Magnetization Properties of YBaCuO Prepared by Quench and Melt Growth Process

S. Gotoh; M. Murakami; N. Koshizuka; S. Tanaka

doi:10.1109/TJMJ.1991.4565215

Magnetization Properties of YBaCuO Prepared by Quench and Melt Growth Process

S. Gotoh, M. Murakami, N. Koshizuka, S. Tanaka

Research output: Contribution to journal › Article › peer-review

Abstract

DC magnetization measurements were carried out on YBaCuO prepared by the quench and melt-growth (QMG) process using a vibrating sample magnetometer and a SQUID magnetometer below 100 K. It was found that the DC magnetization behavior of QMGgrown YBaCuO at 4.2 K can be quantitatively explained in terms of Bean 's critical state model. This sample also can become a strong bulk permanent magnet with an energy product of more than 80 MGOe at 5 K because of its strong pinning force.

Original language	English
Pages (from-to)	590-596
Number of pages	7
Journal	IEEE Translation Journal on Magnetics in Japan
Volume	6
Issue number	7
DOIs	https://doi.org/10.1109/TJMJ.1991.4565215
Publication status	Published - 1991 Jul
Externally published	Yes

ASJC Scopus subject areas

Engineering (miscellaneous)
Engineering(all)

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abstract = "DC magnetization measurements were carried out on YBaCuO prepared by the quench and melt-growth (QMG) process using a vibrating sample magnetometer and a SQUID magnetometer below 100 K. It was found that the DC magnetization behavior of QMGgrown YBaCuO at 4.2 K can be quantitatively explained in terms of Bean 's critical state model. This sample also can become a strong bulk permanent magnet with an energy product of more than 80 MGOe at 5 K because of its strong pinning force.",

author = "S. Gotoh and M. Murakami and N. Koshizuka and S. Tanaka",

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AU - Tanaka, S.

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AB - DC magnetization measurements were carried out on YBaCuO prepared by the quench and melt-growth (QMG) process using a vibrating sample magnetometer and a SQUID magnetometer below 100 K. It was found that the DC magnetization behavior of QMGgrown YBaCuO at 4.2 K can be quantitatively explained in terms of Bean 's critical state model. This sample also can become a strong bulk permanent magnet with an energy product of more than 80 MGOe at 5 K because of its strong pinning force.

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