在韦尔激发性绝缘体中,Axion电动力学和巨大的磁双断率
A A Grigoreva1, A V Andreev1, L I Glazman2
1University of Washington, Department of Physics, Seattle, Washington 98195, USA.
Physical review letters
|December 5, 2025
概括
我们发现,韦尔半金属中的莱格特模式充当了巨大的动态动力. 这种与电磁场的轴轴合会导致巨大的异构极化和双折射,特别是在磁场下.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子材料 量子材料是一种量子材料.
- 粒子物理学 粒子物理学
背景情况:
- 韦尔半金属 (WSMs) 由于其带结构,具有独特的电子特性.
- 激发性绝缘体相可以在低温下在WSM中出现.
- 时间逆转 (TR) 对称性在WSM电子相中起着至关重要的作用.
研究的目的:
- 在TR不变的WSM中研究激电绝缘器相的电磁反应.
- 描述这个系统中形成的莱格特模式的属性.
- 探索Leggett模式和axion物理之间的联系.
主要方法:
- 在WSM中激发性绝缘分离器阶段的理论分析.
- 通过约瑟夫森道研究凝结物的合.
- 研究性异常和性磁力效应的作用.
主要成果:
- 在低温下形成两个TR-对称的激子凝聚物.
- 由于约瑟夫森在凝结物之间进行了道化,出现了一个空隙的莱格特模式.
- 莱杰特模式与电磁场结合为一个巨大的动态动力.
结论:
- 莱杰特模式在WSM激发性绝缘体中表现为一个动态的动力.
- 这种类似于轴的行为导致了巨大的异性极化性和磁场中的双折射.
- 光子-轴子杂交导致在轴子间隙附近的极子子共振.
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