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Determining the Thickness of the Dead Layer in Superconducting Film Using a Two-Coil Mutual-Inductance Technique

Ruozhou Zhang, Zhanyi Zhao, Mingyang Qin, Juan Xu, Wenxin Cheng, Yangmu Li, Qihong Chen, Jie Yuan, Kui Jin

DOI 10.1103/PhysRevApplied.17.054034 · Physical Review Applied

T1

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Abstract

A dead layer without superconductivity, i.e., zero resistance and Meissner effect, commonly exists at the interface between substrate and superconducting film. It is demonstrated that the dead layer can significantly degrade the performance of superconducting devices at microwave frequencies. Knowing the thickness of the dead layer, ddead, is necessary when using a two-coil mutual-inductance (TCMI) technique to measure the absolute value of the magnetic penetration depth, λ, in superconducting films. However, there is still no established method to determine ddead in superconducting films. Here, we propose employing the TCMI technique to determine ddead, based on a multilayered model in which the dead layer is sandwiched between superconducting layer and substrate. Using this method, we find that ddead=43±10nm for our superconducting FeSe films, in agreement with the absence of diamagnetism for the 42-nm-thick film. With the ddead determined, we accurately determine the absolute value of λ in superconducting FeSe films.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
FeSe

Archive — visibility unverified

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8Pressure not reportedonset
FeSe

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

8Pressure not reportedonset

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