Signatures of Amorphous Shiba State in FeTe$_{0.55}$Se$_{0.45}$

Jinwon Lee, Sanghun Lee, Andreas Kreisel, Jens Paaske, Brian M. Andersen, Koen M. Bastiaans, Damianos Chatzopoulos, Genda Gu, Doohee Cho, Milan P. Allan
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Abstract

The iron-based superconductor FeTe$_{0.55}$Se$_{0.45}$ is a peculiar material: it hosts a surface state with a Dirac dispersion, is a putative topological superconductor hosting Majorana modes in vortices, and has an unusually low Fermi energy. The superconducting state is generally thought to be characterized by three gaps in different bands, with the usual homogenous, spatially extended Bogoliubov excitations -- in this work, we uncover evidence that it is instead of a very different nature. Our scanning tunneling spectroscopy data shows several peaks in the density of states above a full gap, and by analyzing the spatial and junction-resistance dependence of the peaks, we conclude that the peaks above the first one are not coherence peaks from different bands. Instead, comparisons with our simulations indicate that they originate from generalized Shiba states that are spatially overlapping. This can lead to an amorphous state of Bogoliubov quasiparticles, reminiscent of impurity bands in semiconductors. We discuss the origin and implications of this new state.
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FeTe$_{0.55}$Se$_{0.45}$ 中非晶态芝态的特征
铁基超导体 FeTe$_{0.55}$Se$_{0.45}$ 是一种奇特的材料:它具有狄拉克色散的表面态,是一种假定的拓扑超导体,在涡流中容纳马约拉纳模式,并且具有异常低的费米能。超导态通常被认为具有三个不同带的间隙,并具有通常的同质、空间扩展的波哥留布夫激发--在这项研究中,我们发现了其性质截然不同的证据。通过分析这些峰值的空间和结电阻依赖性,我们得出结论:第一个峰值之上的峰值并非来自不同波段的相干峰值。相反,与我们的模拟比较表明,它们源于在空间上重叠的广义芝波态。这可能会导致博戈利乌波夫准粒子的非晶态,让人想起半导体中的杂质带。我们将讨论这种新状态的起源和影响。
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