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SrIrO₃中的反铁磁激子绝缘体态

Antiferromagnetic excitonic insulator state in SrIrO.

作者信息

Mazzone D G, Shen Y, Suwa H, Fabbris G, Yang J, Zhang S-S, Miao H, Sears J, Jia Ke, Shi Y G, Upton M H, Casa D M, Liu X, Liu Jian, Batista C D, Dean M P M

机构信息

Department of Condensed Matter Physics and Materials Science, Brookhaven National Laboratory, Upton, NY, 11973, USA.

Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, CH-5232, Villigen, Switzerland.

出版信息

Nat Commun. 2022 Feb 17;13(1):913. doi: 10.1038/s41467-022-28207-w.

DOI:10.1038/s41467-022-28207-w
PMID:35177583
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8854623/
Abstract

Excitonic insulators are usually considered to form via the condensation of a soft charge mode of bound electron-hole pairs. This, however, presumes that the soft exciton is of spin-singlet character. Early theoretical considerations have also predicted a very distinct scenario, in which the condensation of magnetic excitons results in an antiferromagnetic excitonic insulator state. Here we report resonant inelastic x-ray scattering (RIXS) measurements of SrIrO. By isolating the longitudinal component of the spectra, we identify a magnetic mode that is well-defined at the magnetic and structural Brillouin zone centers, but which merges with the electronic continuum in between these high symmetry points and which decays upon heating concurrent with a decrease in the material's resistivity. We show that a bilayer Hubbard model, in which electron-hole pairs are bound by exchange interactions, consistently explains all the electronic and magnetic properties of SrIrO indicating that this material is a realization of the long-predicted antiferromagnetic excitonic insulator phase.

摘要

激子绝缘体通常被认为是通过束缚电子 - 空穴对的软电荷模式凝聚形成的。然而,这假定软激子具有自旋单重态特征。早期的理论研究也预测了一种非常不同的情况,即磁激子的凝聚会导致反铁磁激子绝缘体态。在此,我们报告了对SrIrO的共振非弹性X射线散射(RIXS)测量结果。通过分离光谱的纵向分量,我们识别出一种磁模式,它在磁和结构布里渊区中心定义明确,但在这些高对称点之间与电子连续体合并,并且在加热时随着材料电阻率的降低而衰减。我们表明,一种双层哈伯德模型,其中电子 - 空穴对通过交换相互作用束缚在一起,能够一致地解释SrIrO的所有电子和磁特性,表明这种材料是长期预测的反铁磁激子绝缘相的一种实现。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/5860682e9218/41467_2022_28207_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/dad22eb183e9/41467_2022_28207_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/a9b47cc4126c/41467_2022_28207_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/b0e61c4d55b3/41467_2022_28207_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/5860682e9218/41467_2022_28207_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/dad22eb183e9/41467_2022_28207_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/a9b47cc4126c/41467_2022_28207_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/b0e61c4d55b3/41467_2022_28207_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1e96/8854623/5860682e9218/41467_2022_28207_Fig4_HTML.jpg

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本文引用的文献

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Amplitude Mode in Quantum Magnets via Dimensional Crossover.通过维度交叉实现量子磁体中的振幅模式
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Coherent many-body exciton in van der Waals antiferromagnet NiPS.范德瓦尔斯反铁磁体 NiPS 中的相干多体激子。
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Zero-gap semiconductor to excitonic insulator transition in TaNiSe.TaNiSe 中零能隙半导体到激子绝缘体态的转变
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