Abstract
We have observed the flux motion using Hall probe sensors that are placed on the surface of high quality Y-Ba-Cu-O and Gd-Ba-Cu-O disks 15 mm in diameter with 0.95 mm thickness with applying pulsed magnetic field. The peak value of the field was varied from 0.1 to 0.8 T. The effects of static bias fields was also studied in the field range of 0-3 T at 77 K. Gd-Ba-Cu-O shows the clear secondary peak effect on the Jc-B curve so that the pinning property was different from Y-Ba-Cu-O for which Jc monotonically decreases with field. The flux motion was enhanced in Y-Ba-Cu-O with increasing static bias field, while that was suppressed in Gd-Ba-Cu-O, reflecting the secondary peak effect.
| Original language | English |
|---|---|
| Pages (from-to) | 391-395 |
| Number of pages | 5 |
| Journal | Physica C: Superconductivity and its Applications |
| Volume | 392-396 |
| Issue number | PART 1 |
| DOIs | |
| Publication status | Published - 2003 Oct |
| Externally published | Yes |
Fingerprint
Keywords
- GdBaCu O
- Peak effect
- Pulsed-magnetic magnetization
- YBaCuO
ASJC Scopus subject areas
- Condensed Matter Physics
Cite this
Effect of pinning on the flux motion of Gd-Ba-Cu-O bulk superconductors. / Yoshizawa, K.; Nariki, S.; Murakami, Masato; Takizawa, T.
In: Physica C: Superconductivity and its Applications, Vol. 392-396, No. PART 1, 10.2003, p. 391-395.Research output: Contribution to journal › Article
}
TY - JOUR
T1 - Effect of pinning on the flux motion of Gd-Ba-Cu-O bulk superconductors
AU - Yoshizawa, K.
AU - Nariki, S.
AU - Murakami, Masato
AU - Takizawa, T.
PY - 2003/10
Y1 - 2003/10
N2 - We have observed the flux motion using Hall probe sensors that are placed on the surface of high quality Y-Ba-Cu-O and Gd-Ba-Cu-O disks 15 mm in diameter with 0.95 mm thickness with applying pulsed magnetic field. The peak value of the field was varied from 0.1 to 0.8 T. The effects of static bias fields was also studied in the field range of 0-3 T at 77 K. Gd-Ba-Cu-O shows the clear secondary peak effect on the Jc-B curve so that the pinning property was different from Y-Ba-Cu-O for which Jc monotonically decreases with field. The flux motion was enhanced in Y-Ba-Cu-O with increasing static bias field, while that was suppressed in Gd-Ba-Cu-O, reflecting the secondary peak effect.
AB - We have observed the flux motion using Hall probe sensors that are placed on the surface of high quality Y-Ba-Cu-O and Gd-Ba-Cu-O disks 15 mm in diameter with 0.95 mm thickness with applying pulsed magnetic field. The peak value of the field was varied from 0.1 to 0.8 T. The effects of static bias fields was also studied in the field range of 0-3 T at 77 K. Gd-Ba-Cu-O shows the clear secondary peak effect on the Jc-B curve so that the pinning property was different from Y-Ba-Cu-O for which Jc monotonically decreases with field. The flux motion was enhanced in Y-Ba-Cu-O with increasing static bias field, while that was suppressed in Gd-Ba-Cu-O, reflecting the secondary peak effect.
KW - GdBaCu O
KW - Peak effect
KW - Pulsed-magnetic magnetization
KW - YBaCuO
UR - http://www.scopus.com/inward/record.url?scp=0043192503&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0043192503&partnerID=8YFLogxK
U2 - 10.1016/S0921-4534(03)01047-5
DO - 10.1016/S0921-4534(03)01047-5
M3 - Article
AN - SCOPUS:0043192503
VL - 392-396
SP - 391
EP - 395
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
SN - 0921-4534
IS - PART 1
ER -