Nematicity and Magnetism in FeSe and Other Families of Fe-Based Superconductors

Nematicity and magnetism are two key features in Fe-based superconductors, and their interplay is one of the most important unsolved problems. In FeSe, the magnetic order is absent below the structural transition temperature T_{str}=90  K, in stark contrast to the fact that the magnetism emerges sli...

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Main Authors: Youichi Yamakawa, Seiichiro Onari, Hiroshi Kontani
Format: Article
Language:English
Published: American Physical Society 2016-06-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.6.021032
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spelling doaj-1d1039fb3afc43f8adf05c48cc1f94482020-11-24T23:42:35ZengAmerican Physical SocietyPhysical Review X2160-33082016-06-016202103210.1103/PhysRevX.6.021032Nematicity and Magnetism in FeSe and Other Families of Fe-Based SuperconductorsYouichi YamakawaSeiichiro OnariHiroshi KontaniNematicity and magnetism are two key features in Fe-based superconductors, and their interplay is one of the most important unsolved problems. In FeSe, the magnetic order is absent below the structural transition temperature T_{str}=90  K, in stark contrast to the fact that the magnetism emerges slightly below T_{str} in other families. To understand such amazing material dependence, we investigate the spin-fluctuation-mediated orbital order (n_{xz}≠n_{yz}) by focusing on the orbital-spin interplay driven by the strong-coupling effect, called the vertex correction. This orbital-spin interplay is very strong in FeSe because of the small ratio between the Hund’s and Coulomb interactions (J[over ¯]/U[over ¯]) and large d_{xz}, d_{yz}-orbital weight at the Fermi level. For this reason, in the FeSe model, the orbital order is established irrespective of the fact that the spin fluctuations are very weak, so the magnetism is absent below T_{str}. In contrast, in the LaFeAsO model, the magnetic order appears just below T_{str} both experimentally and theoretically. Thus, the orbital-spin interplay due to the vertex correction is the key ingredient in understanding the rich phase diagram with nematicity and magnetism in Fe-based superconductors in a unified way.http://doi.org/10.1103/PhysRevX.6.021032
collection DOAJ
language English
format Article
sources DOAJ
author Youichi Yamakawa
Seiichiro Onari
Hiroshi Kontani
spellingShingle Youichi Yamakawa
Seiichiro Onari
Hiroshi Kontani
Nematicity and Magnetism in FeSe and Other Families of Fe-Based Superconductors
Physical Review X
author_facet Youichi Yamakawa
Seiichiro Onari
Hiroshi Kontani
author_sort Youichi Yamakawa
title Nematicity and Magnetism in FeSe and Other Families of Fe-Based Superconductors
title_short Nematicity and Magnetism in FeSe and Other Families of Fe-Based Superconductors
title_full Nematicity and Magnetism in FeSe and Other Families of Fe-Based Superconductors
title_fullStr Nematicity and Magnetism in FeSe and Other Families of Fe-Based Superconductors
title_full_unstemmed Nematicity and Magnetism in FeSe and Other Families of Fe-Based Superconductors
title_sort nematicity and magnetism in fese and other families of fe-based superconductors
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2016-06-01
description Nematicity and magnetism are two key features in Fe-based superconductors, and their interplay is one of the most important unsolved problems. In FeSe, the magnetic order is absent below the structural transition temperature T_{str}=90  K, in stark contrast to the fact that the magnetism emerges slightly below T_{str} in other families. To understand such amazing material dependence, we investigate the spin-fluctuation-mediated orbital order (n_{xz}≠n_{yz}) by focusing on the orbital-spin interplay driven by the strong-coupling effect, called the vertex correction. This orbital-spin interplay is very strong in FeSe because of the small ratio between the Hund’s and Coulomb interactions (J[over ¯]/U[over ¯]) and large d_{xz}, d_{yz}-orbital weight at the Fermi level. For this reason, in the FeSe model, the orbital order is established irrespective of the fact that the spin fluctuations are very weak, so the magnetism is absent below T_{str}. In contrast, in the LaFeAsO model, the magnetic order appears just below T_{str} both experimentally and theoretically. Thus, the orbital-spin interplay due to the vertex correction is the key ingredient in understanding the rich phase diagram with nematicity and magnetism in Fe-based superconductors in a unified way.
url http://doi.org/10.1103/PhysRevX.6.021032
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