This thesis builds upon the concept of quantum simulation, where an inherently quantum system functions as an analogue computer. The programming of the dynamics in the simulator is done through the controlled engineering of the Hamiltonian that describes the time evolution of an ensemble of ultracold atoms. This enables multiple systems of interest to be studied in a controllable environment, providing an alternative to the sought after 'quantum computer'. The quantum simulator developed at the University of Auckland is presented, highlighting the elements used to provide the necessary degree of control over the system dynamics. Furthermore, we present a series of transmissive experiments conducted on a twodimensional degenerate quantum gas of 87Rb designed to study quantum transport eects. Starting from a Bose-Einstein condensate, the atoms are loaded into a twodimensional trap with a superimposed customizable optical potential. created by imaging a spatial light modulator. We focus on a potential consisting of two reservoirs and a connecting channel that functions as an atomic waveguide. An 'atomtronic' approach to the study of transport properties in the potential allows us to model the dynamics as an analogous electronic system. Addition of point-like disorder in the potential enables the study of Anderson localization eects through the measurement of an eective channel resistance. The observed dynamics of the atomic conductance in long channels is consistent with quantum interference eects, showing signatures of two-dimensional Anderson localization.
This thesis builds upon the concept of quantum simulation, where an inherently quantum system functions as an analogue computer. The programming of the dynamics in the simulator is done through the controlled engineering of the Hamiltonian that describes the time evolution of an ensemble of ultracold atoms. This enables multiple systems of interest to be studied in a controllable environment, providing an alternative to the sought after 'quantum computer'. The quantum simulator developed at the University of Auckland is presented, highlighting the elements used to provide the necessary degree of control over the system dynamics. Furthermore, we present a series of transmissive experiments conducted on a twodimensional degenerate quantum gas of 87Rb designed to study quantum transport eects. Starting from a Bose-Einstein condensate, the atoms are loaded into a twodimensional trap with a superimposed customizable optical potential. created by imaging a spatial light modulator. We focus on a potential consisting of two reservoirs and a connecting channel that functions as an atomic waveguide. An 'atomtronic' approach to the study of transport properties in the potential allows us to model the dynamics as an analogous electronic system. Addition of point-like disorder in the potential enables the study of Anderson localization eects through the measurement of an eective channel resistance. The observed dynamics of the atomic conductance in long channels is consistent with quantum interference eects, showing signatures of two-dimensional Anderson localization.
The transport of quantum particles in non ideal material media (eg the conduction of electrons in an imperfect crystal) is strongly affected by scattering from impurities of the medium. Even for a weak disorder, semi-classical theories, such as those based on the Boltzmann equation for matter-waves scattering from the impurities, often fail to describe transport properties and full quantum approaches are necessary. The properties of the quantum systems are of fundamental interest as they show intriguing and non-intuitive phenomena that are not yet fully understood such as Anderson localization, percolation, disorder-driven quantum phase transitions and the corresponding Bose-glass or spin-glass phases. Understanding quantum transport in amorphous solids is one of the main issues in this context, related to electric and thermal conductivities. Ultracold atomic gases can now be considered to revisit the problem of quantum conductivity and quantum transport under unique control possibilities. Dilute atomic Bose-Einstein condensates (BEC) and degenerate Fermi gases (DFG) are produced routinely taking advantage of the recent progress in cooling and trapping of neutral atoms. Transport has been widely investigated in controlled potentials with no defects, for instance periodic potentials (optical lattices). Controlled disordered potentials can also be produced with various techniques such as the use of magnetic traps designed on atomic chips with rough wires, the use of localized impurity atoms, the use of radio-frequency fields or the use of optical potentials. This recently lead to the observation of the Anderson Localisation of a BEC and the measurement of the diffusion coefficient of a 2D gaz in the presence of disorder.
The transport of quantum particles in non ideal mate- rial media (eg the conduction of electrons in an imperfect crystal) is strongly affected by scattering from impurities of the medium. Even for a weak disorder, semi-classical theories, such as those based on the Boltzmann equation for matter-waves scattering from the impurities, often fail to describe transport properties and full quantum approaches are necessary. The properties of the quan- tum systems are of fundamental interest as they show intriguing and non-intuitive phenomena that are not yet fully understood such as Anderson localization, percola- tion, disorder-driven quantum phase transitions and the corresponding Bose-glass or spin-glass phases. Under- standing quantum transport in amorphous solids is one of the main issues in this context, related to electric and thermal conductivities. Ultracold atomic gases can now be considered to re- visit the problem of quantum conductivity and quan- tum transport under unique control possibilities. Dilute atomic Bose-Einstein condensates (BEC) and degener- ate Fermi gases (DFG) are produced routinely taking advantage of the recent progress in cooling and trap- ping of neutral atoms. Transport has been widely in- vestigated in controlled potentials with no defects, for instance periodic potentials (optical lattices). Controlled disordered potentials can also be produced with various techniques such as the use of magnetic traps designed on atomic chips with rough wires, the use of localized impurity atoms, the use of radio-frequency fields or the use of optical potentials. This recently lead to the ob- servation of the Anderson Localisation of a BEC and the measurement of the diffusion coefficient of a 2D gaz in the presence of disorder.
