The average energy-pumping rate between two incommensurate drives is exactly one-half the topological quantized value at the drive-induced Dirac transition, with Kibble-Zurek scaling functions describing the crossover.
Dynamical Singularities of Floquet Higher-Order Topological Insulators
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abstract
We propose a versatile framework to dynamically generate Floquet higher-order topological insulators by multi-step driving of topologically trivial Hamiltonians. Two analytically solvable examples are used to illustrate this procedure to yield Floquet quadrupole and octupole insulators with zero- and/or $\pi$-corner modes protected by mirror symmetries. Furthermore, we introduce dynamical topological invariants from the full unitary return map and show its phase bands contain Weyl singularities whose topological charges form dynamical multipole moments in the Brillouin zone. Combining them with the topological index of Floquet Hamiltonian gives a pair of $\mathbb{Z}_2$ invariant $\nu_0$ and $\nu_\pi$ which fully characterize the higher-order topology and predict the appearance of zero- and $\pi$-corner modes. Our work establishes a systematic route to construct and characterize Floquet higher-order topological phases.
fields
cond-mat.mes-hall 1years
2019 1verdicts
CONDITIONAL 1representative citing papers
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Half-integer quantized topological response in quasiperiodically driven quantum systems
The average energy-pumping rate between two incommensurate drives is exactly one-half the topological quantized value at the drive-induced Dirac transition, with Kibble-Zurek scaling functions describing the crossover.