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arXiv 2201.01656cond-mat.supr-con
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最大角度扭转同质双层体系中的高角动量拓扑超导性

High-Angular-Momentum Topological Superconductivity in the Largest-Angle Twisted Homo-bilayer Systems

Yu-Bo Liu, Yongyou Zhang, Wei-Qiang Chen, Fan Yang

AI总结:

研究最大角度扭转同质双层体系,利用其准晶体对称性产生高角动量拓扑超导性,并通过微观框架在三个实例中预测了不同角动量的拓扑超导态。

摘要:

我们研究了最大角度扭转同质双层(LA-THB)体系,其具有无莫尔条纹的准晶体(QC)结构。我们提出利用这些材料来产生受其准晶体对称性保护的高角动量(HAM)拓扑超导性(TSCs),这种对称性在传统晶体材料中是不存在的。这一提议基于我们普适的Ginzburg-Landau理论分析,该分析得出一般性结论:当每个具有$D_n$对称性($n$为偶数)的单层承载配对角动量为$l\le \frac{n}{2}$的超导性时,层间约瑟夫森耦合将在LA-THB中诱导出配对角动量为$L=l$或$L=n-l$的超导性,具体由微观细节决定。后者在$l>0$时即为高角动量拓扑超导性。基于我们修正的微扰能带理论,我们发展了研究涉及电子-电子相互作用的准晶体LA-THB体系的通用微观框架,并利用该框架研究了三个实例,即30$^\circ$扭转双层石墨烯、30$^\circ$扭转双层BC$_3$和45$^\circ$扭转双层铜氧化物。在这些体系的特定掺杂区间内,可分别涌现出具有高角动量$L=4,5$和$2$的$g+ig$-、$h+ih$-和$d+id$-拓扑超导性。

英文摘要:

We study the largest-angle twisted homo-bilayer (LA-THB) systems, hosting Moiréless quasi-crystal (QC) structure. We propose to use these materials to generate high-angular-momentum (HAM) topological superconductivities (TSCs) protected by their QC symmetries absent on conventional crystalline materials. This proposal is based on our universal Ginzburg-Landau theory based analysis which yields the general conclusion that, when each $D_n$-symmetric ($n$ is even) monolayer hosts SC with pairing angular momentum $l\le \frac{n}{2}$, the interlayer Josephson coupling will induce SC with pairing angular momentum $L=l$ or $L=n-l$ in the LA-THB, determined by microscopic details. The latter one is just the HAM TSC if $l>0$. Based on our revised perturbational-band theory, we develop general microscopic framework to study the QC LA-THBs involving electron-electron interactions, adopting which we study three examples, i.e. the 30$^\circ$- twisted bilayer graphene, the 30$^\circ$- twisted bilayer BC$_3$, and the 45$^\circ$- twisted bilayer cuprates. The $g+ig$- $h+ih$- and $d+id$- TSCs with HAM $L=4,5$ and $2$ can emerge in certain doping regimes in these systems, respectively.

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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