The work identifies topologically enforced Lifshitz multicritical points in 1D chiral symmetric fermions that host robust degeneracies and violate the Li-Haldane bulk-boundary correspondence.
Anomalous Dynamical Scaling at Topological Quantum Criticality
2 Pith papers cite this work. Polarity classification is still indexing.
abstract
We study the nonequilibrium driven dynamics at topologically nontrivial quantum critical points (QCPs), and find that topological edge modes at criticality give rise to anomalous dynamical scaling behavior. By analyzing the driven dynamics of bulk and boundary order parameters at topologically distinct QCPs in quantum spin chains, we demonstrate that, while the bulk dynamics remain indistinguishable and follow standard Kibble Zurek (KZ) scaling, the anomalous boundary dynamics are unique to topological criticality, obeying modified scaling relation beyond the traditional KZ framework. To elucidate the unified origin of this anomaly, we further study the dynamics of defect production at topologically distinct QCPs in free-fermion models and demonstrate similar anomalous scaling exclusive to topological criticality. These findings establish the existence of anomalous dynamical scaling arising from the interplay between topology and driven dynamics, challenging standard paradigms of quantum critical dynamics.
years
2026 2verdicts
UNVERDICTED 2representative citing papers
Closed quench paths through two critical points in generalized Creutz ladders produce ICDZM interference patterns that vanish or show period doubling when linking two topologically nontrivial phases, explained via WKB phase accumulation and detectable via boundary particle number deviation.
citing papers explorer
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Interference of critical dynamics associated with zero modes
Closed quench paths through two critical points in generalized Creutz ladders produce ICDZM interference patterns that vanish or show period doubling when linking two topologically nontrivial phases, explained via WKB phase accumulation and detectable via boundary particle number deviation.