arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2602.20458cond-mat.mes-hall
收藏

集成YIG纳米结构中的磁弹性转换

Magnetoelastic conversion in integrated YIG nanostructures

Delft University of Technology(代尔夫特理工大学);Institute of Magnetism of NAS and MOS of Ukraine(乌克兰国家科学院和教育部磁性研究所);RWTH Aachen University(亚琛工业大学);Max Planck Institute for the Science of Light(马克斯·普朗克光科学研究所);Luxembourg Institute of Science & Technology (LIST)(卢森堡科学与技术研究所);Université Grenoble Alpes(格勒诺布尔阿尔卑斯大学);CEA(法国原子能和替代能源委员会);CNRS(法国国家科学研究中心);Grenoble INP(格勒诺布尔理工学院);Spintec(自旋电子学与技术中心);WPI-AIMR, Tohoku University(东北大学世界顶尖科学研究学院);University of the Chinese Academy of Sciences(中国科学院大学)

Artem V. Bondarenko, Fabian Engelhardt, Marios Kounalakis, Thierry Valet, Olivier Klein, Gerrit E. W. Bauer, Silvia Viola Kusminskiy, Yaroslav M. Blanter

AI总结:

本研究通过优化YIG环结构参数,实现了磁弹性模式的高效共振耦合,为可调频率转换器件的设计提供了新途径。

摘要:

受最近通过磁性和弹性中间阶段将微波转换为光学域的两步转换方案arXiv:2205.05088的启发,我们考虑在一种简单的轴对称纳米器件中的共振磁性和弹性模式的耦合,该器件设计用于容纳高品质因子的声学模式:一个由连续单晶薄膜制成的悬空YIG环结构,支撑在中央杆上。我们使用自定义的有限元求解器研究该系统的模式。我们识别出磁性涡旋的最低阶“呼吸”模式和最低阶弹性呼吸模式具有最大的模式重叠。对于这对模式,外部垂直磁偏置场对于使它们共振是至关重要的;然而,我们表明同时它也影响耦合强度。为了克服这一点,我们优化了环的半径,保持厚度固定。对于100纳米厚的薄膜,共振耦合在g/2π=8MHz时达到最大值,当R≈1.7μm时,表明重叠积分接近之前顺序数量级估计所假设的理想极限。我们的结果为基于磁弹性的可调频率转换器件的设计铺平了道路。

英文摘要:

Motivated by the recent proposal of two-step transduction from microwave to optical domain using magnetic and elastic intermediate stages arXiv:2205.05088, we consider the coupling between resonant magnetic and elastic modes within a simple axially-symmetric nanodevice designed to host high-quality-factor acoustic modes: A suspended YIG ring structure supported by a central stem, fabricated from a continuous single-crystal film. We study the modes of the system with our custom finite element solvers. We identify the lowest order ``breathing'' mode of a magnetic vortex and the lowest order elastic breathing mode as having the largest mode overlap. For this pair of modes, the external out-of-plane magnetic bias field is critical for bringing them into resonance; however, we show that at the same time it also affects the strength of the coupling. To counteract this, we optimize the radius of the ring at fixed thickness. For the 100 nm-thick film the resonant coupling is maximized at $g/2π= 8\text{MHz}$ at $R\approx1.7μ\text{m}$, indicating that the overlap integral approaches the idealized limit assumed in previous order-of-magnitude estimates. Our results pave the way for the design of tunable frequency-conversion devices based on magnetoelastics.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