Critical States Generators from Perturbed Flatbands
arXiv:2304.05769 · doi:10.1063/5.0153819
Abstract
One-dimensional all-bands-flat lattices are networks with all bands being flat and highly degenerate. They can always be diagonalized by a finite sequence of local unitary transformations parameterized by a set of angles \(θ_{i}\). In our previous work, Ref.~\onlinecite{lee2023critical}, we demonstrated that quasiperiodic perturbations of the one-dimensional all-bands-flat lattice with \(θ_{i} = π/4\) give rise to a critical-to-insulator transition and fractality edges separating critical from localized states. In this study we consider the full range of angles \(θ_{i}\)s available for the all-bands-flat model and study the effect of the quasiperiodic perturbation. For weak perturbation, we derive an effective Hamiltonian and we identify the sets of \(θ_{i}\)s for which the effective model maps to extended or off-diagonal Harper models and hosts critical states. For all the other values of the angles the spectrum is localized. Upon increasing the perturbation strength, the extended Harper model evolves into the system with energy dependent critical-to-insulator transitions, that we dub \emph{fractality edges}. The case where the effective model maps onto the off-diagonal Harper model features a critical-to-insulator transition at a finite disorder strength.
arXiv comment8 pages, 6 figures, 1 table
References in corpus (41)
- Magic-angle graphene superlattices: a new platform for unconventional superconductivity
- Anderson Transitions
- Artificial flat band systems: from lattice models to experiments
- Direct observation of a localization transition in quasi-periodic photonic lattices
- Aharonov-Bohm cages in two-dimensional structures
- Topological Equivalence between the Fibonacci Quasicrystal and the Harper Model
- Strongly correlated flat-band systems: The route from Heisenberg spins to Hubbard electrons
- Detangling Flat Bands into Fano Lattices
- End states, ladder compounds, and domain wall fermions
- Interaction induced delocalisation for two particles in a periodic potential
- How to escape Aharonov-Bohm cages ?
- Hofstadter butterflies for flat bands
- Critical and bicritical properties of Harper's equation with next nearest neighbor coupling
- Preformed pairs in flat Bloch bands
- Observation of interaction-induced mobility edge in a disordered atomic wire
- Flat Band Quantum Scar
- Phase diagram and pair Tomonaga-Luttinger liquid in a Bose-Hubbard model with flat bands
- Geometry induced pair condensation
- Flat-band many-body localization and ergodicity breaking in the Creutz ladder
- Topological circuits of inductors and capacitors
- Flat-Band Ferromagnetism as a Pauli-Correlated Percolation Problem
- Topological Creutz Ladder in a Resonantly Shaken 1D Optical Lattice
- Many-Body Flatband Localization
- Aharonov-Bohm Caging and Inverse Anderson transition in Ultracold Atoms
- Universal flatband generator from compact localized states
- Flat-band localization in Creutz superradiance lattices
- Nonlinear dynamics of Aharonov-Bohm cages
- Nonlinear caging in All-Bands-Flat Lattices
- Spectral theory of extended Harper's model and a question by Erdős and Szekeres
- Quantum Caging in Interacting Many-Body All-Bands-Flat Lattices
- Interaction-induced topological properties of two bosons in flat-band systems
- Nonlinear symmetry breaking of Aharonov-Bohm cages
- Arithmetic Spectral Transitions for the Maryland Model
- Inverse Anderson transition in photonic cages
- Critical-to-Insulator Transitions and Fractality Edges in Perturbed Flatbands
- Interaction induced doublons and embedded topological subspace in a complete flat-band system
- Observation of inverse Anderson transitions in Aharonov-Bohm topolectrical circuits
- Influence of different disorder types on Aharonov-Bohm caging in the diamond chain
- Metal-insulator transition in infinitesimally weakly disordered flatbands
- Many-body localization transition from flatband fine-tuning
- Signatures of many-body localization of quasiparticles in a flat band superconductor