiments explore some specific features of the thermodynamics and the out-of equilibrium dynamics of two-dimensional systems. Working with ultracold atoms provides the experimentalist with a rich toolbox: geometry, temperature and internal state of the system are well controlled, and various methods to investigate their properties are available. In particular we work with uniform Boses gases in highly tunable geometries. I describe the set-up and our experimental toolbox in a first part. In a second part I present experiments to investigate the Berezinskii-Kosterlitz-Thouless transition of a two-dimensional Bose gas. It is a topological phase transition for which the system displays a quasi-long range order below the critical temperature. We have developed two experimental schemes to probe this quasi-long range order. In a third and final part I explain the symmetries that underlie the dynamics of a cloud near zero temperature in a harmonic potential. These symmetries are the hidden symmetries of the two-dimensional non-linear Schrödinger equation, which describes many other physical systems. We could probe these symmetries experimentally, and we also observed initial shapes whose evolution is periodic in a harmonic potential in the presence of a non-linearity. They could constitute new breathers of this non-linear equation

Cette thèse est consacrée à la description de la physique à une particule ainsi qu'à celle de fluides quantiques bosoniques dans des systèmes topologiques. Les deux premiers chapitres sont introductifs. Dans le premier, nous introduisons des éléments de théorie des bandes et les quantités géométriques et topologiques associées : tenseur métrique quantique, courbure de Berry, nombre de Chern. Nous discutons différents modèles et réalisations expérimentales donnant lieu à des effets topologiques. Dans le second chapitre, nous introduisons les condensats de Bose-Einstein ainsi que les excitons-polaritons de cavité.La première partie des résultats originaux discute des phénomènes topologiques à une particule dans des réseaux en nid d'abeilles. Cela permet de comparer deux modèles théoriques qui mènent à l'effet Hall quantique anormal pour les électrons et les photons dû à la présence d'un couplage spin-orbite et d'un champ Zeeman. Nous étudions aussi l'effet Hall quantique de vallée photonique à l'interface entre deux réseaux de cavités avec potentiels alternés opposés.Dans une seconde partie, nous discutons de nouveaux effets qui émergent due à la présence d'un fluide quantique interagissant décrit par l’équation de Gross-Pitaevskii dans ces systèmes. Premièrement, il est montré que les interactions spin anisotropes donnent lieu à des transitions topologiques gouvernées par la densité de particules pour les excitations élémentaires d’un condensat spineur d’exciton-polaritons.Ensuite, nous montrons que les tourbillons quantifiés d'un condensat scalaire dans un système avec effet Hall quantique de vallée, manifestent une propagation chirale le long de l'interface contrairement aux paquets d'ondes linéaires. La direction de propagation de ces derniers est donnée par leur sens de rotation donnant lieu à un transport de pseudospin de vallée protégé topologiquement, analogue à l’effet Hall quantique de spin.Enfin, revenant aux effets géométriques linéaires, nous nous sommes concentrés sur l’effet Hall anormal. Dans ce contexte, nous présentons une correction non-adiabatique aux équations semi-classiques décrivant le mouvement d’un paquet d’ondes qui s’exprime en termes du tenseur géométrique quantique. Nous proposons un protocole expérimental pour mesurer cette quantité dans des systèmes photonique radiatifs
This thesis is dedicated to the description of both single-particle and bosonic quantum fluid Physics in topological systems. After introductory chapters on these subjects, I first discuss single-particle topological phenomena in honeycomb lattices. This allows to compare two theoretical models leading to quantum anomalous Hall effect for electrons and photons and to discuss the photonic quantum valley Hall effect at the interface between opposite staggered cavity lattices.In a second part, I present some phenomena which emerge due to the interplay of the linear topological effects with the presence of interacting bosonic quantum fluid described by mean-field Gross-Pitaevskii equation. First, I show that the spin-anisotropic interactions lead to density-driven topological transitions for elementary excitations of a condensate loaded in the polariton quantum anomalous Hall model (thermal equilibrium and out-of-equilibrium quasi-resonant excitation configurations). Then, I show that the vortex excitations of a scalar condensate in a quantum valley Hall system, contrary to linear wavepackets, can exhibit a robust chiral propagation along the interface, with direction given by their winding in real space, leading to an analog of quantum spin Hall effect for these non-linear excitations. Finally, coming back to linear geometrical effects, I will focus on the anomalous Hall effect exhibited by an accelerated wavepacket in a two-band system. In this context, I present a non-adiabatic correction to the known semiclassical equations of motion which can be expressed in terms of the quantum geometric tensor elements. We also propose a protocol to directly measure the tensor components in radiative photonic systems

