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Superconducting Properties of (Mx/YBa2Cu3O7-δy)N Multilayer Films with Variable Layer Thickness x.

Authors :
Haugan, T. J.
Barnes, P. N.
Campbell, T. A.
Pierce, N. A.
Baca, F. J.
Locke, M. F.
Brockman, I.
Westerfield, A. L.
Evans, J. M.
Morgan, R.
Klenk, P.
Harrison, B. C.
Chaney, A. D.
Maartense, I.
Source :
Journal of Electronic Materials; Oct2007, Vol. 36 Issue 10, p1234-1242, 9p, 3 Diagrams, 1 Chart, 4 Graphs
Publication Year :
2007

Abstract

The superconducting properties of (M<subscript>x</subscript>/YBa<subscript>2</subscript>Cu<subscript>3</subscript>O<subscript>7-δy</subscript>)<subscript>N</subscript> multilayer films were studied for varying layer thickness x. Different M phases were examined including green-phase Y<subscript>2</subscript>BaCuO<subscript>5</subscript> (211), Y<subscript>2</subscript>O<subscript>3</subscript>, BaZrO<subscript>3</subscript>, CeO<subscript>2</subscript>, SmBa<subscript>2</subscript>Cu<subscript>3</subscript>O<subscript>7-δ</subscript> (Sm123), brown-phase La<subscript>2</subscript>BaCuO<subscript>5</subscript> (La211), and MgO. Multilayer (M<subscript>x</subscript>/YBa<subscript>2</subscript>Cu<subscript>3</subscript>O<subscript>7-δy</subscript>)N structures were grown by pulsed laser deposition onto SrTiO<subscript>3</subscript> or LaAlO<subscript>3</subscript> single-crystal substrates by alternate ablation of separate YBa<subscript>2-</subscript>Cu<subscript>3</subscript>O<subscript>7-δ</subscript> (123) and M targets, at temperatures of 750°C to 790°C. The x layer thickness was varied from 0.1 nm to 4.5 nm, and the y 123 layer thickness was kept constant within a given range of 10 to 25 nm. Different M phase and x layer thicknesses caused large variations of the microstructural and superconducting properties, including superconducting transition (T<subscript>c</subscript>), critical current density as a function of applied magnetic field J<subscript>c</subscript>(H), self-field J<subscript>c</subscript>(77 K), and nanoparticle layer coverage. Strong flux-pinning enhancement up to 1 to 3x was observed to occur for M additions of 211 and BaZrO<subscript>3</subscript> at 65 to 77 K, Y2O<subscript>3</subscript> at 65 K, and CeO<subscript>2</subscript> for H < 0.5 T. BaZrO<subscript>3</subscript> had a noticeably different epitaxy forming smaller size nanoparticles ~8 nm with 3 to 4x higher areal surface particle densities than other M phases, reaching 5 x 10<superscript>11</superscript> nanoparticles cm<superscript>-2</superscript>. To optimize flux pinning and J<subscript>c</subscript> (65 to 77 K, H = 2 to 3 T), the M layer thickness had to be reduced below a critical value that correlated with a nanoparticle surface coverage <15% by area. Unusual effects were observed for poor pinning materials including Sm123 and La211, where properties such as self-field J<subscript>c</subscript> unexpectedly increased with increasing x layer thickness. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
03615235
Volume :
36
Issue :
10
Database :
Complementary Index
Journal :
Journal of Electronic Materials
Publication Type :
Academic Journal
Accession number :
27671792
Full Text :
https://doi.org/10.1007/s11664-007-0229-y