This work presents an alternative method for analyzing EMCCD-microscopy images of two-dimensional quantum optical lattices, using neuronal networks to automate the recognition of lattice occupation states. We introduce a multi-step algorithm, whose overall performance as well as step-by-step performance is analyzed, and which is compared to several different architectures. Training the networks requires a large amount of training data with known lattice occupation states. These images are simulated by convolution of the experimentally estimated point spread function of the imaging system with the atomic distribution masks. The algorithm allows for an accuracy of up to 99.76 % on our simulated data.
This thesis details the experimental efforts towards quantification of laser frequency noise by the use of an optical frequency discriminator and its suppression by means of measuring and reducing optical path length differences to prevent heating and loss of ultracold Caesium atoms trapped in two-dimensional state-dependent optical lattice. The discriminator used is a Fabry-Perót cavity with the side-of-fringe locking technique to be sensitive to frequency fluctuations of the input light field which are detected as changes in the intensity of the cavity signal. The measured noise spectrum revealed the performance of the laser in the frequency domain and was used to refine the same. A reduction in the laser linewidth was achieved in this manner. The same cavity was also transformed in to a transfer cavity to prevent long-term drift in the laser frequency. The frequency noise cannot be completely eliminated from the laser and so the task then became the reduction of the optical path length differences in the experiment by which the noise can manifest at the postion of the atoms. Conditions for achieving minimal path length differences were derived. Three methods were employed to measure the path length differences: A geometric distance measurement, an optical measurement using interferometry and at last using the atoms. The use of the atoms in particular displayed the extent to which the common-mode frequency noise can influence the experiment.
Diese Bachelorarbeit beschäftigt sich mit dem LCoS räumlichen Lichtmodulator (SLM). Dabei soll die durch Phasenmodulation erfolgende Holografie und der auf Amplitudenmodulation beruhende Aufbau der direkten Abbildung verglichen werden. Insbesondere liegt das Augenmerk auf der Verwendung des SLM zur Erstellung von Intensitätsmustern im zweidimensionalen optischen Gitter des 2D discrete quantum simulator (DQSIM). Es wurden dafür Muster mit beiden Modulationsmodi aufgenommen und analysiert. Die direkte Abbildung liefert im Vergleich zur Holografie Muster mit besserer Ebenheit, Auflösung und Hintergrund-Dunkelheit bei vergleichbarem Kontrast und Signal-Rausch- Verhältnis. Die Holografie kann jedoch je nach Muster eine höhere Lichtausbeute bieten.
Our group’s 2D Discrete Quantum Simulator (DQSIM) experiment is dedicated to the idea of a discrete time quantum walk. A quantum walk is the quantum mechanical analogue of a classical random walk. Discrete refers here to the timing in which evolution operators are applied to two quantum systems, a walker and a coin. It not only exhibits different statistics than the classical counterpart but may be employed in a multitude of ways. For example the experimental simulation of a perfect conductor in which Bloch oscillations are performed or the simulation of topological systems that are otherwise inaccessible in solid state physical scales.
The first chapter reviews the DQSIM setup and necessary concepts to assess the place the content of the thesis is going to take within the experimental effort of our group. Then this thesis deals with two additions to the DQSIM experiment. The first part concerns a specifically designed photodiode amplifier circuit to improve the intensity stabilization of the lattice beams. Improving it would ensure that the coherence time of the atoms isn’t limited by intensity noise any more.
The second part introduces a scheme to realize compression of atomic ensembles trapped in our optical lattice. Furthermore it is a first step in achieving an efficient single plane selection and addressing in our experiment opening the door to many-particle quantum walks. The thesis concludes with a discussion about initial experimental attempts on compression and a summary of the results.
