| |
Tuesday, 08/19/08
| Session Title: |
Flux Pinning and Dynamics II - Engineered Pinning Arrangements |
|
Session Chairs: |
Paul Barnes, Air Force Research Laboratory, Wright-Patterson AFB & Takanobu Kiss, Kyushu University
|
| Paper Number: |
2MPD03 |
| Start Time: |
10:00am |
| Session Type: |
Poster |
Difference between BaSnO3 and BaZrO3 nano-rods for c-axis correlated pinning properties in REBa2Cu3Oy
M. Namba, S. Awaji, K. Watanabe, HFLSM, IMR, Tohoku Univ.; H. Kai, S. Yasunaga, M. Mukaida, Kyushu Univ.
|
The introduction of the c-axis correlated disorder is a promising technique for the improvement of the critical current density Jc at B//c for the REBa2Cu3Oy (RE123) films and tapes. In particular, for the RE123 film with BaZrO3, the columnar shaped BaZrO3 precipitate, called nano-rods, can be introduced as the c-axis correlated pinning centers. Recently, it is found that the BaSnO3 nano-rods can be introduced in RE123 films with a slight decrease of Tc in comparison with BaZrO3. In order to understand the vortex pinning state by BaSnO3 nano-rods, the angular dependence of Jc was measured in detail for Er123 films with BaSnO3 prepared by pulsed laser deposition. The peak at the parallel external field to the c-axis (B//c) in the angular dependence of Jc appears in a wide magnetic field region from the low magnetic field to the irreversible field at various temperatures, although it disappears in a high field region in the case of the BaZrO3 nano-rods. Hence, we found that the c-axis correlated pinning properties for two kinds of nano-rods are different each other at the high magnetic field. The different behavior of the c-axis correlated pinning may be related with the alignment of the nano-rods.
|
|
|
|
|
 |
|