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Local density of states and superconducting gap in the iron chalcogenide superconductor Fe$_{1+\delta}$Se$_{1-x}$Te$_{x}$ observed by scanning tunneling spectroscopy

机译:铁硫族化合物的局部态密度和超导间隙   通过扫描观察超导体Fe $ _ {1+ \ delta} $ se $ _ {1-x} $ Te $ _ {x} $   隧道光谱学

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摘要

We report on the first investigation of the quasiparticle local density ofstates and superconducting gap in the iron chalcogenide superconductorFe$_{1+\delta}$Se$_{1-x}$Te$_{x}$ ($T_{\mathrm{c}} \sim 14$ K). The surface ofa cleaved crystal revealed an atomic square lattice, superimposed on theinhomogeneous background, with a lattice constant of $\sim 3.8$ \AA without anyreconstruction. Tunneling spectra measured at 4.2 K exhibit the superconductinggap, which completely disappears at 18 K, with a magnitude of $\sim 2.3$ meV,corresponding to $2\Delta / k_{\mathrm{B}}T_{\mathrm{c}}=3.8$.In stark contrastto the cuprate superconductors, the value of the observed superconducting gapis relatively homogeneous, following a sharp distribution with a small standarddeviation of 0.23 meV. Conversely, the normal-state local density of statesobserved above $T_{\mathrm{c}}$ shows spatial variation over a wide energyrange of more than 1 eV, probably due to the excess iron present in thecrystal.
机译:我们报告了关于硫族硫化物超导体中的准粒子局部态密度和超导间隙的首次调查Fe $ _ {1+ \ delta} $ Se $ _ {1-x} $ Te $ _ {x} $($ T _ {\ mathrm {c}} \ sim 14 $ K)。裂开的晶体表面显示出原子正方形晶格,叠加在不均匀的背景上,晶格常数为\\ sim 3.8 \\ AA,没有任何重构。在4.2 K处测得的隧道谱显示出超导间隙,在18 K时完全消失,幅度为\\ sim 2.3 $ meV,相当于$ 2 \ Delta / k _ {\ mathrm {B}} T _ {\ mathrm {c}} = 3.8 $。与铜酸盐超导体形成鲜明对比,观察到的超导间隙的值相对均匀,遵循尖锐的分布,标准偏差为0.23 meV。相反,在$ T _ {\ mathrm {c}} $以上观察到的状态的常态局部密度显示了在超过1 eV的较宽能量范围内的空间变化,这可能是由于晶体中存在的铁过多所致。

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