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This study investigates the Aharonov-Casher effect in ultracold atoms, demonstrating how specific atom-light coupling configurations can engineer synthetic magnetic fields and flat energy bands suitable for simulating fractional Hall states. By analyzing deviations from ideal fine-tuning conditions, the authors provide a pathway to creating nearly perfect geometries essential for advanced quantum simulation protocols.
Aharonov-Casher Chern bands for ultracold dark state atoms
arXiv:2606.00207v2 Announce Type: replace-cross Abstract: We consider the Aharonov-Casher (AC) condition for ultracold atoms adiabatically following the dark-state in a $\Lambda$-type atom-light coupling scheme. The AC condition establishes a relation between the geometric scalar potential and the synthetic magnetic field, resulting in a fully degenerate lowest Landau-level-like band in the adiabatic limit even if the magnetic field is inhomogeneous but has a proper sign. We derive a general requirement for the atom-light coupling under which the AC condition applies. The requirement holds if the Rabi frequencies of the $\Lambda$ scheme are superpositions of plane waves with the appropriate amplitudes and phases. In particular, the Rabi frequencies made of $N=3,\,4,\,6$ fine tuned plane waves yield a smooth background magnetic field of definite sign, as well as an array of non-measurable Aharonov-Bohm flux singularities. Departing from the fine tuning, the latter singularities turn into narrow subwavelength patches of the magnetic field with an opposite sign, which broaden the lowest energy band. The lowest band is also broadened for the fine tuned situation due to deviation from the adiabatic approach because of the finite atom-light coupling strength. It is shown that a proper combination of the two imperfections (departure from fine tuning and finite atom-light coupling strength) can lead to a significant reduction of the width of the lowest band, which can be made almost completely flat and furthermore becomes characterized by a nearly perfect geometry needed for simulating the fractional Hall states.
Abstract:We consider the Aharonov-Casher (AC) condition for ultracold atoms adiabatically following the dark-state in a $\Lambda$-type atom-light coupling scheme. The AC condition establishes a relation between the geometric scalar potential and the synthetic magnetic field, resulting in a fully degenerate lowest Landau-level-like band in the adiabatic limit even if the magnetic field is inhomogeneous but has a proper sign. We derive a general requirement for the atom-light coupling under which the AC condition applies. The requirement holds if the Rabi frequencies of the $\Lambda$ scheme are superpositions of plane waves with the appropriate amplitudes and phases. In particular, the Rabi frequencies made of $N=3,\,4,\,6$ fine tuned plane waves yield a smooth background magnetic field of definite sign, as well as an array of non-measurable Aharonov-Bohm flux singularities. Departing from the fine tuning, the latter singularities turn into narrow subwavelength patches of the magnetic field with an opposite sign, which broaden the lowest energy band. The lowest band is also broadened for the fine tuned situation due to deviation from the adiabatic approach because of the finite atom-light coupling strength. It is shown that a proper combination of the two imperfections (departure from fine tuning and finite atom-light coupling strength) can lead to a significant reduction of the width of the lowest band, which can be made almost completely flat and furthermore becomes characterized by a nearly perfect geometry needed for simulating the fractional Hall states.
18 pages, 10 figures. v2 of manuscript
Quantum Gases (cond-mat.quant-gas); Mesoscale and Nanoscale Physics (cond-mat.mes-hall); Quantum Physics (quant-ph)
arXiv:2606.00207 [cond-mat.quant-gas]
(or arXiv:2606.00207v2 [cond-mat.quant-gas] for this version)
https://doi.org/10.48550/arXiv.2606.00207 Focus to learn more arXiv-issued DOI via DataCite
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