在空间上不均的逆法拉第效应提供可调节的交换主导的旋转波的非热激发
Denis M Krichevsky1,2, Vladislav A Ozerov1,2, Alexandra V Bel'kova1,3
1Russian Quantum Center, 143025, Skolkovo, Moscow Region, Russia.
Nanophotonics (Berlin, Germany)
|December 5, 2024
概括
我们展示了光如何激发磁光晶体中的自旋波. 调节光波长精确地控制哪些自旋波被激发,从而为自旋波设备提供了新的应用.
科学领域:
- 光学和光子学 在光学和光子学.
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
背景情况:
- 磁光子晶体结合了磁性和光子性质.
- 对自旋波的光学控制对于自旋电子学至关重要.
- 相反的法拉第效应调解了光旋相互作用.
研究的目的:
- 为了证明磁光子晶体中自旋波的光学非热刺激.
- 为了研究光子带间隙中光物质相互作用的作用.
- 通过波长控制探索调整旋转波激发效率.
主要方法:
- 用磁性薄膜和布拉格堆制造磁光学晶体.
- 利用相反的法拉第效应用于光学自旋波激发.
- 在光子带间隙内分析相反法拉第效应的相位滑动.
主要成果:
- 实现了各种顺序交换主导的自旋波的光学非热刺激.
- 在光子带间隙内观察到相反法拉第效应的明显相位滑动.
- 证明了不同自旋波顺序的波长可调节的激发效率.
结论:
- 该研究提供了一种用于光学控制磁光子晶体中自旋波的方法.
- 在光子带间隙内的相位滑动允许精确调整自旋波激发.
- 这种方法扩大了旋波设备中磁性介电物的应用.
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