TY - JOUR
T1 - Three-dimensional vortex pinning by nano-precipitates in a Sm-doped YBa2Cu3O7-x coated conductor
AU - Chen, Z.
AU - Feldmann, D. M.
AU - Song, X.
AU - Kim, S. I.
AU - Gurevich, A.
AU - Reeves, J. L.
AU - Xie, Y. Y.
AU - Selvamanickam, V.
AU - Larbalestier, D. C.
PY - 2007/9/1
Y1 - 2007/9/1
N2 - We report on the thickness and angular dependence of the critical current density Jc(H,), the irreversibility field Hirr, and the bulk pinning force Fp(H) of a metal-organic chemical vapour deposition (MOCVD) grown YBa2Cu3O7-x (YBCO) coated conductor, which contains ∼17vol% of ∼10nm sized (Y,Sm) 2O3 precipitates with an average spacing of ∼10-15nm. Some surface porosity and amorphous second-phase particles on the scale of ∼0.5-1νm appear to reduce the current-carrying cross-section, which controls the magnitude of Jc but not the vortex pinning. We observed an enhanced Hirr∼9 T at 77K along the c-axis which, like the shape of Jc(H) and Fp(H), was independent of thickness as the sample was milled down to ∼0.16νm. Angular-dependent measurements of Jc showed the usual excess vortex pinning along the c-axis and along the ab-plane, but with a background that could only be fitted with an unusually small anisotropy parameter of 3, which, like the high Hirr and the thickness-independent shape of Fp(H), we ascribe to strong vortex pinning centre interactions. Together, these measurements show very different behaviour from most pulsed-laser-deposited films, which exhibit strong thickness-dependent properties. We ascribe the present different results to the dense array of small, insulating precipitates, which act as strong pinning centres and produce strong three-dimensional (3D) vortex pinning, because their separation of 10-15nm is always much smaller than the film thickness.
AB - We report on the thickness and angular dependence of the critical current density Jc(H,), the irreversibility field Hirr, and the bulk pinning force Fp(H) of a metal-organic chemical vapour deposition (MOCVD) grown YBa2Cu3O7-x (YBCO) coated conductor, which contains ∼17vol% of ∼10nm sized (Y,Sm) 2O3 precipitates with an average spacing of ∼10-15nm. Some surface porosity and amorphous second-phase particles on the scale of ∼0.5-1νm appear to reduce the current-carrying cross-section, which controls the magnitude of Jc but not the vortex pinning. We observed an enhanced Hirr∼9 T at 77K along the c-axis which, like the shape of Jc(H) and Fp(H), was independent of thickness as the sample was milled down to ∼0.16νm. Angular-dependent measurements of Jc showed the usual excess vortex pinning along the c-axis and along the ab-plane, but with a background that could only be fitted with an unusually small anisotropy parameter of 3, which, like the high Hirr and the thickness-independent shape of Fp(H), we ascribe to strong vortex pinning centre interactions. Together, these measurements show very different behaviour from most pulsed-laser-deposited films, which exhibit strong thickness-dependent properties. We ascribe the present different results to the dense array of small, insulating precipitates, which act as strong pinning centres and produce strong three-dimensional (3D) vortex pinning, because their separation of 10-15nm is always much smaller than the film thickness.
UR - http://www.scopus.com/inward/record.url?scp=34548772941&partnerID=8YFLogxK
U2 - 10.1088/0953-2048/20/9/S14
DO - 10.1088/0953-2048/20/9/S14
M3 - Article
AN - SCOPUS:34548772941
SN - 0953-2048
VL - 20
SP - S205-S210
JO - Superconductor Science and Technology
JF - Superconductor Science and Technology
IS - 9
M1 - S14
ER -