This thesis highlights the versatility of ultracold atoms as quantum simulators by utilizing Bose gases and engineered light-induced Hamiltonians to investigate quantum phenomena across multiple areas of physics.As a high-energy simulator, an analog experiment simulating particle–antiparticle pair creation from the quantum vacuum, emulated these strong-field effects at energy scales accessible in the laboratory. The Dirac picture of particle-antiparticle vacuum and the concept of optical lattice band theory was the foundation of our approach. In this framework, we readily measured pair creation and demonstrated that this high-field phenomenon is well-characterized by Landau-Zener tunneling. Within condensed matter physics, ultracold atoms were employed to study topological dynamics of periodically driven Floquet systems. Using a Floquet “switching” protocol in a one-dimensional bipartite magnetic lattice, we realized a periodically driven Su–Schrieffer–Heeger model that maps onto a massless Dirac Hamiltonian. By alternating between two lattice configurations with near-optimal timing, we observed spin–momentum–locked transport characterized by well-defined drift velocities and with spatial displacement linearly increasing over many Floquet periods, establishing a platform for exploring topological band dynamics. The culminating focus of this thesis is localization physics in Rb-87 Bose-Einstein condensates subjected to disordered artificial gauge fields over a range of energy and time scales, in both equilibrium and out-of-equilibrium settings. The effective Hamiltonian was implemented by driving two-photon Raman transitions with laser fields, while disordered vector potential landscapes were independently generated using tunable intensity patterns projected by a digital micromirror device (DMD). By varying the experimental protocols—including the turn on times of the Raman coupling and disorder, as well as the disorder strength—we obtained insight into quantum dynamics in the presence of disordered gauge fields. The resulting dynamics revealed rich behavior: including spatially inhomogeneous magnetization for high-energy dynamics and increases in the condensate width after time-of-flight for pulsed disorder in lower energy and near-equilibrium conditions; lastly, signatures of localization, in the form of damped oscillations, were observed as the system was driven out-of-equilibrium.
Anderson localization of waves in disordered media was originally predicted[1] fifty years ago, in the context of transport of electrons in crystals[2]. The phenomenon is much more general[3] and has been observed in a variety of systems, including light waves[4, 5]. However, Anderson localization has not been observed directly for matter waves. Owing to the high degree of control over most of the system parameters (in particular the interaction strength), ultracold atoms offer opportunities for the study of disorder-induced localization[6]. Here we use a non-interacting Bose-Einstein condensate to study Anderson localization. The experiment is performed with a one-dimensional quasi-periodic lattice - a system that features a crossover between extended and exponentially localized states, as in the case of purely random disorder in higher dimensions. Localization is clearly demonstrated through investigations of the transport properties and spatial and momentum distributions. We characterize the crossover, finding that the critical disorder strength scales with the tunnelling energy of the atoms in the lattice. This controllable system may be used to investigate the interplay of disorder and interaction (ref. 7 and references therein), and to explore exotic quantum phases[8, 9].
This thesis is primarily a comprehensive discussion of the development of two experimental studies: the quantum transport and effects of heating of ultracold atoms. It specifically provides details of the manipulation and control of ultracold atoms in magnetic waveguides, optical lattices, and optical billiards. The design, construction, and implementation of experimental apparati are also outlined and additional experimental tests are summarized, including the realization of a macroscopic transport (> 20 cm) system for ultracold atoms and transmission of ultracold atoms through a random optical potential. The first experiment is a study of the quantum transport for atoms confined in a periodic potential. These results include a comparison made of thermal and BEC initial conditions. Here, observation of ballistic transport is made for all values of well depth and initial conditions, and the expansion rates for thermal atoms are shown to be in excellent agreement with a singleparticle model. For weak wells (V0/ER ≤ 6), the expansion of the BEC is also in excellent agreement with single-particle theory, using an effective temperature model based on single (non-interacting) particle theory. For deep wells (V0/ER ≥ 6), a crossover is observed to a new regime for the BEC case, indicating the importance of interactions on quantum transport. The second experiment is a study of the effect of different heating rates on a dilute Bose gas confined in a quasi-1D finite, leaky box. An optical kicked-rotor is used to transfer energy to the atoms while two repulsive optical beams are used to confine the atoms. The average energy of the atoms is localized after a large number of kicks and the system reaches a nonequilibrium steady state. A numerical simulation of the experimental data suggests that the localization is due to energetic atoms leaking over the barrier. Our data also indicates a correlation between collisions and the destruction of the BoseEinstein condensate fraction and an exponential decay in phase space density.
A cold atom experiment can be used to simulate analogous solid-state systems. This provides the bene�t of having a high degree of control over the system parameters and allowing direct detection methods. Disordered transport is one example of where such a system has much to o�er. This thesis concerns the development of a Bose-Fermi mixture experiment for study of two-dimensional optical lattice systems. To achieve single site resolution of the lattice, the experiment makes use of a double microscope set-up. One microscope provides imaging and the second is used to image a spatial light modulator onto the atomic plane. This provides an extremely versatile potential landscape for a trapped cloud. This thesis presents an overview of the set-up of the experiment including progress towards condensation. Particular focus is given to the design and characterisation of the vacuum system and the combined double microscope and spatial light modulator system. The vacuum system design requires a narrow magneto-optical trapping chamber. A novel epoxy sealing technique has been developed, allowing construction of a chamber of just 36mm thickness whilst maintaining high optical access. To provide illumination for the spatial light modulator a technique for homogenising the output of multi-mode �bre has been developed.