零频奇拉尔磁力边缘状态受到无平衡拓学的保护
Pieter M Gunnink1, Joren S Harms1, Rembert A Duine1,2
1Institute for Theoretical Physics and Center for Extreme Matter and Emergent Phenomena, Utrecht University, Leuvenlaan 4, 3584 CE Utrecht, The Netherlands.
Physical review letters
|October 6, 2023
概括
通常在高能量的拓磁子,可以在非平衡状态下在零频率下访问. 这一突破使未来设备能够直接激发和检测磁边缘状态.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子马格尼尼克斯 量子马格尼尼克斯
- 拓学材料 拓学材料
背景情况:
- 拓玻色子激发,像磁子,通常存在于有限的能量,阻碍他们的实验可访问性.
- 这种能源需求对在设备中利用拓保护的磁边缘状态构成了重大挑战.
研究的目的:
- 为了克服拓磁子的能量障碍.
- 为了实现实际应用,可以直接激发和检测磁边缘状态.
主要方法:
- 通过将磁化与外部磁场对齐,诱导一个不平衡状态.
- 利用旋转轨道扭矩来稳定这种独特的磁性配置.
- 执行数值兰道-利夫希茨-吉尔伯特模拟.
- 提出传播自旋波光谱法用于检测.
主要成果:
- 证明了在马格农切尔恩绝缘体中的拓性奇拉边缘状态可以降低到零频率.
- 表明这些零频边缘状态可以通过当前的实验技术直接访问.
- 使用微波场通过模拟确认了边缘状态的激发.
- 通过传播自旋波光谱学确定了直接检测的可行性.
结论:
- 在控制和访问拓巨子方面取得了重大进展.
- 拟议的方法通过使边缘状态随时可用,为磁设备开辟了新的途径.
- 这项工作弥合了理论预测和拓学磁力学实验实现之间的差距.
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