In Floquet topological systems the two-terminal conductance quantizes to |W_ε| e²/h and the Hall conductance to W_ε e²/h after summing all Floquet sidebands, where W_ε is the winding invariant of the quasienergy gap.
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Floquet engineering via quantum resonances in periodically driven rotors enables analytical control of tight-binding parameters in momentum-space lattices, experimentally realized with a Bose-Einstein condensate to simulate the Rice-Mele model and related configurations.
Periodic driving of the generalized Aubry-André model produces controllable delocalized-localized and multifractal-localized Floquet mobility edges with corresponding superdiffusive to subdiffusive transport.
Tuning the angle between sites in an OAM l=1 staggered lattice switches the winding number and number of topologically protected edge states in a Creutz-ladder mapping.
Kibble-Zurek defect scaling does not generally correspond to quantum criticality in representative quasi-1D Fermi models.
citing papers explorer
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Quantized Transport in Floquet Topological Insulators
In Floquet topological systems the two-terminal conductance quantizes to |W_ε| e²/h and the Hall conductance to W_ε e²/h after summing all Floquet sidebands, where W_ε is the winding invariant of the quasienergy gap.
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Floquet engineering of tight-binding Hamiltonians in momentum space lattices
Floquet engineering via quantum resonances in periodically driven rotors enables analytical control of tight-binding parameters in momentum-space lattices, experimentally realized with a Bose-Einstein condensate to simulate the Rice-Mele model and related configurations.
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Floquet mobility edges and transport in a periodically driven generalized Aubry-Andr\'e model
Periodic driving of the generalized Aubry-André model produces controllable delocalized-localized and multifractal-localized Floquet mobility edges with corresponding superdiffusive to subdiffusive transport.
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Geometrical control of topology with orbital angular momentum modes
Tuning the angle between sites in an OAM l=1 staggered lattice switches the winding number and number of topologically protected edge states in a Creutz-ladder mapping.
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Separation of the Kibble-Zurek Mechanism from Quantum Criticality
Kibble-Zurek defect scaling does not generally correspond to quantum criticality in representative quasi-1D Fermi models.