Abstract

The use of RE-Ba–Cu–O [(RE)BCO] bulk superconductors, where RE = Y, Gd, Sm, in practical applications is, at least in part, limited by their mechanical properties and brittle nature, in particular. Alloying these materials with silver, however, produces a significant improvement in strength without any detrimental impact on their superconducting properties. Unfortunately, the top seeded melt growth technique, used routinely to process bulk (RE)BCO superconductors in the form of large, single grains required for practical applications, is complex and has a large number of inter-related variables, so the addition of silver increases the complexity of the growth process even further. This can make successful growth of this system extremely challenging. Here we report measurements of the growth rate of YBCO-Ag fabricated using a new growth technique consisting of continuous cooling and isothermal hold process. The resulting data form the basis of a model that has been used to derive suitable heating profiles for the successful single grain growth of YBCO-Ag bulk superconductors of up to 26 mm in diameter. The microstructure and distribution of silver within these samples have been studied in detail. The maximum trapped field at the top surface of the bulk YBCO-Ag samples has been found to be comparable to that of standard YBCO processed without Ag. The YBCO-Ag samples also exhibit a much more uniform trapped field profile compared to that of YBCO.

Highlights

  • Single grain routinely to process bulk (RE)-Ba–Cu–O [(RE)BCO] bulk high temperature superconductors, where RE = Y, Gd or Sm, are able to trap large magnetic fields that are significantly larger than those generated by permanent magnets [1, 2]

  • The top seeded melt growth technique, used routinely to process bulk (RE)BCO superconductors in the form of large, single grains required for practical applications, is complex and has a large number of inter-related variables, so the addition of silver increases the complexity of the growth process even further

  • We recently reported detailed growth rate data for the YBCO-Ag system [25] and a new, two-stage method for the study of growth rate of the YBCO-Ag system; the so-called continuous cooling and isothermal hold (CCIH) technique

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Summary

Introduction

Single grain RE-Ba–Cu–O [(RE)BCO] bulk high temperature superconductors, where RE = Y, Gd or Sm, are able to trap large magnetic fields that are significantly larger than those generated by permanent magnets [1, 2]. Slow, controlled undercooling in the presence of a suitable seed crystal subsequently enables the nucleation and growth of a large, single grain composed of a continuous superconducting Y-123 matrix but containing a distribution of discrete, non-superconducting Y-211 phase inclusions [14, 18]

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