Abstract

Bulk (RE)BCO, where RE is a rare-earth element or yttrium, superconductors fabricated in the form of rings are potentially useful for a variety of solenoidal-type applications, such as small, high field nuclear magnetic resonance and electromagnetic undulators. It is anticipated that the practical exploitation of these technologically important materials will involve pulse field magnetization (PFM) and, consequently, it is important to understand the behavior of ring-shaped samples subjected to the PFM process. Macroscopic flux jumps were observed in PFM experiments on ring-shaped bulk samples when the peak applied field reaches a threshold magnitude, similar to behavior reported previously in cylindrical samples. Magnetic flux jumps inward when the thermal instability is triggered, however it subsequently flows outwards from the sample, resulting in a relatively low trapped field. This behavior is attributed to a variety of effects, including the inhomogeneity of the material, which may lead to the formation of localized hot spots during the PFM process. In order to further elucidate this phenomena, the properties of a structure consisting of a bulk superconducting ring with a cylindrical superconductor core were studied. We observe that, although a flux jump occurs consistently in the ring, a critical state is established at the boundary of the ring-shaped sample and the core. We provide a detailed account of these experimental observations and provide an explanation in terms of the current understanding of the PFM process.

Highlights

  • Bulk superconductors have the ability to trap large magnetic field and may be used potentially as cryo-permanent magnets

  • It can be seen that the flux jump occurs only within the region of the ring, and the core remains in a critical state during the entire pulse field magnetization (PFM) process

  • Flux jumps have been observed during the PFM process for both ring-shaped samples and assembled samples

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Summary

Introduction

Bulk superconductors have the ability to trap large magnetic field and may be used potentially as cryo-permanent magnets. Overall, it is possible to achieve a trapped field profile after PFM that is characterised by a single peak for a single grain bulk sample, as is obtained generally in a field-cooled (FC) process. At lower temperatures, flux jumps are prone to occur at the outer region of the bulk superconductor, which leads to two distinct and separated peaks in the trapped field profile.

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