Les gaz quantiques atomiques constituent un outil de choix pour étudier la physique à N corps grâce à leurs nombreux paramètres de contrôle. Ils offrent la possibilité d’explorer la physique en basse dimension, modifiée par rapport au cas à trois dimensions (3D) à cause du rôle accru des fluctuations. Dans ce travail, nous étudions le gaz de Bose à deux dimensions (2D) avec un confine-ment original dans le plan atomique, uniforme et de motif arbitraire. Ces gaz2D et uniformes, développés sur un montage existant, ont été installés sur un nouveau montage grâce à des potentiels optiques polyvalents.Nous présentons une série d’expériences exploitant cette géométrie flexible.D’abord, nous étudions le comportement statique et dynamique d’un gaz uni-forme lors de la transition d’un état 3D normal vers un état 2D superfluide.Nous observons l’établissement de la cohérence de phase dans un gaz à l’équilibre puis nous montrons l’apparition après une trempe de défauts topologiques dont le nombre est comparé à la prédiction de Kibble-Zurek. Ensuite, nous étudions grâce au nouveau montage les effets collectifs dans l’interaction lumière-matière, où les propriétés de résonance d’un nuage d’atomes dense sont fortement modifiées par rapport à celles d’un atome unique. Enfin, nous proposons deux protocoles pour le nouveau montage. Le premier permet d’évaporer de manière uniforme un gaz 2D grâce au réseau incliné du confinement à 2D. Le second propose de produire des supercourants de manière déterministe dans des pièges en anneaux, soit par condensation dans un champ de jauge, soit en réalisant une pompe à vortex topologique
Degenerate atomic gases are a versatile tool to study many-body physics. They offer the possibility to explore low-dimension physics, which strongly differs from the three dimensional (3D) case due to the enhanced role of fluctuations. In this work, we study degenerate 2D Bose gases whose original in-plane confinement is uniform and of arbitrary shape. These 2D uniform traps, which we first developed on an existing set-up, were subsequently implemented on a newset-up using versatile optical potentials. We present a series of experiments that take advantage of this flexible geometry. First, we study the static and dynamic behaviours of a uniform gas at the transition between a 3D normal and a 2D superfluid state. We observe the establishement of extended phase coherence, followed, as the gas is quench cooled, by the apparition of topological defects whose scaling is compared to the Kibble-Zurek prediction. Second, we present the first results of the new set-up : we investigate collective effects in light-matter interactions, where the resonance properties of a dense ensemble of atoms are strongly modified with respect to the single atom ones. Last, we develop two experimental proposals for the new set-up. The first one studies how a 2D gas can be uniformly evaporated using the tilted lattice providing the 2D confinement. In the second one, we propose to produce su-percurrents in a deterministic way in ring-shaped traps either by condensing inan artificial gauge field or by implementing a topological vortex pump

Two-component fluids can be miscible (if they overlap in space) or immiscible (if they remain phase-separated). In the context of trapped two-species Bose-Einstein condensates (BECs), these miscibility regions can only be fully characterize if one considers the interspecies interaction, the mass ratio and the number of atoms in each species. The dynamics of coupled vortices is different for each miscibility region and exotic vortices configurations (such as, square vortex lattices, \"vortex sheets\", skyrmions, etc.) are expected to occur. In this thesis, we present the construction of a new experimental system able to produce a two-species Bose-Einstein condensate of 23Na-41K atoms with tunable interspecies interactions and study the dynamics of coupled vortices in the different miscibility regimes. The BEC of sodium atoms obtained first in a Plug trap and later, in a crossed optical dipole trap, is fully characterized as well as the cold atomic cloud of potassium atoms produced by means of a Gray molasses cooling procedure. In the crossed optical dipole trap, the vortices will be nucleated with the use of a stirring beam. Therefore, in the end of this thesis, we present the stirring beam setup and its characterization prior aligning it into the 23Na BEC.
Um sistema de dois fluídos pose ser miscível (se os fluídos ocupam a mesma região do espaço) ou imiscível (se eles permanecem separados). No caso de condesados de Bose-Einstein (do inglês, \"Bose-Einstein condensate\" - BEC) de duas espécies atômicas aprisionados, as regiões de miscibilidade só podem ser completamentamente caracterizadas se considerarmos a interção entre as espécies, a razão entre as massas e o número de átomos em cada uma das espécies. A dinâmica de vórices é diferente para cada região de miscibilidade possibilitando a obtenção de configurações exóticas de vórtices (como, a produção de redes de vórtices quadradas, de folhas de vórtices (do inglês, \"vortex sheets\"), skyrmions, etc.). Nesta tese, apresentamos a construção de um novo sistema experimental capaz de produzir um condensado de Bose-Einstein de duas espécies atômicas, 23Na-41K, com interação variável e estudar a dinâmica de vórtices em diferentes regimes de miscibilidade. O condensado de átomos de sódio, inicialmente obtido na armadilha Plug e depois, em uma armadilha ótica cruzada, é completamentamente caracterizado assim como a nuvem atômica ultra-fria produzida a partir da técnica de molasses cinza (do inglês, \"Gray molasses\"). Na armadilha ótica, os vórtices serão produzidos a partir da utilização de um feixe de laser denominado stirring. Assim, ao final da tese, apresentamos o esquema ótico para a produção deste feixe de laser e a sua caracterização antes de alinhá-lo nos átomos.

