Abstract

The trapped field distributions on the surface of MTG YBCO disks were measured by a Hall probe automated scanning system, and exhibit a cone profile for sample A with levitation force up to 12.6 N/cm 2, whereas four peaks for sample B with 4.4 N/cm 2. However, c-axis orientations of two samples are all perpendicular to the sample surfaces according to the pole figure. For sample B, the boundaries between the sectors seem to be weak links, and the T c in the sector, which is very low, is higher than that in the boundary. The microstructure reveals that the agglomerates of non-superconductive phases occur in the boundary and the center for sample B, but do not occur in the sectors of sample B and nor in any part of sample A. So, it can be assumed that the agglomerates of non-superconductive phases in the boundary are mainly responsible for the low levitation force and trapped field with four peaks in distribution of sample B.

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