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arXiv 2302.04489cond-mat.supr-con
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在更高阶Van Hove填充下的自旋轨道耦合系统中鲁棒的拓扑超导性

Robust topological superconductivity in spin-orbit coupled systems at higher-order van Hove filling

Kavli Institute for Theoretical Sciences, University of Chinese Academy of Sciences(中国科学院大学 Kavli 理论科学研究院);Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences(中国科学院物理研究所 北京凝聚态物理国家研究中心);School of Physical Sciences, University of Chinese Academy of Sciences(中国科学院大学 物理科学学院);CAS Key Laboratory of Theoretical Physics, Institute of Theoretical Physics, Chinese Academy of Sciences(中国科学院理论物理研究所 理论物理国家重点实验室)

Xinloong Han, Jun Zhan, Fu-chun Zhang, Jiangping Hu, Xianxin Wu

AI总结:

该研究通过分析自旋轨道耦合与Van Hove奇异点的相互作用,揭示了在更高阶填充下系统成为鲁棒拓扑超导体的机制。

摘要:

Van Hove奇异点(VHSs)接近费米能级会促进电子相互作用并产生多种竞争的不稳定性。此外,来自自旋轨道耦合(SOC)的非平凡 Berry 阶可以引入有趣的装饰到相互作用中,从而改变相关现象。然而,不清楚在VHSs和Berry相相互作用的系统中,如何以及会产生什么类型的新物理。在此,基于平方晶格上的通用Rashba模型,我们全面探讨了这种相互作用及其对竞争电子不稳定性的重要影响,通过进行parquet重整化群分析。尽管粒子-粒子和粒子-空穴通道中与更高阶VHSs相关的各种可比较波动存在,我们发现chiral p±ip配对在通用相互作用参数空间中作为两个稳定的固定轨迹出现,即系统成为鲁棒的拓扑超导体。chiral配对源于非平凡Berry相诱导的跃迁相互作用。讨论了可能的实验实现和影响。我们的工作为具有强SOC的量子材料中的相关态提供了新的视角,并为拓扑超导性的探索提供了新的见解。

英文摘要:

Van Hove singularities (VHSs) in proximity to the Fermi level promote electronic interactions and generate diverse competing instabilities. It is also known that a nontrivial Berry phase derived from spin-orbit coupling (SOC) can introduce an intriguing decoration into the interactions and thus alter correlated phenomena. However, it is unclear how and what type of new physics can emerge in a system featured by the interplay between VHSs and the Berry phase. Here, based on a general Rashba model on the square lattice, we comprehensively explore such an interplay and its significant influence on the competing electronic instabilities by performing a parquet renormalization group analysis. Despite the existence of a variety of comparable fluctuations in the particle-particle and particle-hole channels associated with higher-order VHSs, we find that the chiral $p \pm ip$ pairings emerge as two stable fixed trajectories within the generic interaction parameter space, namely the system becomes a robust topological superconductor. The chiral pairings stem from the hopping interaction induced by the nontrivial Berry phase. The possible experimental realization and implications are discussed. Our work sheds new light on the correlated states in quantum materials with strong SOC and offers fresh insights into the exploration of topological superconductivity.

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。

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