Diverse Exotic Orders and Fermiology in Fe-based Superconductors: A Unified Mechanism for Nematicity in FeSe/(Cs,Rb)FeAs and Smectic Order in BaFeAs
arXiv:2204.03928 · doi:10.3389/fphy.2022.915619
Abstract
A rich variety of nematic/smectic orders in Fe-based superconductors is an important unsolved problem in strongly correlated electron systems. A unified understanding of these orders has been investigated for the last decade. In this article, we explain the symmetry nematic transition in FeSeTe, the symmetry nematicity in AFeAs (A=Cs, Rb), and the smectic state in BaFeAs based on the same framework. We investigate the quantum interference mechanism between spin fluctuations by developing the density wave equation. The observed rich variety of nematic/smectic orders is naturally understood in this mechanism. The nematic/smectic orders depend on the characteristic shape and topology of the Fermi surface (FS) of each compound. (i) In FeSeTe, each FS is very small and the dxy-orbital hole pocket is below the Fermi level. In this case, the small spin fluctuations on three dxz, dyz, and dxy orbitals cooperatively lead to the nematic order. The experimental Lifshitz transition below the nematic transition temperature is naturally reproduced. (ii) In BaFeAs, the dxy-orbital hole pocket emerges around M point, and each FS is relatively large. The strong spin fluctuations due to the dxy-orbital nesting give rise to the nematic order and the smectic order, and the latter transition temperature () exceeds the former one . (iii) In heavily hole-doped AFeAs, the large dxy-orbital hole pocket and the four tiny Dirac pockets appear due to the hole-doping. The nematic bond order emerges on the dxy-orbital hole pocket due to the same interference mechanism. The present paramagnon interference mechanism provides a unified explanation of why the variety of nematic/smectic orders in Fe-based superconductors is so rich, based on the well-established fermiology of Fe-based superconductors.
24 pages, 14 figures
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