This paper demonstrates a quadrupole topological insulator with zero-energy corner modes and a pair of edge polarizations. The authors also find that such topological phenomena can arise from quench dynamics in non-equilibrium systems.
Direct measurement of a bulk topological observable in topological phase of matter has been a long-standing issue. Recently, detection of bulk topology through quench dynamics has attracted growing interests. Here, we propose that topological characters of a quantum quadrupole insulator can be read out by quench dynamics. Specifically, we introduce a quantity, a quadrupole moment weighted by the eigenvalues of the chiral operator, which takes zero for the trivial phase and finite for the quadrupolar topological phase. By utilizing an efficient numerical method to track the unitary time evolution, we elucidate that the quantity we propose indeed serves as an indicator of topological character for both noninteracting and interacting cases. The robustness against disorders is also demonstrated.
The authors have discovered a topological classification of quantum many-body systems undergoing dynamical evolution, which can be applied to insulators and superconductors driven out of equilibrium. This classification is analogous to the equilibrium classification of topological insulators, which explains the remarkably quantized experimental signatures that these phases are known for. The nonequilibrium classification successfully predicts whether topological edge modes remain stable under external time-dependent fluctuations. This, in turn, has ramifications for the use of such systems in quantum technologies.
This article introduces a general and experimentally feasible protocol to engineer dynamic higher-order topological phases by periodically driving its static lower-order counterparts with a suitable discrete symmetry breaking Dirac mass perturbation. Realization of dynamic corner modes in 2D, protected by a quantized Floquet quadrupole moment, exemplifies this general protocol. Additionally, the authors show that corner modes leave their signature even in a quantum spin Hall insulator for a long time after a sudden quench, manifesting their topological nature through periodic appearances of partial and complete revival of the survival probability.
The quadrupole insulator is a well-known instance of higher-order topological insulators in two dimensions, which possesses midgap corner states in both the energy spectrum and entanglement spectrum. Here, by constructing and exploring a model Hamiltonian under a staggered Z2 gauge field that respects momentum-glide reflection symmetries, we surprisingly find a quadrupole insulator that lacks zero-energy corner modes in its energy spectrum, despite possessing a nonzero quadrupole moment. Remarkably, the existence of midgap corner modes is found in the entanglement spectrum. Since these midgap states cannot be continuously eliminated, the quadrupole insulator cannot be continuously transformed into a trivial topological insulator, thereby confirming its topological nature. We show that the breakdown of the correspondence between the energy spectrum and entanglement spectrum occurs due to the closure of the edge energy gap when the Hamiltonian is flattened. Finally, we present a model that demonstrates an insulator with corner modes in the energy spectrum even in the absence of the quadrupole moment. In this phase, the entanglement spectrum does not display any midgap states. The results suggest that the bulk-edge correspondence of quadrupole insulators generally manifests in the entanglement spectrum rather than the energy spectrum.