A theoretical protocol using Gaussian wave packets shows that initial momenta parallel and perpendicular to a boundary independently select counterpropagating edge modes in the anomalous Floquet valley-Hall phase.
Non-Abelian dynamical gauge field and topological superfluids in optical Raman lattice
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abstract
We propose an experimental scheme to realize non-Abelian dynamical gauge field for ultracold fermions, which induces a novel pairing mechanism of topological superfluidity. The dynamical gauge fields arise from nontrivial interplay effect between the strong Zeeman splitting and Hubbard interaction in a two-dimensional (2D) optical Raman lattice. The spin-flip transitions are forbidden by the large Zeeman detuning, but are restored when the Zeeman splitting is compensated by Hubbard interaction. This scheme allows to generate a dynamical non-Abelian gauge field that leads to a Dirac type correlated 2D spin-orbit interaction depending on local state configurations. The topological superfluid from a novel pairing driven by 2D dynamical gauge fields is reached, with analytic and numerical results being obtained. Our work may open up a door to emulate non-Abelian dynamical gauge fields and correlated topological phases with experimental feasibility.
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cond-mat.quant-gas 1years
2024 1verdicts
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Preparation and observation of anomalous counterpropagating edge states in a periodically driven optical Raman lattice
A theoretical protocol using Gaussian wave packets shows that initial momenta parallel and perpendicular to a boundary independently select counterpropagating edge modes in the anomalous Floquet valley-Hall phase.