| People | Locations | Statistics |
|---|---|---|
| Naji, M. |
| |
| Motta, Antonella |
| |
| Aletan, Dirar |
| |
| Mohamed, Tarek |
| |
| Ertürk, Emre |
| |
| Taccardi, Nicola |
| |
| Kononenko, Denys |
| |
| Petrov, R. H. | Madrid |
|
| Alshaaer, Mazen | Brussels |
|
| Bih, L. |
| |
| Casati, R. |
| |
| Muller, Hermance |
| |
| Kočí, Jan | Prague |
|
| Šuljagić, Marija |
| |
| Kalteremidou, Kalliopi-Artemi | Brussels |
|
| Azam, Siraj |
| |
| Ospanova, Alyiya |
| |
| Blanpain, Bart |
| |
| Ali, M. A. |
| |
| Popa, V. |
| |
| Rančić, M. |
| |
| Ollier, Nadège |
| |
| Azevedo, Nuno Monteiro |
| |
| Landes, Michael |
| |
| Rignanese, Gian-Marco |
|
Driessche, I. Van
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (2/2 displayed)
- 2020Effect of oxygenation process on flux pinning in pristine and BaHfO<sub>3</sub> nanocomposite GdBa<sub>2</sub>Cu<sub>3</sub>O<sub>7</sub> superconducting thin filmscitations
- 2020Importance of the pyrolysis for microstructure and superconducting properties of CSD-grown GdBa$_{2}$Cu$_{3}$O$_{7-x}$-HfO$_{2}$ nanocomposite films by the ex-situ approachcitations
Places of action
| Organizations | Location | People |
|---|
article
Effect of oxygenation process on flux pinning in pristine and BaHfO<sub>3</sub> nanocomposite GdBa<sub>2</sub>Cu<sub>3</sub>O<sub>7</sub> superconducting thin films
Abstract
<jats:title>Abstract</jats:title><jats:p>Pristine and BaHfO<jats:sub>3</jats:sub> (BHO) nanocomposite GdBa<jats:sub>2</jats:sub>Cu<jats:sub>3</jats:sub>O<jats:sub>7</jats:sub> (GdBCO) superconducting thin films were deposited at 800 °C, 0.4 mbar O<jats:sub>2</jats:sub> partial pressure using a Nd:YAG laser (λ=355 nm) with 10 Hz frequency on MgO substrate. The influence of the oxygenation process on flux pinning and electrical transport properties was investigated by changing the annealing temperature (<jats:italic>T</jats:italic><jats:sub>ann</jats:sub>) between 450 °C and 780 °C and the holding time (<jats:italic>t</jats:italic><jats:sub>hold</jats:sub>) between 10 and 30 min. The irreversibility field shows the largest shift toward higher fields for <jats:italic>T</jats:italic><jats:sub>ann</jats:sub> = 450 °C and thus the largest in-field <jats:italic>J</jats:italic><jats:sub>c</jats:sub>. Angular dependence of <jats:italic>J</jats:italic><jats:sub>c</jats:sub> for most of the pristine GdBCO films exhibits a large peak for <jats:italic>B</jats:italic>‖<jats:italic>c</jats:italic>, however the sample with <jats:italic>T</jats:italic><jats:sub>ann</jats:sub> = 550 °C has a large peak in the 90°-120° region, i.e. near <jats:italic>B</jats:italic> ‖ <jats:italic>ab</jats:italic>. For BHO nanocomposites, a decrease in <jats:italic>T</jats:italic><jats:sub>ann</jats:sub> increases in-field <jats:italic>J</jats:italic><jats:sub>c</jats:sub> by a factor of 2.</jats:p>