This thesis focuses on the simulation of the physics of a charged particle under an external magnetic field by using discrete-time quantum walks of a spin-1/2 particle in a two-dimensional lattice. By Floquet-engineering the quantum-walk protocol, an Aharonov–Bohm geometric phase is imprinted onto closed-loop paths in the lattice, thus realizing an abelian gauge field—the analog of a magnetic flux threading a two-dimensional electron gas. I show that in the strong-field regime, i.e. when the flux per plaquette of the lattice is a sizable fraction of the flux quantum, magnetic quantum walks give rise to nearly flat energy bands. I demonstrate that the system behaves like a Chern insulator by computing the Chern numbers of the energy bands and studying the excitation of the midgap topologically protected edge modes. These modes are extended all along the boundaries of the magnetic domains and remain robust against perturbations that respect the gap closing conditions. Furthermore, I discuss a possible experimental implementation of this scheme using neutral atoms trapped in two dimensional spin-dependent optical lattices. The proposed scheme has a number of unique features, e.g. it allows one to generate arbitrary magnetic-field landscapes, including those with sharp boundaries along which topologically protected edge states can be localized and probed. Additionally, I introduce the scattering matrix approach in discrete-time quantum walks to probe the Hofstadter spectrum and compute its topological invariants. By opening up a discrete-time quantum walk system and connecting it to metallic leads, I demonstrate that the reflection/transmission probabilities of a particle from the scattering region give information on the energy spectrum and topological invariants of the system. Although the work presented here focuses on the physics of a single particle in a clean system, it sets the stage for studies of many-body topological states in the presence of interactions and disorder.
Im Rahmen dieser Arbeit soll die Intensität eines Lasers über eine Feedback-Schleife stabilisiert werden, und dabei soll eine Bandbreite von über einem MHz erreicht werden, da Rauschen und Schwankungen bei diesen und höheren Frequenzen von den Atomen nicht mehr "wahrgenommen" werden. Es ist bereits möglich eine Stabilisierung der Intensität des Lasers mit einer Bandbreite bis zu ungefähr 100kHz aufzubauen. Dieser Aufbau soll in dieser Arbeit optimiert werden, um Rauschen bis zu mindestens einem MHz zu unterdrücken. Dabei soll hauptsächlich ein geeigneter Verstärker gebaut und so angepasst werden, dass er eine optimale Rauschunterdrückung gewährleistet.
This thesis describes the theoretical and experimental work for reaching fast, high fidelity transport operations of single cesium atoms in a state-dependent optical lattice. By applying optimal control theory to position and depth of the optical lattice potential and using a computer simulation judging the fidelity, fast transport sequences preserving the internal atomic quantum state and preventing any motional excitation can be identified. To allow transport times down to a few microseconds the feedback control system used for steering depth and position of the optical lattice deterministically is overdriven in a controlled way. Transport induced motional excitations are measured experimentally by means of a special microwave sideband spectroscopy, which is improved to reliably detect any excitation and allows a full tomography of the vibrational states of the anharmonic optical lattice potential. Optimal control sequences allowing single site transport of atoms in the oscillation period of the trapping potential are believed to reach the fundamental quantum speed limit of the system.
In our laboratory, we use cesium atoms, which are trapped in the optical lattices. For the practice of quantum walks, atoms must be well isolated from the noisy environment so that long decoherence time can be achieved. It has been analyzed that fluctuations of the lattice depth originated from intensity fluctuations is one mechanism of decoherence. To suppress the intensity noise of optical lattices, we implement an intensity stabilization control loop based on a field-programmable gate array (FPGA) digital platform (Keysight AIO-H3336F). With the advantages of its integratability and flexibility, the application of digital control opens more possibilities for light intensity modulation. In addition to the intensity stabilization, a feedforward control of light intensity becomes feasible with the use of digital signal processing function of FPGA. The realization of intensity feedforward control provides us with a high bandwidth of intensity modulation as well as the conveniences of creating arbitrary intensity ramp implementation. Therefore, it plays an important role in our exploration into the physics related with a time-varying optical trap depth.
This thesis reports on a novel concept of state-dependent transport, which achieves an unprecedented control over the position of individual atoms in optical lattices. Utilizing this control I demonstrate an experimental violation of the Leggett Garg inequality, which rigorously excludes (i.e. falsifies) any explanation of quantum transport based on classical, well-defined trajectories. Furthermore, I demonstrate the generation of arbitrary low-entropy states of neutral atoms following a bottom-up approach by rearranging a dilute thermal ensemble into a predefined, ordered distribution in a one-dimensional optical lattice. Additionally, I probe two-particle quantum interference effects of two atom trajectories by realizing a microwave Hong-Ou-Mandel interferometer with massive particles, which are cooled into the vibrational ground state.
