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基于双稳性的全磁子中继器。

All-magnonic repeater based on bistability.

作者信息

Wang Qi, Verba Roman, Davídková Kristýna, Heinz Björn, Tian Shixian, Rao Yiheng, Guo Mengying, Guo Xueyu, Dubs Carsten, Pirro Philipp, Chumak Andrii V

机构信息

School of Physics, Huazhong University of Science and Technology, Wuhan, China.

Institute of Magnetism, Kyiv, Ukraine.

出版信息

Nat Commun. 2024 Aug 31;15(1):7577. doi: 10.1038/s41467-024-52084-0.

Abstract

Bistability, a universal phenomenon found in diverse fields such as biology, chemistry, and physics, describes a scenario in which a system has two stable equilibrium states and resets to one of the two states. The ability to switch between these two states is the basis for a wide range of applications, particularly in memory and logic operations. Here, we present a universal approach to achieve bistable switching in magnonics, the field processing data using spin waves. A pronounced bistable window is observed in a 1 μm wide magnonic conduit under an external rf drive. The system is characterized by two magnonic stable states defined as low and high spin-wave amplitude states. The switching between these two states is realized by another propagating spin wave sent into the rf driven region. This magnonic bistable switching is used to design a magnonic repeater, which receives the original decayed and distorted spin wave and regenerates a new spin wave with amplified amplitude and normalized phase. Our magnonic repeater can be installed at the inputs of each magnonic logic gate to overcome the spin-wave amplitude degradation and phase distortion during previous propagation and achieve integrated magnonic circuits or magnonic neuromorphic networks.

摘要

双稳态是在生物学、化学和物理学等不同领域中发现的一种普遍现象,它描述了一个系统具有两个稳定平衡态并重置为这两个状态之一的情形。在这两个状态之间进行切换的能力是广泛应用的基础,特别是在存储器和逻辑运算中。在此,我们提出一种在磁振子学中实现双稳态切换的通用方法,磁振子学是利用自旋波处理数据的领域。在外部射频驱动下,在一个1微米宽的磁振子管道中观察到明显的双稳态窗口。该系统的特征在于两个磁振子稳定态,定义为低自旋波幅度态和高自旋波幅度态。这两个状态之间的切换是通过发送到射频驱动区域的另一个传播自旋波来实现的。这种磁振子双稳态切换被用于设计一个磁振子中继器,它接收原始衰减和失真的自旋波,并再生一个具有放大幅度和归一化相位的新自旋波。我们的磁振子中继器可以安装在每个磁振子逻辑门的输入端,以克服先前传播过程中自旋波幅度衰减和相位失真的问题,并实现集成磁振子电路或磁振子神经形态网络。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/7814/11365973/0deb82c68411/41467_2024_52084_Fig1_HTML.jpg

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