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Bulletin of the American Physical Society

Quench dynamics of a spinor condensate with strong spin-dependent interactions

Hil Fung Harry Cheung, Yogesh Sharad Patil, Mukund Vengalattore

Published Jun 8, 2017• 0 citations
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arXiv:1909.00681•Physical Review A•Feb 20, 2020•7 citations
We present an experimental study on nonequilibrium dynamics of a spinor condensate after it is quenched across a superfluid to Mott insulator (MI) phase transition in cubic lattices. Intricate dynamics consisting of spin-mixing oscillations at multiple frequencies are observed in time evolutions of the spinor condensate localized in deep lattices after the quantum quench. Similar spin dynamics also appear after spinor gases in the MI phase are suddenly moved away from their ground states via quenching magnetic fields. We confirm these observed spectra of spin-mixing dynamics can be utilized to reveal atom number distributions of an inhomogeneous system, and to study transitions from two-body to many-body dynamics. Our data also imply the nonequilibrium dynamics depend weakly on the quench speed but strongly on the lattice potential. This enables precise measurements of the spin-dependent interaction, a key parameter determining the spinor physics.
We investigate the early-time dynamics of a quasi-two-dimensional spin-1 antiferromagnetic Bose-Einstein condensate after a sudden quench from the easy-plane to the easy-axis polar phase. The postquench dynamics shows a crossover behavior as the quench strength $\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{q}$ is increased, where $\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{q}$ is defined as the ratio of the initial excitation energy per particle to the characteristic spin interaction energy. For a weak quench of $\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{q}<1$, long-wavelength spin excitations are dominantly generated, leading to the formation of irregular spin domains. With increasing $\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{q}$, the length scale of the initial spin excitations decreases, and we demonstrate that the long-wavelength instability is strongly suppressed for high $\stackrel{\ifmmode \tilde{}\else \~{}\fi{}}{q}>2$. The observed crossover behavior is found to be consistent with the Bogoliubov description of the dynamic instability of the initial spinor condensate.