In this work we constructed an experimental system to realize a BEC of sodium atoms. In the first part of the work, we study two atomic sources in order to choose the most suitable for our system. The comparison between a Zeeman slower and a bidimensional magnetooptical trap (2D-MOT) was performed to evaluate the capacity of producing an appropiate flux of atoms in order to load a tridimensional magneto-optical trap (3D-MOT). The experimental results show that the 2D-MOT is as efficient as the Zeeman slower with the advantage of being more compact and easier to operate, and for these reasons we choose it as our source of cold atoms. After this, the experimental apparatus to produce a Bose-Einstein condensate was constructed and characterized. With this experimental system we realized all the required stages to achieve the Bose-Einstein condensation (BEC). Initially, we characterized and compared the performance between the Bright-MOT and Dark-SPOT MOT of sodium atoms, observing the great advantages this last configuration offers. Afterward, we implemented the experimental sequence for the achivement of the BEC of sodium atoms. After the optical molasses process, the atoms are tranferred to an optically plugged quadrupole trap (OPT) where the process of evaporative cooling is performed. With this setup, we achive a sodium BEC with ∼ 5×105 atoms and a critical temperature of ∼ 1.1 μK. Finally, with the constructed and characterized machine, we started to perform experiments of cooperative absorption of two photons by two trapped atoms. With the new system, we wanted to take advantage of the higher densities in the magnetic trap and BEC to explore some features of this phenomenon in the classical and quantum regimes. We were interested in exploring some features of this nonlinear light-matter interaction effect. The idea of having two or more photons interacting with two or more atoms is the beginning of a new possible class of phenomena that we could call many photons-many body intercation. In this new possibity, photons and atoms will be fully correlated, introducing new aspects of interactions.
Neste trabalho, realizamos a construção de um sistema experimental para a realização de um condensado de Bose-Einstein de átomos de sódio. Na primeira parte do trabalho, realizamos o estudo de duas fontes átomicas com o intuito de escolher a mais adequada para nosso sistema experimental. A comparação foi realizada entre um Zeeman slower e uma armadilha magneto-óptica bidimensional (MOT-2D), que são técnicas usadas para fornecer um grande fluxo de átomos com distribuição de velocidades adequadas para serem capturados numa armadilha magneto-óptica tridimensional (MOT-3D). Os resultados experimentais da caracterização de ambos os sistemas mostra que o MOT-2D oferece um grande fluxo atômico da mesma ordem do Zeeman slower, mas com a vantagem de ser um sistema mais compacto em questão de tamanho, razão pela qual foi escolhido como fonte atômica no nosso sistema. A partir daqui, realizamos a construção do sistema experimental para a realização do condensado de sódio. Inicialmente realizamos o aprisionamento numa MOT-3D, realizando subsequentemente os passos de resfriamento sub-Doppler mediante o processo de molasses ópticas. Depois disto, os átomos são transferidos para uma armadilha magnética, que consiste de um par de bobinas em configuração anti-Helmholtz, as mesmas usadas para a MOT-3D mas com um gradiente de campo magnético ao redor de uma ordem de grandeza maior. Esta armadilha é combinada com um laser com dessintonia para o azul focado a 30 μm no centro da armadilha, onde o campo magnético é zero com o objetivo de evitar as perdas por majorana que acontecem nessa região. Com esta configuração, um condensado de ∼ 5 × 105 átomos é obtido a uma temperatura crítica de ∼ 1.1 μK. Por último, com a máquina construída e caracterizada, começamos re-explorar o experimento de absorção cooperativa de dois fótons por dois átomos aprisionados. Com nosso novo sistema, é possível explorar este efeito no regime clássico e quântico. Estamos interessados em explorar algumas características da interação não linear entre luz e matéria. A ideia de ter dois ou mais fótons interagindo com um ou mais átomos, é possivelmente o começo de uma nova classe de fenômenos que poderíamos chamar de interação de muitos fótons com muitos átomos.

