Optimization of Transport Critical Currents at 4.2 K – 20 K at Magnetic Fields Up to 31 T for MOCVD REBCO Conductors With Variable Zr and Growth Conditions

The critical current, <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$I_{\mathrm{c}}$</tex-math></inline-formula>, of REBCO full-width 4 mm short samples made by metal-organic chemical vapor deposition (MOCVD), optimized for high-field applications, were measured at magnetic fields perpendicular to sample plane up to 31.2 T in resistive magnets and temperature range <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\text{4.2}}\,{\text{K}}$</tex-math></inline-formula>–55 K. Dependencies of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$I_{\mathrm{c}}$</tex-math></inline-formula>, critical current density (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$J_{\mathrm{c}}$</tex-math></inline-formula>), and pinning force density (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$F_{\mathrm{p}}$</tex-math></inline-formula>) on Zr doping and REBCO growth conditions were studied. SEM images of cross-section and top view of the REBCO layers for tapes with 15%, 20%, and 25% Zr doping show dense REBCO layers without secondary phases or porosity. REBCO tapes with 20% and 25% Zr doping perform better in transport <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$I_{\mathrm{c}}$</tex-math></inline-formula>(<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">T,</i><inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\mu _{o}H$</tex-math></inline-formula>) tests at 20 K and 20 T conditions than tapes with lower Zr doping and can be promising candidates for applications focusing on magnetic plasma confinement.

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Journal
IEEE Transactions on Applied Superconductivity
Published
2025-03-11
DOI
https://doi.org/10.1109/tasc.2025.3549409
Citations
1
Primary Topic
Physics of Superconductivity and Magnetism
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article
Field-Weighted Citation Impact
1.26

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article

Optimization of Transport Critical Currents at 4.2 K – 20 K at Magnetic Fields Up to 31 T for MOCVD REBCO Conductors With Variable Zr and Growth Conditions

Griffin Bradford, J. Kvitkovič, Yaron Oz, Ji-Kwang Lee et al.
1 citations
IEEE Transactions on Applied Superconductivity
Physics of Superconductivity and Magnetism
1.26
article

Optimization of Transport Critical Currents at 4.2 K – 20 K at Magnetic Fields Up to 31 T for MOCVD REBCO Conductors With Variable Zr and Growth Conditions

Griffin Bradford, J. Kvitkovič, Yaron Oz, Ji-Kwang Lee, J. Jaroszyński, Dmytro Abraimov, Shaolin Mao, Yifei Zhang, J. Gillman, Norman I. Bishop, Chen Zha, Hannah H. L. S. M. Pimentel
article en
1 citations

Abstract

The critical current, <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$I_{\mathrm{c}}$</tex-math></inline-formula>, of REBCO full-width 4 mm short samples made by metal-organic chemical vapor deposition (MOCVD), optimized for high-field applications, were measured at magnetic fields perpendicular to sample plane up to 31.2 T in resistive magnets and temperature range <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">${\text{4.2}}\,{\text{K}}$</tex-math></inline-formula>–55 K. Dependencies of <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$I_{\mathrm{c}}$</tex-math></inline-formula>, critical current density (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$J_{\mathrm{c}}$</tex-math></inline-formula>), and pinning force density (<inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$F_{\mathrm{p}}$</tex-math></inline-formula>) on Zr doping and REBCO growth conditions were studied. SEM images of cross-section and top view of the REBCO layers for tapes with 15%, 20%, and 25% Zr doping show dense REBCO layers without secondary phases or porosity. REBCO tapes with 20% and 25% Zr doping perform better in transport <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$I_{\mathrm{c}}$</tex-math></inline-formula>(<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">T,</i><inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><tex-math notation="LaTeX">$\mu _{o}H$</tex-math></inline-formula>) tests at 20 K and 20 T conditions than tapes with lower Zr doping and can be promising candidates for applications focusing on magnetic plasma confinement.

IEEE Transactions on Applied SuperconductivityVol. 35(5)
Florida State University (US)
U.S. Department of Energy, National High Magnetic Field Laboratory
Openalex Percentile: Top 23%
Physics of Superconductivity and Magnetism
1.26
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