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调控 NaLiFeAs 超导体中向列有序和自旋涨落之间的相互作用。

Tuning the interplay between nematicity and spin fluctuations in NaLi FeAs superconductors.

机构信息

IFW Dresden, Helmholtzstr. 20, 01069, Dresden, Germany.

Department of Physics and Astronomy, Center for Novel State of Complex Materials Research, Seoul National University, Seoul, 151-747, Korea.

出版信息

Nat Commun. 2018 May 30;9(1):2139. doi: 10.1038/s41467-018-04471-7.

Abstract

Strong interplay of spin and charge/orbital degrees of freedom is the fundamental characteristic of the iron-based superconductors (FeSCs), which leads to the emergence of a nematic state as a rule in the vicinity of the antiferromagnetic state. Despite intense debate for many years, however, whether nematicity is driven by spin or orbital fluctuations remains unsettled. Here, by use of transport, magnetization, and As nuclear magnetic resonance (NMR) measurements, we show a striking transformation of the relationship between nematicity and spin fluctuations (SFs) in NaLi FeAs; For x ≤ 0.02, the nematic transition promotes SFs. In contrast, for x ≥ 0.03, the system undergoes a non-magnetic phase transition at a temperature T into a distinct nematic state that suppresses SFs. Such a drastic change of the spin fluctuation spectrum associated with nematicity by small doping is highly unusual, and provides insights into the origin and nature of nematicity in FeSCs.

摘要

铁基超导体(FeSCs)的基本特征是自旋和电荷/轨道自由度的强烈相互作用,这导致在反铁磁态附近通常会出现向列相。然而,尽管多年来激烈争论,但向列相是由自旋还是轨道涨落驱动仍未解决。在这里,我们通过输运、磁化和砷核磁共振(NMR)测量,展示了 NaLiFeAs 中向列性和自旋涨落(SFs)之间关系的惊人转变;对于 x≤0.02,向列相变促进 SFs。相比之下,对于 x≥0.03,系统在温度 T 下经历非磁性相变进入一个明显的向列相,抑制 SFs。这种由小掺杂引起的与向列性相关的自旋涨落谱的剧烈变化非常罕见,为理解 FeSCs 中向列性的起源和性质提供了线索。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/47bf/5976654/bcf6f7335834/41467_2018_4471_Fig1_HTML.jpg

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