La physique moderne repose sur deux théories fondamentales distinctes, la relativité générale et la mécanique quantique. Toutes les deux décrivent d’une part les phénomènes macroscopiques et cosmologiques tels que les ondes gravitationnelles et les trous noirs et d’autre part les phénomènes microscopiques comme la superfluidité ou le spin des particules. L’unification de ces deux théories reste, jusqu’à présent, un problème non résolu. Il est intéressant de noter que les différentes théories de gravité quantique prédisent une violation des principes de la relativité générale à différents niveaux.Il est donc hautement intéressant de détecter les violations de ces principes et de déterminer à quel niveau elles se produisent.De récentes propositions pour effectuer des tests du principe d’ équivalence d’Einstein suggèrent une amélioration spectaculaire des performances en utilisant des capteurs atomiques `a ondes de matière.Dans ce contexte, il est nécessaire de concevoir des états d’entrée de l’interferomètre avec des conditions initiales bien définies. Un test de pointe de l’universalité de la chute libre (Universality of FreeFall en anglais (UFF) ) nécessiterait, par exemple,un contrôle des positions et des vitesses avec une précision de l’ordre de 1 μm et 1 μm.s⁻¹ , respectivement.De plus, les systématiques liées à la taille du paquet d’ondes limitent le taux d’expansion maximum possible à 100 μm.s⁻¹. La création initiale des états d’entrée de l’interféromètre doit être assez rapide,de l’ordre de quelques centaines de ms au maximum,pour que le temps de cycle de l’expérience soit pertinent d’un point de vue métrologique. Dans cette thèse j’ai développé des séquences optimisées s’appuyant sur l’excitation du centre de masse et de la taille d’un ou plusieurs ensembles d’atomes refroidis ainsi que dégénérés. Certaines séquences proposé dans cette thèse ont déjà été implémenté dans des expériences augmentant de manière significative le contrôle des ensembles atomiques
Modern physics relies on two distinct fundamental theories, General Relativity and Quantum Mechanics. Both describe on one hand macroscopic and cosmological phenomena such as gravitational waves and black holes and on the other hand microscopic phenomena as superfluidity or the spin of particles. The unification of these two theories remains, so far, an unsolved problem. Interestingly, candidate Quantum Gravity theories predict a violation of the principles of General Relativity at different levels. It is, therefore, of a timely interest to detect violations of these principles and determine at which level they occur. Recent proposals to perform Einstein Equivalence Principle tests suggest a dramatic performance improvement using matter-wave atomic sensors. In this context, the design of the input states with well defined initial conditions is required. A state-of-the-art test of the universality of free fall (UFF) would, for example, require a control of positions and velocities at the level of 1 µm and 1 µm.s⁻¹, respectively. Moreover, sizerelated systematics constrain the maximum expansion rate possible to the 100 µm.s⁻¹level. This initial engineering of the input states has to be quite fast, of the order of few hundred ms at maximum, for the experiment’s duty cycle to be metrologically-relevant. In this thesis I developed optimized sequences based on the excitation of the center of mass and the size excitation of one or two cooled atomic sample as well as degenerated gases. Some sequences proposed in this thesis have already been implemented in experiments and significantly increase the control of atomic ensembles

