通过电磁波动介导的单位内细胞单元配对.
Yi-Ming Wu1, Yuxuan Wang2, Rafael M Fernandes3,4
1Stanford University, Leinweber Institute for Theoretical Physics, Stanford, California 94305, USA.
变磁波动驱动超导,有利于基于波动范围的独特配对状态. 较短范围的波动会诱导单元细胞内部的配对,而较长范围的波动会稳定旋转三重p波状态.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子材料是一种量子材料.
- 超导电性 超导电性 超导电性
背景情况:
- 变磁,一种新的磁性秩序,呈现出独特的电子特性.
- 了解磁波动对于预测超导不稳定性至关重要.
- 亚晶格结构在变磁诱导的超导性中的作用仍未得到充分研究.
研究的目的:
- 研究由变磁波动驱动的超导不稳定性.
- 确定变磁秩序对配对对称性的影响.
- 探索从变磁性-超导性共存中出现的拓性质.
主要方法:
- 对变磁波动的理论分析.
- 研究库珀配对机制.
- 探索拓不变量及其符号.
主要成果:
- 短距离的变磁波动稳定了单元细胞内部的配对 (s波,p波,d波).
- 较长范围的波动有利于标准的旋转三重波 p 波配对.
- 与反磁性共存诱导非碎的拓,包括博格鲁布沃夫费米表面和更高阶的拓超导.
结论:
- 亚晶格自由度是变磁波动介导相互作用的关键.
- 变磁提供了一条通往异国情调超导体状态和拓现象的新途径.
- 这项工作为变磁超导建立了理论框架.
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