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Engineering topological chiral transport in a flat-band lattice of ultracold atoms

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arxiv 2401.03611 v1 pith:5ZQSCKXN submitted 2024-01-07 cond-mat.quant-gas cond-mat.mes-hallphysics.atom-ph

classification cond-mat.quant-gascond-mat.mes-hallphysics.atom-ph
keywords transportflat-bandchiralfluxsynthetictopologicalatomsdesign
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abstract

The manipulation of particle transport in synthetic quantum matter is an active research frontier for its theoretical importance and potential applications. Here we experimentally demonstrate an engineered topological transport in a synthetic flat-band lattice of ultracold $^{87}$Rb atoms. We implement a quasi-one-dimensional rhombic chain with staggered flux in the momentum space of the atomic condensate and observe biased local oscillations that originate from the interplay of the staggered flux and flat-band localization under the mechanism of Aharonov-Bohm caging. Based on these features, we design and experimentally confirm a state-dependent chiral transport under the periodic modulation of the synthetic flux. We show that the phenomenon is topologically protected by the winding of the Floquet Bloch bands of a coarse-grained effective Hamiltonian. The observed chiral transport offers a strategy for efficient quantum device design where topological robustness is ensured by fast Floquet driving and flat-band localization.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Observation of Higher-order Topological Bound States in the Continuum using Ultracold Atoms

    cond-mat.quant-gas 2025-01 conditional novelty 6.0 of 10

    Ultracold 87Rb atoms in a programmable 2D momentum lattice realize a 2D SSH model and show the dynamics of higher-order topological bound states in the continuum.

  2. Magnetic Field Induced Band Deformation in a Lieb Lattice:Aharonov-Bohm Caging and Zeeman Splitting

    cond-mat.quant-gas 2025-08 reject novelty 2.0 of 10

    Spin-resolved flat bands in a magnetized Lieb lattice are simply the zero-field bands shifted by ±Bz, because the Hamiltonian is block diagonal in spin.

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