Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

nanoGe Fall Meeting

Simulation of Chiral Topological Phases in Driven Low Dimensional Systems

Gloria Platero

Published Jul 16, 2019• 0 citations
Publisher
DOI
10.29363/nanoge.ngfm.2019.317

Related papers

Simulation of Chiral Topological Phases in Driven Low Dimensional Systems

Gloria Platero

nanoGe Fall Meeting•Jul 18, 2019•0 citations

Topological phases in two-dimensional systems

Emmanuel V. C. Lopes

•Jul 18, 2025•0 citations

Phase-Modulated 2D Topological Physics in a One-Dimensional Ultracold System

Gang-Feng Guo, Xi-Xi Bao, Lei Tan +1 more

We propose a one-dimensional optical lattice model to simulate and explore two-dimensional topological phases with ultracold atoms, considering the phases of the hopping strengths as an extra dimension. It is shown that the model exhibits nontrivial phases, and corresponding two chiral-edge states. Moreover, we demonstrate the connections between changes in the topological invariants and the Dirac points. Furthermore, the topological order detected by the particle pumping approach in cold atoms is also investigated. The results obtained here provide a feasible and flexible method of simulating and exploring high-dimensional topological phases in low-dimension systems via the controllable phase of the hopping strength.

Chinese Physics Letters•May 1, 2021•3 citations

Detecting Topological Phases Through Dynamics of Chiral Density in Momentum-space Lattices

Rui Tian, Xiayao He, Tianhao Wu +3 more

•Jan 1, 2026•0 citations

Universal Fluctuations of Floquet Topological Invariants at Low Frequencies

Martin Rodriguez-Vega, Babak Seradjeh

We study the low-frequency dynamics of periodically driven one-dimensional systems hosting Floquet topological phases. We show, both analytically and numerically, in the low frequency limit Ω→0, the topological invariants of a chirally symmetric driven system exhibit universal fluctuations. While the topological invariants in this limit nearly vanish on average over a small range of frequencies, we find that they follow a universal Gaussian distribution with a width that scales as 1/sqrt[Ω]. We explain this scaling based on a diffusive structure of the winding numbers of the Floquet-Bloch evolution operator at low frequency. We also find that the maximum quasienergy gap remains finite and scales as Ω^{2}. Thus, we argue that the adiabatic limit of a Floquet topological insulator is highly structured, with universal fluctuations persisting down to very low frequencies.

arXiv:1706.05303•Physical Review Letters•Jul 18, 2018•49 citations

Numerical studies of topological quantum phase transitions in low dimensional systems

Yasuhiro Hatsugai

•May 31, 2004•0 citations
We propose a one-dimensional optical lattice model to simulate and explore two-dimensional topological phases with ultracold atoms, considering the phases of the hopping strengths as an extra dimension. It is shown that the model exhibits nontrivial phases, and corresponding two chiral-edge states. Moreover, we demonstrate the connections between changes in the topological invariants and the Dirac points. Furthermore, the topological order detected by the particle pumping approach in cold atoms is also investigated. The results obtained here provide a feasible and flexible method of simulating and exploring high-dimensional topological phases in low-dimension systems via the controllable phase of the hopping strength.
We study the low-frequency dynamics of periodically driven one-dimensional systems hosting Floquet topological phases. We show, both analytically and numerically, in the low frequency limit Ω→0, the topological invariants of a chirally symmetric driven system exhibit universal fluctuations. While the topological invariants in this limit nearly vanish on average over a small range of frequencies, we find that they follow a universal Gaussian distribution with a width that scales as 1/sqrt[Ω]. We explain this scaling based on a diffusive structure of the winding numbers of the Floquet-Bloch evolution operator at low frequency. We also find that the maximum quasienergy gap remains finite and scales as Ω^{2}. Thus, we argue that the adiabatic limit of a Floquet topological insulator is highly structured, with universal fluctuations persisting down to very low frequencies.