The effect of facet lines on critical current density and trapped field in bulk RE-Ba-Cu-O single grains

Bulk, single grain RE-Ba-Cu-O (where RE = rare earth or yttrium) [(RE)BCO] high temperature superconductors could potentially be used to generate stable magnetic fields for magnetic resonance imaging (MRI) and nuclear magnetic resonance (NMR). In these applications, however, the homogeneity of the magnetic field is of critical importance. As a result, the spatial distribution of critical current density, J (c), within the bulk single grain and the effects of the magnetisation process, which are primary drivers of the uniformity of the achievable trapped magnetic field, are fundamental to assessing the performance of these technologically important materials. This paper reports the systematic measurement of the distribution of J (c)-B at 77 K over a vertical cross-section of a single grain along a facet line and through the seed crystal [(110)-F] at 20 positions within a 20 mm diameter Gd-Ba-Cu-O sample in an attempt to understand and assess the distribution of J (c) along this microstructural feature. A comparison of the data within the whole vertical plane across the seed measured along the a or b direction within the [(100)-a] plane shows that J (c)-B at 77 K at the facet line is more than 10% higher for applied fields between 0.2 T and 2.5 T. The effect of the J (c)-B relationship of the facet line on the overall trapped field measured in an individual bulk sample was investigated by measuring the magnitudes of trapped fields and their contour maps for sections cut from four single grain samples of GdBCO-Ag at different sizes and shapes parallel to the ab-plane from the top to the bottom of the bulk sample. Based on the results reported here, we demonstrate a method to achieve more uniform trapped fields through an optimal arrangement of an assembly of sections of individual GdBCO single grains.

Automated summary

This paper systematically investigates the distribution of J(c)-B along a vertical cross-section and the facet line of a seed crystal in a Gd-Ba-Cu-O sample at 77 K. The results show that the J(c)-B at the facet line is more than 10% higher than that at the seed for applied fields between 0.2 T and 2.5 T. The study also demonstrates that a more uniform trapped magnetic field can be achieved by optimizing the arrangement of individual GdBCO single grains.