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旋转腔光磁学中的非互易对称磁振子激光器。

Nonreciprocal -symmetric magnon laser in spinning cavity optomagnonics.

作者信息

Wang Zheng-Yang, He Xiao-Wei, Han Xue, Wang Hong-Fu, Zhang Shou

出版信息

Opt Express. 2024 Feb 12;32(4):4987-4997. doi: 10.1364/OE.513536.

Abstract

We propose a scheme to achieve nonreciprocal parity-time ( )-symmetric magnon laser in a -symmetric cavity optomagnonical system. The system consists of active and passive optical spinning resonators. We demonstrate that the Fizeau light-dragging effect induced by the spinning of a resonator results in significant variations in magnon gain and stimulated emitted magnon numbers for different driving directions. We find that utilizing the Fizeau light-dragging effect allows the system to operate at ultra-low thresholds even without reaching gain-loss balance. A one-way magnon laser can also be realized across a range of parameters. High tunability of the magnon laser is achieved by changing the spinning speed of the resonators and driving direction. Our work provides a new way to explore various nonreciprocal effects in non-Hermitian magnonic systems, which may be applied to manipulate photons and magnons in multi-body non-Hermitian coupled systems.

摘要

我们提出了一种在 -对称腔光磁系统中实现非互易宇称 - 时间( )对称磁振子激光器的方案。该系统由有源和无源光学自旋谐振器组成。我们证明,谐振器的自旋所诱导的斐索光拖曳效应会导致不同驱动方向下磁振子增益和受激发射磁振子数的显著变化。我们发现,利用斐索光拖曳效应可使系统即使在未达到增益 - 损耗平衡的情况下也能在超低阈值下运行。在一系列参数范围内还可实现单向磁振子激光器。通过改变谐振器的自旋速度和驱动方向可实现磁振子激光器的高可调谐性。我们的工作为探索非厄米磁振子系统中的各种非互易效应提供了一种新方法,这可能应用于多体非厄米耦合系统中对光子和磁振子的操控。

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