Critical Role Played by Interface Engineering in Weakening Thickness Dependence of Superconducting and Structural Properties of FeSe0.5Te0.5-Coated Conductors

被引:8
|
作者
Song, Jiannan [1 ,2 ]
Xu, Zhongtang [1 ]
Xiong, Xuming [3 ]
Yuan, Wen [3 ]
Dong, Chiheng [1 ]
Sun, Qiao [1 ]
Tang, Minghui [1 ]
Chen, Wanping [2 ]
Tian, Huanfang [4 ]
Li, Jianqi [4 ]
Ma, Yanwei [1 ,5 ]
机构
[1] Chinese Acad Sci, Inst Elect Engn, Key Lab Appl Superconduct, Beijing 100190, Peoples R China
[2] Wuhan Univ, Sch Phys & Technol, Key Lab Artificial Micro & Nanostruct, Minist Educ, Wuhan 430072, Hubei, Peoples R China
[3] Suzhou Adv Mat Res Inst Co Ltd, Suzhou 215123, Peoples R China
[4] Chinese Acad Sci, Inst Phys, Beijing Natl Lab Condensed Matter Phys, Beijing 100190, Peoples R China
[5] Univ Chinese Acad Sci, Beijing 100049, Peoples R China
基金
国家重点研发计划; 中国国家自然科学基金;
关键词
iron-based superconductors; interface engineering; flux pinning; thickness effect; coated conductors; SURFACE-MORPHOLOGY; FABRICATION; FESE; YBA2CU3O7-DELTA; SRTIO3; TAPES; FILMS; SITU;
D O I
10.1021/acsami.3c04531
中图分类号
TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
Increasing the thickness of a superconducting layer andsimultaneouslyreducing the thickness effect in iron-based superconducting coatedconductors are particularly essential for improving the critical current I (c). Here, for the first time, we have depositedhigh-performance FeSe0.5Te0.5 (FST) superconductingfilms up to 2 mu m on LaMnO3-buffered metal tapes bypulsed laser deposition. An interface engineering strategy, alternatinggrowth of a 10 nm-thick nonsuperconducting FST seed layer and a 400nm-thick FST superconducting layer, was employed to guarantee thecrystalline quality of the films with thicknesses of the order ofmicrometers, resulting in a highly biaxial texture with grain boundarymisorientation angle less than the critical value theta(c) similar to 9 degrees. Moreover, the thickness effect, that the criticalcurrent density (J (c)) shows a clear dependenceon thickness as in cuprates, is reduced by the interface engineering.Also, the maximum J (c) was found for a 400nm-thick film with 1.3 MA/cm(2) in self-field at 4.2 K and0.71 MA/cm(2) (H parallel to ab) and 0.50 MA/cm(2) (H parallel to c) at 9 T. Anisotropic Ginzburg-Landau scaling indicates thatthe major pinning centers vary from correlated to uncorrelated asthe film thickness increases, while the thickness effect is most likelyrelated to the weakening of flux pinning by the fluctuation of charge-carriermean free path (delta l) and strengthening of fluxpinning caused by the variation of superconducting transition temperature(delta T (c)) due to off-stoichiometry withthickness.
引用
收藏
页码:26215 / 26224
页数:10
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