In recent years, there has been a growing interest in flatband systems which exhibit macroscopic degeneracies. These systems offer a valuable mathematical framework for the extreme sensitivity to perturbations and interactions. This sensitivity unveils a wide variety of exotic and unconventional physical phenomena. Moreover, the progress in their experimental realization contributes to the expanding landscape of exploration in this field. This thesis aims to summarize all the works throughout the Ph.D. program. Firstly, an in-depth exploration was conducted on the impact of weak quasiperiodic perturbations on one-dimensional two-band all-bands-flat lattices. These tight-binding Hamiltonian are diagonalized through a sequence of local unitary transformations. By adjusting the quasiperiodic potential parameters, the key achievement involves finding a critical-to-insulator transition and identifying fractality edges in the flatband systems with quasiperiodic perturbations. Next, the investigation delved into the effects of on-site interactions among hard-core bosons in one- and two-dimensional cross-stitch lattices. One key finding is that groundstate energy primarily depends on compact localized states. Moreover, the presence of barriers of compact localized states trap bosons, leading to the emergence of non-ergodic excitation and Hilbert space fragmentation. Lastly, a compact localized eigenstate of the one-dimensional diamond chain using an electric circuit was successfully generated via local (linear and non-linear) driving. This achievement opens up a versatile circuit platform for the generation of flatbands and holds promise for potential applications in the field of quantum information. I hope these collective efforts have expanded the frontiers of the field and made a meaningful contribution to the scientific community.
In recent years, there has been a growing interest in flatband systems which exhibit macroscopic degeneracies. These systems offer a valuable mathematical framework for the extreme sensitivity to perturbations and interactions. This sensitivity unveils a wide variety of exotic and unconventional physical phenomena. Moreover, the progress in their experimental realization contributes to the expanding landscape of exploration in this field. This thesis aims to summarize all the works throughout the Ph.D. program. Firstly, an in-depth exploration was conducted on the impact of weak quasiperiodic perturbations on one-dimensional two-band all-bands-flat lattices. These tight-binding Hamiltonian are diagonalized through a sequence of local unitary transformations. By adjusting the quasiperiodic potential parameters, the key achievement involves finding a critical-to-insulator transition and identifying fractality edges in the flatband systems with quasiperiodic perturbations. Next, the investigation delved into the effects of on-site interactions among hard-core bosons in one- and two-dimensional cross-stitch lattices. One key finding is that groundstate energy primarily depends on compact localized states. Moreover, the presence of barriers of compact localized states trap bosons, leading to the emergence of non-ergodic excitation and Hilbert space fragmentation. Lastly, a compact localized eigenstate of the one-dimensional diamond chain using an electric circuit was successfully generated via local (linear and non-linear) driving. This achievement opens up a versatile circuit platform for the generation of flatbands and holds promise for potential applications in the field of quantum information. I hope these collective efforts have expanded the frontiers of the field and made a meaningful contribution to the scientific community.
In this thesis I study the topological properties exhibited in cold atom systems trapped in periodic and finite-size one-dimensional potentials. Ultracold atoms provide an excellent platform for exploring various many-body quantum models that are challenging to identify in traditional condensed matter systems. In particular, recent advancements in experimental cold atom physics have enabled the creation of subwavelength nanoscale potentials, making it possible to realize the Kronig-Penney model and its variations. One of these considers shifting a regular lattice of point-like barriers within a finite-sized box, which allows topologically protected edge states to emerge as a function of the shift parameter. The continuous shift parameter then provides a virtual dimension and the system becomes effectively two-dimensional, allowing topological states to be explored over a large and flexible parameter space. In my work I go beyond the standard singleparticle treatment of topological system and analyze the equilibrium and non-equilibrium physics of fermionic and bosonic many-body systems. The first project I present focuses on the non-equilibrium dynamics of a ground-state fermionic many-body gas following a quench between different lattice shift parameters that allow for edge states with different chirality. I examine the role of the single-particle chiral edge states in the non-equilibrium dynamics of the system and demonstrate that the usual monotonic decay associated with the orthogonality catastrophe, typically observed with increasing system size, is significantly altered. The second study explores the topological characteristics of a system of two interacting particles in the Kronig-Penney-type nanoscale potential and examines the appearance of two-particle topological states within the spectrum. This investigation is extended to the Rice-Mele model, where similar topological features are observed. Finally, the third study considers the optical realization of a height-modulated nanoscale potential, which generates a complex potential landscape. To probe the many-body properties of such a system, I examined the spectral function of a Tonks–Girardeau gas in a quasiperiodically modulated KP potential. By varying the modulation amplitude and frequency, I identified a transition between delocalized and localized single-particle eigenstates. In the localized regime, the spectral function shows flat, non-dispersive modes that reflect localized states, whereas in the delocalized regime it becomes continuous and dispersive.