Cette thèse est dédiée à l'étude des fluctuations non-linéaires dans les condensats de Bose-Einstein à deux composantes. On présente dans le premier chapitre la dynamique de champ moyen des condensats à deux composantes et les différents phénomènes typiques associés au degré de liberté spinoriel. Dans ce même chapitre, on montre que la dynamique des excitations se sépare en deux modes distincts : un mode dit de densité correspondant au mouvement global des atomes à l'intérieur du condensat et un mode dit de polarisation correspondant à la dynamique relative entre les deux espèces constituant le condensat. Ce calcul est généralisé dans le deuxième chapitre où l'on montre que le mode de polarisation persiste en présence d'un couplage cohérent entre les deux composantes. En particulier on analyse la stabilité modulationnelle du mode en déterminant, à l'aide d'une analyse multi-échelle, la dynamique des excitations non-linéaires. On montre alors que les excitations de polarisation, au contraire des excitations de densité, souffrent d'une instabilité de Benjamin-Feir. Cette instabilité est stabilisée aux grandes impulsions par une résonance onde longue - onde courte. Enfin dans le dernier chapitre, on dérive de façon non-perturbative la dynamique de polarisation proche de la limite de Manakov, dynamique quise révèle être régie par une équation de Landau-Lifshitz sans dissipation. Les équations de Landau-Lifshitz appartiennent à une hiérarchie d'équations intégrables (hiérarchie Ablowitz-Kaup-Newell-Segur) et on étudie les solutions à une phase à l'aide de la méthode d'intégration finite-gap ; on détermine notamment à l'aide de cette méthode un nouveau type de soliton pour les condensats à deux composantes. Finalement, profitant de l'intégrabilité du système, on résout le problème de Riemann à l'aide de la théorie de modulation de Whitham et on montre que les condensats à deux composantes peuvent propager des ondes de raréfaction ainsi que des ondes de choc dispersives ; on décrit notamment la modulation de ces ondes de choc par la propagation d'ondes simples et d'ondes de contact d'invariants de Riemann
This thesis is devoted to the study of nonlinear fluctuations in two-component Bose-Einstein condensates. In the first chapter we derive the mean field dynamics of two-component condensates and we present the distinctive phenomena associated to the spinorial degree of freedom. In the same chapter, we show that the dynamics of the excitations is divided in two distinct modes: a so-called density mode which corresponds to the global motion of the atoms, and a so-called polarization mode which corresponds to the relative motion between the two species composing the condensate. The computation is generalized in the second chapter in which we demonstrate that the polarization mode remains in presence of a coherent coupling between the two components. In particular we study the modulational stability of the mode and we determine through a multi-scaling analysis the dynamics of non-linear excitations. We show that the excitations of polarization undergo a Benjamin-Feir instability contrary to the density excitations. This instability is then stabilized in the short wavelength regime by a long wave - short wave resonance. Finally in the last chapter, we derive in a non-perturbative way the polarisation dynamics close the Manakov limit.In this limit, the dynamics proves to be governed by a Landau-Lifshitz equation without dissipation. Landau-Lifshitz equations belong to a hierarchy of integrable equations (Ablowitz-Kaup-Newell-Segur hierarchy) and we derive the single-phase solutions thanks to the finite-gap method; in particular we identify a new type of soliton for the two-component Bose-Einstein condensates. Finally, taking advantage of the integrability of the system, we solve the Riemann problem thanks to the Whitham modulation theory and we show that the two-component condensates can propagate rarefaction waves as well as dispersive shockwaves; we describe the modulation of the shockwaves by the propagation of simple waves and contact waves of Riemann invariants

Nesta dissertação estudaremos sistemas de bósons ultrafrios armadilhados em uma rede ótica quadrada bidimensional sem levar em consideração o confinamento harmônico. A dinâmica desses sistemas é bem descrita pelo modelo de Bose-Hubbard, que prevê uma transição de fase quântica de um superfluido para um isolante de Mott a temperaturas baixas, e pode ser induzida variando a profundidade do potencial da rede ótica. Apresentaremos o diagrama de fases dessa transição construído a partir de uma aproximação de campo médio e também com um cálculo numérico usando um algoritmo de Monte Carlo Quântico, denominado algoritmo Worm. Encontramos o ponto crítico para o primeiro lobo de Mott em ambos os casos, concordando com trabalhos anteriores.
This work study the two-dimensional ultracold bosonic atoms loaded in a square optical lattice, without harmonic confinement. The dynamics of this system is described by the Bose-Hubbard model, which predicts a quantum phase transition from a superfluid to a Mott-insulator at low temperatures that can be induced by varying the depth of the optical potential. We present here the phase diagram of this transition built from a mean field approach and from a numerical calculation using a Quantum Monte Carlo algorithm, namely the Worm algorithm. We found the critical transition point for the first Mott lobe in both cases, in agreement with the standard literature.

