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淬火自旋轨道耦合简并费米气体中的动力学相。

Dynamical phases in quenched spin-orbit-coupled degenerate Fermi gas.

机构信息

Department of Physics, Hangzhou Normal University, Hangzhou, Zhejiang 310036, China.

Department of Physics and Astronomy, Rice Quantum Institute, Rice University, Houston, Texas 77251-1892, USA.

出版信息

Nat Commun. 2015 Jan 20;6:6103. doi: 10.1038/ncomms7103.

Abstract

The spin-orbit-coupled degenerate Fermi gas provides a new platform for realizing topological superfluids and related topological excitations. However, previous studies have been mainly focused on the topological properties of the stationary ground state. Here, we investigate the quench dynamics of a spin-orbit-coupled two-dimensional Fermi gas in which the Zeeman field serves as the major quench parameter. Three post-quench dynamical phases are identified according to the asymptotic behaviour of the order parameter. In the undamped phase, a persistent oscillation of the order parameter may support a topological Floquet state with multiple edge states. In the damped phase, the magnitude of the order parameter approaches a constant via a power-law decay, which may support a dynamical topological phase with one edge state at the boundary. In the overdamped phase, the order parameter decays to zero exponentially although the condensate fraction remains finite. These predictions can be observed in the strong-coupling regime.

摘要

自旋轨道耦合简并费米气体为实现拓扑超流和相关拓扑激发提供了新的平台。然而,以前的研究主要集中在静止基态的拓扑性质上。在这里,我们研究了在塞曼场作为主要淬火参数的情况下,二维自旋轨道耦合费米气体的淬火动力学。根据序参量的渐近行为,确定了三个后淬火动力学相。在无阻尼相中,序参量的持续振荡可能支持具有多个边缘态的拓扑 Floquet 态。在阻尼相中,序参量的大小通过幂律衰减趋近于常数,这可能支持具有一个边界边缘态的动力学拓扑相。在过阻尼相中,尽管凝聚分数仍然有限,但序参量指数衰减为零。这些预测可以在强耦合情况下观察到。

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