This PhD thesis is devoted to explore non-local orders in low-dimensional Hubbard-like systems. This kind of systems plays a crucial role in condensed matter physics. They were originally introduced to model solid state materials and, indeed, they successfully describe many observed physical phenomena. Additionally, in last decades, their scientific interest has exponentially increased thanks to the experiments with cold atoms, which have opened the opportunity to simulate and manipulate this type of lattice models. Trapping ultracold atomic gases into an optical lattice potential provides the purest realization of Hubbard Hamiltonians. Most important, the high control on the parameters involved allows to achieve even new fascinating regimes, among them exotic phases occurring in one and two spatial dimensions. These investigations are extremely interesting, since they unveil a totally novel physics, with many potential applications. On the other hand, from the theoretical point of view, Landau developed a theory that classifies possible phases of matter according to their symmetry. These are called spontaneous symmetry breaking phases and are typically identified by a local order parameter. Nevertheless, recent researches have proven that many more phases may exist in quantum systems. These are often called non-symmetry-breaking, hidden, exotic or topological phases. Hidden phases can be revealed by non-local order parameters. Given their central task in this attractive scenario, here we undertake to provide an overview on the capability of non-local order parameters to detect fully or partly gapped quantum phases and capture their essential microscopic features. To this end, we study their behavior, both analytically and numerically, in different systems. First of all we show that they can probe a large variety of one-dimensional quantum phases, actually all of them in the kind of Hamiltonians we will consider. Then, we will use them to uncover possible new phases and, finally, we will successfully attempt a generalization to the two dimensional case. Our results supply a step forward in the comprehension of this valuable tool and its range of applicability, in addition to the information we managed to disclose about the physical systems we studied, thanks to their employment.
We highlight recent progress in the study of artificial flat band systems with a threefold focus. First, we discuss single-particle flat band physics, which has advanced through the design of various flat band generators. These generators rely on the classification of flat bands in terms of compact localized states - their fundamental building blocks. A related development is the complete real-space description of flat band projectors. Next, we review studies on perturbations of flat bands, which provide new insights into the effects of disorder and, more importantly, the intricate interplay between many-body interactions and flat band physics. Finally, we survey the growing number of experimental realizations of flat bands across diverse physical platforms.
We highlight recent progress in the study of artificial flat band systems with a threefold focus. First, we discuss single-particle flat band physics, which has advanced through the design of various flat band generators. These generators rely on the classification of flat bands in terms of compact localized states – their fundamental building blocks. A related development is the complete real-space description of flat band projectors. Next, we review studies on perturbations of flat bands, which provide new insights into the effects of disorder and, more importantly, the intricate interplay between many-body interactions and flat band physics. Finally, we survey the growing number of experimental realizations of flat bands across diverse physical platforms.
We study the effect of quasiperiodic perturbations on one-dimensional all-bands-flat lattice models. Such networks can be diagonalized by a finite sequence of local unitary transformations parameterized by angles ${\ensuremath{\theta}}_{i}$. Without loss of generality, we focus on the case of two bands with bandgap $\mathrm{\ensuremath{\Delta}}$. Weak perturbations lead to an effective Hamiltonian with both on- and off-diagonal quasiperiodic terms that depend on ${\ensuremath{\theta}}_{i}$. For some angle values, the effective model coincides with the extended Harper model. By varying the parameters of the quasiperiodic potentials, we observe localized insulating states and an entire parameter range hosting critical states with subdiffusive transport. For finite quasiperiodic potential strength, the critical-to-insulating transition becomes energy dependent with what we term fractality edges separating localized from critical states.
In this thesis, we discuss quantum phase transitions in low-dimensional optical lattices, namely one- and two-dimensional lattices. The dimensional confinement is realized in experiments by suppressing the hopping in the extra dimensions through a deep potential barrier that prevents the atoms to tunnel across dimensions. The dimensionality considerably affects the physical behavior of the system. For instance, in one dimension, the celebrated Fermi-liquid theory does not describe the many-body behavior of a fermionic system. There are no single particle excitations, but instead collective behavior, and spin and charge degrees of freedom are decoupled . In the first part of this thesis, we consider one-dimensional fermionic gases under the effect of time-dependent driving forces. First, we describe a proposal to realize non-standard Hubbard models that display correlated-hopping terms by modulating interactions through a time-dependent magnetic field. The extra terms describe hopping processes that depend on the particle-density difference in neighboring sites. The effective model is obtained in arbitrary spatial dimensions, but only in one-dimension it is known to be exactly solvable for specific values of the parameters. Moreover, an SU(2) symmetry in the charge sector allows to construct non-trivial superconducting eigenstates (eta-states), discovered by Yang as excited states of the Hubbard model. Then, we study a one-dimensional bipartite optical lattice with fermionic atoms at half-filling. The lattice potential barriers have heights alternating in magnitude. As a consequence, the hopping amplitudes also alternate in magnitude and the elementary unit cell has two sites. This system is known to display Peierls dimerization at half-filling: the fermions form dimers in neighboring sites that inhibit transport and open a gap in the spectrum. After applying shaking on this system we discover that one can dynamically induce a phase transition to an unconventional metallic state with four Fermi-points. The second part of this thesis describes bosonic systems in two-dimensional optical lattices. First, we consider a square optical lattice with alternating deep-shallow wells arranged in a checkerboard pattern. This lattice is realized in the experimental laboratory of Prof. Hemmerich in Hamburg. In the experiment, the visibility is extracted from the time-of-flight imaging to quantify the phase coherence of the bosonic gas. We develop a mean-field theory and determine the phase diagram of this model. We interpret the experimental data by assuming that at large detuning, only the deeper wells are populated and form an imbalanced Mott insulator with empty shallow wells and integer density on the deeper wells. We support this hypothesis by large-scale Gutzwiller calculations. Then, we investigate a system of bosons in the Lieb lattice, which is the lattice geometry of the Cu-O plane in cuprates . We consider configurations of the optical potential where s and p orbitals sitting on neighboring wells become resonant and hybridize. The interest in this problem comes from the possibility to realize time-reversal broken phases, usually known as Varma phases for electronic systems, which have been proposed to explain the pseudo-gap regime of cuprate superconductors. We show the conditions under which the symmetry breaking in a four-band model can lead to states with loop currents. Moreover, the lowest branch of the excitation spectrum has a non-vanishing Chern number and therefore supports topological excitations.