博士
國立中興大學
應用數學系所
100
In this dissertation, we study various types of numerical continuation methods for computing numerical solutions of multi-parameter nonlinear eigenvalue problems. These include two-grid continuation algorithms, spectral Galerkin and continuation algorithms, and spectral collocation and continuation algorithms. For the last two types of continuation algorithms, we use the second kind Chebyshev polynomials as the basis functions for the trial function space. The proposed algorithms are exploited to compute symmetry-breaking solutions of the Gross-Pitaevskii equation, the ground state solutions of rotating Bose-Einstein condensates (BEC), and rotating two-component BECs. First, We present an efficient spectral-Galerkin continuation method (SGCM) and two-grid centered difference approximations for symmetry-breaking solutions of the GPE. Some basic formulae for the SGCM are derived so that the eigenvalues of the associated linear eigenvalue problems can be easily computed. The SGCM is implemented to investigate the ground and first excited state solutions of the GPE. Both the parabolic and quadruple-well trapping potentials are considered. We also study BEC in optical lattices, where the periodic potential described by the sine or cosine functions is imposed on the GPE. Next, we study spectral collocation continuation method (SCCM) for rotating BEC and rotating BEC in optical lattices. The ground state and first excited state solutions of rotating BEC in optical lattices are investigated. Finally, We study efficient SCCM for rotating two-component BECs and rotating two-component BECs in optical lattices. A novel two-parameter continuation algorithm is proposed for computing the ground state and first excited state solutions of the governing GPEs, where the classical tangent vector is split into two constraint conditions for the bordered linear systems. Numerical results on rotating two-component BECs and rotating two-component BECs in optical lattices are reported. The results on the former are consistent with published numerical results.

碩士
國立東華大學
應用物理研究所
97
We investigate the ground state configuration under the mean-field approximation for two interacting Bose-Einstein condensates (BECs) trapped in a cigar-shaped potential. Using the steepest decent method we find the corresponding lowest energy state of a novel spatially phase-separated form. In particular, when the number ratio between two components as well as the degree of anisotropy for the trapped potential are larger than the critical values, the interspecies interaction repels the minority component to the extreme ends that leads to the split-shell/core configuration. This result shows that the shell/core configuration obtained from solving the coupled Gross-Pitaevskii equations under the Thomas-Fermi approximation is not a lowest energy state.

碩士
國立臺灣大學
數學研究所
103
We investigate interaction of bright solitons for two-component Bose-Einstein condensates (BECs) in one and two dimensions numerically (1D, 2D). The numerical methods we adopt are: (1) Gradient flow with discrete normalization (GFDN) method for computing the profile function of solitons in 2D. We use backward Euler sine pseudospectral (BESP) method to discretize it. The algorithm is constructed by Chern and Bao [2]. (2) Timesplitting sine pseudospectral (TSSP) method for computing the evolution of wave functions. The algorithm is construct by Bao [1]. We discuss the change of velocities and shapes of the wave packets during and after the interactions between them. It is found that (1) In 1D, soliton collisions are like elastic collisions under strong repulsive interactions. When the interactions are attractive and strong enough, the wave packets may split into two or more parts after collisions. (2) In 2D, wave packets spread out after collisions when the interactions are repulsive or weak attractive. The wave functions blow up during interactions when the attractive interactions are strong enough.

碩士
國立東華大學
應用物理研究所
98
In the present work, we investigate the ground state configurations for a system of two Bose-Einstein condensates with different atomic masses. We numerically solve the Gross-Pitaevskii equations and find the mean-field solutions of a binary mixture of trapped atomic Bose-Einstein condensates. The numerical simulations show that the differences of masses of the atoms have no significant influence on the boundaries of mixed and separated phases. In the separated phases of parameter space, the larger ratio of atomic masses always leads to “the split-shell/core configuration. It is easier to have symmetric phase-separation, when the ratios of the scattering lengths between two atomic species is larger.

