pith:3M53OGF2
Quantized Transport in Floquet Topological Insulators
Floquet topological systems show quantized longitudinal and Hall conductances set by the winding invariant once all sideband contributions are summed.
arxiv:2605.13066 v1 · 2026-05-13 · cond-mat.mes-hall · cond-mat.stat-mech · quant-ph
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Claims
Using the Floquet nonequilibrium Green's-function (NEGF) formalism we show, from exact numerics for a strip geometry, that the two-terminal (longitudinal) conductance is quantized as |W_ε| e²/h, while the Hall (transverse) conductance is quantized as W_ε e²/h, where W_ε is the Floquet winding invariant associated with the quasienergy gap at ε = 0 or ε = Ω/2.
Quantization holds only after summing over the contribution of all Floquet sidebands; the analytic proof is restricted to the weak-coupling limit to the reservoirs.
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.
References
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| First computed | 2026-05-18T03:08:58.974120Z |
|---|---|
| Builder | pith-number-builder-2026-05-17-v1 |
| Signature | Pith Ed25519
(pith-v1-2026-05) · public key |
| Schema | pith-number/v1.0 |
Canonical hash
db3bb718bad41e37b723780f0339aa982d058ec0d29fe622fdb3a45964f7fe43
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Canonical record JSON
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