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The Effect of Infiltration Temperature on the Microstructure and Magnetic Levitation Force of Single-Domain YBaCuO Bulk Superconductors Grown by a Modified Y+011 IG Method.

作者信息

Maimaiti Nuerseman, Abulaiti Abulizi, Yang Wanmin

机构信息

School of Traffic and Transportation Engineering, Xinjiang University, Urumqi 830017, China.

School of Electrical Engineering, Xinjiang University, Urumqi 830017, China.

出版信息

Nanomaterials (Basel). 2024 Dec 27;15(1):21. doi: 10.3390/nano15010021.

DOI:10.3390/nano15010021
PMID:39791781
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11722132/
Abstract

During the preparation of single-domain (S-D) REBaCuO (RE-123) superconducting bulks, the seed crystals can serve as templates for crystal growth, guiding the newly formed crystals to grow in a specific direction, thereby ensuring the consistency of the crystal orientation within the sample. However, the infiltration temperature is typically restricted to approximately 1050 °C when employing NdBaCuO (Nd-123) crystal seeds in the traditional top-seeded infiltration growth (TSIG) technique for producing single-domain Y-123 bulk superconductors. In the present study, to overcome the temperature limitations of the heat treatment process, the optimized YO +011 IG (011 refers to BaCuO powder) method was employed to fabricate a group of single-domain Y-123 bulks with a high-temperature infiltration (1000-1300 °C). The reason for the differences in the superconducting properties between the different samples was analyzed by studying the relationship between the microstructure of the infiltrated pellet and the final Y-123 sample. The research findings were as follows: (1) when the infiltration temperature exceeded 1150 °C, the successful preparation of single-domain YBaCuO (Y-123) bulks became unattainable due to the coarsening or melting decomposition of the YBaCuO (Y-211) phase according to the SEM-EDS analysis; (2) the content of the Y-211 phase within the Y-123 matrix was approximately 40.8%, 37.2%, 32.7%, 30.5%, and 46.4% for the different final samples; (3) with an increasing infiltration temperature, the magnetic levitation forces exhibited an initial increase followed by a subsequent decline. The maximum levitation force of 47.1 N at 77 K was reached in the sample S3 infiltrated at 1100 °C.

摘要
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/881b99dadaa5/nanomaterials-15-00021-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/13251bf0dd43/nanomaterials-15-00021-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/c84604dea31f/nanomaterials-15-00021-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/fa9dd4f2db75/nanomaterials-15-00021-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/f945a8cbae46/nanomaterials-15-00021-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/bfbf7d730fc3/nanomaterials-15-00021-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/ec9d85fa9cfe/nanomaterials-15-00021-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/881b99dadaa5/nanomaterials-15-00021-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/13251bf0dd43/nanomaterials-15-00021-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/c84604dea31f/nanomaterials-15-00021-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/fa9dd4f2db75/nanomaterials-15-00021-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/f945a8cbae46/nanomaterials-15-00021-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/bfbf7d730fc3/nanomaterials-15-00021-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/ec9d85fa9cfe/nanomaterials-15-00021-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/faf5/11722132/881b99dadaa5/nanomaterials-15-00021-g007.jpg

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本文引用的文献

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High-temperature superconductor bulk magnets that can trap magnetic fields of over 17 tesla at 29 K.能够在29K温度下捕获超过17特斯拉磁场的高温超导块状磁体。
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New type of vortex pinning structure effective at very high magnetic fields.
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