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Revisit of the Orbital-Fluctuation-Mediated Superconductivity in LiFeAs: Nontrivial Spin-Orbit Interaction Effects on the Bandstructure and Superconducting Gap Function

机译:再次讨论了轨道 - 波动介导的LiFeas超导电性:   非平凡自旋轨道相互作用对带结构和结构的影响   超导间隙功能

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摘要

Precise gap structure in LiFeAs (Tc = 18 K) given by ARPES studies offers ussignificant information to understand the pairing mechanism in iron-basedsuperconductors. The most remarkable characteristics in LiFeAs gap structurewould be that "the largest gap emerges on the tiny hole-pockets around Zpoint". This result had been naturally explained in terms of theorbital-fluctuation scenario (T. Saito et al., Phys. Rev. B 90, 035104 (2014)),whereas an opposite result is obtained by the spin-fluctuation scenario. Inthis paper, we study the gap structure in LiFeAs by taking the spin-orbitinteraction (SOI) into account, motivated by the recent ARPES studies thatrevealed the significant SOI-induced modification of the Fermi surfacetopology. For this purpose, we construct the two possible tight-binding modelswith finite SOI by referring the bandstructures given by different ARPESgroups. In addition, we extend the gap equation for multiorbital systems withfinite SOI, and calculate the gap functions by applying the orbital-spinfluctuation theory. On the basis of both SOI-induced band structures, maincharacteristics of the gap structure in LiFeAs are naturally reproduced only inthe presence of strong inter-orbital interactions between (xz/yz - xy)orbitals. Thus, the experimental gap structure in LiFeAs is a strong evidencefor the orbital-fluctuation pairing mechanism.
机译:ARPES研究提供的LiFeAs(Tc = 18 K)中的精确间隙结构为理解铁基超导体的配对机理提供了重要的信息。 LiFeAs间隙结构最显着的特征是“最大的间隙出现在Zpoint周围的微小孔穴上”。该结果已经根据轨道波动情况自然地得到了解释(T. Saito等人,Phys。Rev. B 90,035104(2014)),而自旋波动情况得到了相反的结果。在本文中,我们受自旋轨道相互作用(SOI)的影响,研究了LiFeAs中的间隙结构,这是由最近的ARPES研究推动的,该研究揭示了SOI引起的费米表面拓扑学的重大改变。为此,我们通过参考不同的ARPES组给出的能带结构,构建了两个具有有限SOI的紧密绑定模型。此外,我们扩展了具有有限SOI的多轨道系统的间隙方程,并通过应用轨道自旋涨落理论来计算间隙函数。基于两种SOI诱导的能带结构,只有在(xz / yz-xy)轨道之间存在强烈的轨道间相互作用时,才能自然再现LiFeAs中间隙结构的主要特征。因此,LiFeAs中的实验间隙结构是轨道波动配对机制的有力证据。

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