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Over 15 MA/cm(2) of critical current density in 4.8 µm thick, Zr-doped (Gd,Y)Ba(2)Cu(3)O(x) superconductor at 30 K, 3T

An Advanced MOCVD (A-MOCVD) reactor was used to deposit 4.8 µm thick (Gd,Y)BaCuO tapes with 15 mol% Zr addition in a single pass. A record-high critical current density (J(c)) of 15.11 MA/cm(2) has been measured over a bridge at 30 K, 3T, corresponding to an equivalent (I(c)) value of 8705 A/12 mm w...

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Detalles Bibliográficos
Autores principales: Majkic, Goran, Pratap, Rudra, Xu, Aixia, Galstyan, Eduard, Selvamanickam, Venkat
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5934363/
https://www.ncbi.nlm.nih.gov/pubmed/29725127
http://dx.doi.org/10.1038/s41598-018-25499-1
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author Majkic, Goran
Pratap, Rudra
Xu, Aixia
Galstyan, Eduard
Selvamanickam, Venkat
author_facet Majkic, Goran
Pratap, Rudra
Xu, Aixia
Galstyan, Eduard
Selvamanickam, Venkat
author_sort Majkic, Goran
collection PubMed
description An Advanced MOCVD (A-MOCVD) reactor was used to deposit 4.8 µm thick (Gd,Y)BaCuO tapes with 15 mol% Zr addition in a single pass. A record-high critical current density (J(c)) of 15.11 MA/cm(2) has been measured over a bridge at 30 K, 3T, corresponding to an equivalent (I(c)) value of 8705 A/12 mm width. This corresponds to a lift factor in critical current of ~11 which is the highest ever reported to the best of author’s knowledge. The measured critical current densities at 3T (B||c) and 30, 40 and 50 K, respectively, are 15.11, 9.70 and 6.26 MA/cm(2), corresponding to equivalent Ic values of 8705, 5586 and 3606 A/12 mm and engineering current densities (J(e)) of 7068, 4535 and 2928 A/mm(2). The engineering current density (J(e)) at 40 K, 3T is 7 times higher than that of the commercial HTS tapes available with 7.5 mol% Zr addition. Such record-high performance in thick films (>1 µm) is a clear demonstration that growing thick REBCO films with high critical current density (J(c)) is possible, contrary to the usual findings of strong J(c) degradation with film thickness. This achievement was possible due to a combination of strong temperature control and uniform laminar flow achieved in the A-MOCVD system, coupled with optimization of BaZrO(3) nanorod growth parameters.
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spelling pubmed-59343632018-05-10 Over 15 MA/cm(2) of critical current density in 4.8 µm thick, Zr-doped (Gd,Y)Ba(2)Cu(3)O(x) superconductor at 30 K, 3T Majkic, Goran Pratap, Rudra Xu, Aixia Galstyan, Eduard Selvamanickam, Venkat Sci Rep Article An Advanced MOCVD (A-MOCVD) reactor was used to deposit 4.8 µm thick (Gd,Y)BaCuO tapes with 15 mol% Zr addition in a single pass. A record-high critical current density (J(c)) of 15.11 MA/cm(2) has been measured over a bridge at 30 K, 3T, corresponding to an equivalent (I(c)) value of 8705 A/12 mm width. This corresponds to a lift factor in critical current of ~11 which is the highest ever reported to the best of author’s knowledge. The measured critical current densities at 3T (B||c) and 30, 40 and 50 K, respectively, are 15.11, 9.70 and 6.26 MA/cm(2), corresponding to equivalent Ic values of 8705, 5586 and 3606 A/12 mm and engineering current densities (J(e)) of 7068, 4535 and 2928 A/mm(2). The engineering current density (J(e)) at 40 K, 3T is 7 times higher than that of the commercial HTS tapes available with 7.5 mol% Zr addition. Such record-high performance in thick films (>1 µm) is a clear demonstration that growing thick REBCO films with high critical current density (J(c)) is possible, contrary to the usual findings of strong J(c) degradation with film thickness. This achievement was possible due to a combination of strong temperature control and uniform laminar flow achieved in the A-MOCVD system, coupled with optimization of BaZrO(3) nanorod growth parameters. Nature Publishing Group UK 2018-05-03 /pmc/articles/PMC5934363/ /pubmed/29725127 http://dx.doi.org/10.1038/s41598-018-25499-1 Text en © The Author(s) 2018 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Majkic, Goran
Pratap, Rudra
Xu, Aixia
Galstyan, Eduard
Selvamanickam, Venkat
Over 15 MA/cm(2) of critical current density in 4.8 µm thick, Zr-doped (Gd,Y)Ba(2)Cu(3)O(x) superconductor at 30 K, 3T
title Over 15 MA/cm(2) of critical current density in 4.8 µm thick, Zr-doped (Gd,Y)Ba(2)Cu(3)O(x) superconductor at 30 K, 3T
title_full Over 15 MA/cm(2) of critical current density in 4.8 µm thick, Zr-doped (Gd,Y)Ba(2)Cu(3)O(x) superconductor at 30 K, 3T
title_fullStr Over 15 MA/cm(2) of critical current density in 4.8 µm thick, Zr-doped (Gd,Y)Ba(2)Cu(3)O(x) superconductor at 30 K, 3T
title_full_unstemmed Over 15 MA/cm(2) of critical current density in 4.8 µm thick, Zr-doped (Gd,Y)Ba(2)Cu(3)O(x) superconductor at 30 K, 3T
title_short Over 15 MA/cm(2) of critical current density in 4.8 µm thick, Zr-doped (Gd,Y)Ba(2)Cu(3)O(x) superconductor at 30 K, 3T
title_sort over 15 ma/cm(2) of critical current density in 4.8 µm thick, zr-doped (gd,y)ba(2)cu(3)o(x) superconductor at 30 k, 3t
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5934363/
https://www.ncbi.nlm.nih.gov/pubmed/29725127
http://dx.doi.org/10.1038/s41598-018-25499-1
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