The first part of this thesis reports on several new experimental tools and techniques: three-dimensional ground state cooling of single atoms, which are trapped in the combined potential of a polarization-synthesized optical lattice and a blue-detuned hollow dipole potential; A high-NA (0.92) objective lens achieving a diffraction limited resolution of 460 nm; and an improved super-resolution algorithm, which resolves the position of individual atoms in small clusters at high filling factors, even when each lattice site is occupied.
The next part is devoted to the conceptually new optical-lattice technique that relies on a high-precision, high-bandwidth synthesis of light polarization. Polarization-synthesized optical lattices provide two fully controllable optical lattice potentials, each of them confining only atoms in either one of the two long-lived hyperfine states. By employing one lattice as the storage register and the other one as the shift register, I provide a proof of concept that selected regions of the periodic potential can be filled with one particle per site.
In the following part I report on a stringent test of the non-classicality of the motion of a massive quantum particle, which propagates on a discrete lattice. Measuring temporal correlations of the position of single atoms performing a quantum walk, we observe a 6 σ (standard deviation) violation of the Leggett-Garg inequality. The experiment is carried out using so-called ideal negative measurements – an essential requisite for any genuine Leggett-Garg test – which acquire information about the atom’s position while avoiding any direct interaction with it. This interaction-free measurement is based on our polarization-synthesized optical lattice, which allows us to directly probe the absence rather than the presence of atoms at a chosen lattice site. Beyond its fundamental aspect, I demonstrate the application of the Leggett-Garg correlation function as a witness of quantum superposition. The witness allows us to discriminate the quantumness of different types of walks spanning from merely classical to quantum dynamics and further to witness the decoherence of a quantum state.
In the last experimental part I will discuss recent results on collisional losses due to inelastic collisions occurring at high two-atom densities and demonstrate a Hong-Ou-Mandel interference with massive particles. Our precise control over individual indistinguishable particles embodies a direct analogue of the original Hong-Ou-Mandel experiment. By carrying out a Monte Carlo analysis of our experimental data, I demonstrate a signature of the two-particle interference of two-atom trajectories with a statistical significance of 4 σ.
In the final part I will introduce several new experiments which can be realized with the tools and techniques developed in this thesis, spanning from the detection of topologically protected edge states to the prospect of building a one-million-operation quantum cellular automaton.
This thesis describes the development of an optical phase lock loop on a digital platform, in order to realize state-dependent transport on a two-dimensional optical lattice. The digital platform consists of a field programmable gate array in combination of a vector generator module, which is used to steer the amplitude and phase of the optical lattice deterministically. The digital system enables the implementation of a feedforward control scheme based on internal model control, which overcomes the bandwidth limitations of feedback systems. The control bandwidth is shown to be increased by more than an order of magnitude, directly improving the number of coherent operations that can be executed with the atoms in the optical lattice. The system is implemented into the optical setup of the experimental apparatus, and the first signatures of state-dependent transport of atoms in the two-dimensional optical lattice is observed and presented.
This master-thesis investigates a new approach for state-dependent transport of atoms in an optical lattice. It is based on a direct synthesis of light polarization by superimposing two circular polarized beams and employing RF sources integrated with acousto-optic modulators for phase control. An interferometrically stable phase between the two beams is achieved by locking them actively with a heterodyne technique. The influence of polarization crosstalk and erroneous components on the optical lattice and the phase locked loop are investigated and the quality of the phase locked loop is analyzed.
Compared to conventional methods [25] the direct synthesis method avoids the need of an electro-optic modulator, where rotations on the Poincare sphere are limited by the applicable voltage and restrictions on manufacturing and crystal quality exist. Overcoming these limitations it is expected to reach higher polarization purity and larger shift distances in the new design.