Chan Chak Ming = 二元玻色-愛因斯坦凝聚態之硏究 / 陳澤明.
Thesis (M.Phil.)--Chinese University of Hong Kong, 2001.
Includes bibliographical references (leaves [100]-104).
Text in English; abstracts in English and Chinese.
Chan Chak Ming = Er yuan Bose-Aiyinsitan ning ju tai zhi yan jiu / Chen Zeming.
Abstract --- p.i
Acknowledgments --- p.ii
Contents --- p.iii
List of Figures --- p.vi
Chapter Chapter 1. --- Introduction --- p.1
Chapter Chapter 2. --- Theory of Bose-Einstein Condensate (BEC) --- p.4
Chapter 2.1 --- Trapped Ideal Bose Gas --- p.5
Chapter 2.2 --- Bogoliubov Theory of Weakly Interacting Bosons --- p.7
Chapter 2.2.1 --- One-component BEC --- p.7
Chapter 2.2.2 --- Two-component BEC --- p.12
Chapter Chapter 3. --- Condensate Wavefunctions and Collective Excitations --- p.16
Chapter 3.1 --- Properties of Condensate Wavefunctions --- p.16
Chapter 3.2 --- Collective Excitations --- p.21
Chapter 3.3 --- Appendix: Numerical Methods and Practical Procedures --- p.26
Chapter 3.3.1 --- Gradient Descent Method --- p.27
Chapter 3.3.2 --- Iterative Diagonalization Method --- p.28
Chapter 3.3.3 --- Practical Procedures --- p.30
Chapter Chapter 4. --- Noncondensate Atoms in Homogeneous BEC --- p.33
Chapter 4.1 --- Noncondensate Atoms in One-Component BEC --- p.33
Chapter 4.2 --- Bogoliubov Theory for Two-species Homogeneous BEC --- p.35
Chapter 4.3 --- Same Mass System: m1= m2 --- p.37
Chapter 4.4 --- Unequal Mass System: m1 ≠ m2 --- p.48
Chapter 4.5 --- Summary --- p.54
Chapter Chapter 5. --- Noncondensate Atoms in a Trapped BEC --- p.55
Chapter 5.1 --- Case I: The Noncondensate Atoms in the Mixture of Two Spin States of 87Rb --- p.57
Chapter 5.2 --- Case II: The Noncondensate Atom in the Mixture of 87Rb and 23Na --- p.61
Chapter 5.3 --- Summary --- p.64
Chapter Chapter 6. --- Two-component BEC in Relative Motion --- p.65
Chapter 6.1 --- Bogoliubov Theory for Motional Two BEC --- p.65
Chapter 6.2 --- Stability Analysis --- p.69
Chapter 6.2.1 --- Dynamical Stability Analysis --- p.69
Chapter 6.2.2 --- Anomalous Mode Analysis --- p.75
Chapter 6.2.3 --- "Critical Velocity, Anomalous Modes Critical Velocity and Sound Velocities" --- p.78
Chapter 6.3 --- Motional Two-component BEC in a Ring --- p.80
Chapter 6.4 --- Two-component BEC of the Same Species --- p.85
Chapter 6.4.1 --- Moving Particles in Momentum Space --- p.88
Chapter 6.4.2 --- Moving Particles in Real Space --- p.93
Chapter 6.4.2.1 --- Strong coupling regime: (g > k02/2) --- p.93
Chapter 6.4.2.2 --- Weak-coupling regime: (g《Chapter 6.5 --- Summary --- p.95
Chapter Chapter 7. --- Conclusion --- p.93
Bibliography --- p.100

碩士
國立清華大學
數學系
95
In this thesis, we use local continuation method to study a two-component Bose-Einstein condensate (BEC) in magnetic field numerically. First, we show the discretized process of a two-component BEC in magnetic field that is the time-independent coupled nonlinear Schrodinger equation. Second, we present the algorithm and the numerical results.

碩士
國立東華大學
物理學系
102
A system of two-component Bose-Einstein condensate (BEC) with laser-induced coupling is used to mimic the massless and massive particles, in the so-called “analogue gravity” programme. In such experiments, Bose condensate of type 1 creates a second component BEC of type 2 and vice-versa, exhibiting a Josephson-like dynamics. In this case, the hydrodynamics collective excitations involve, in addition to the usual massless Goldstone mode, a massive mode, describing population oscillations between the components. We study the conditions required to decouple these two modes, so that the wavefunctions can be expressed in the Klein-Gordon form. In the restricted parameter space, the spacetime metric and the effective mass term are successfully rewritten in terms of the BEC parameters. The simplest configuration of the model is discussed and we analyze the behaviors of the condensate density, sound speed of phonons, and the effective mass of the Klein-Gordon equations.