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 QMG-grown YBaCuO at 4.2 K can be quantitatively explained in terms of C. P. Bean's critical state model (1962). 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 | |
| Publication status | Published - 1991 Jul |
| Externally published | Yes |
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Magnetization properties of YBaCuO prepared by quench and melt growth process. / Gotoh, S.; Murakami, Masato; Koshizuka, N.; Tanaka, S.
In: IEEE Translation Journal on Magnetics in Japan, Vol. 6, No. 7, 07.1991, p. 590-596.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Magnetization properties of YBaCuO prepared by quench and melt growth process
AU - Gotoh, S.
AU - Murakami, Masato
AU - Koshizuka, N.
AU - Tanaka, S.
PY - 1991/7
Y1 - 1991/7
N2 - 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 QMG-grown YBaCuO at 4.2 K can be quantitatively explained in terms of C. P. Bean's critical state model (1962). 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.
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 QMG-grown YBaCuO at 4.2 K can be quantitatively explained in terms of C. P. Bean's critical state model (1962). 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.
UR - http://www.scopus.com/inward/record.url?scp=0026193701&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0026193701&partnerID=8YFLogxK
U2 - 10.1109/TJMJ.1991.4565215
DO - 10.1109/TJMJ.1991.4565215
M3 - Article
VL - 6
SP - 590
EP - 596
JO - IEEE Translation Journal on Magnetics in Japan
JF - IEEE Translation Journal on Magnetics in Japan
SN - 0882-4959
IS - 7
ER -