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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Zou, Jin
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (26/26 displayed)
- 2022TiB reinforced lattice structures produced by laser powder bed fusion with high elastic admissible straincitations
- 2022High strength and ductility of titanium matrix composites by nanoscale design in selective laser meltingcitations
- 2020Tib nanowhisker reinforced titanium matrix composite with improved hardness for biomedical applicationscitations
- 2018Continuous flow synthesis of phosphate binding h-BN@magnetite hybrid materialcitations
- 2015Pulsed Field Magnetization of Single-Grain Bulk YBCO Processed from Graded Precursor Powderscitations
- 2011Superstructure formation and variation in Ni-GDC cermet anodes in SOFCcitations
- 2011Direct evidence of dopant segregation in Gd-doped ceriacitations
- 2011The diffusions and associated interfacial layer formation between thin film electrolyte and cermet anode in IT-SOFCcitations
- 2011Diffusion and segregation along grain boundary at the electrolyte–anode interface in IT-SOFCcitations
- 2011Two types of diffusions at the cathode/electrolyte interface in IT-SOFCscitations
- 2011Compound semiconductor nanowires for optoelectronic device applications
- 2011Mutual diffusion occurring at the interface between La0.6Sr0.4Co0.8Fe0.2O3 cathode and Gd-doped ceria electrolyte during IT-SOFC cell preparationcitations
- 2011Mutual diffusion and microstructure evolution at the electrolyte−anode interface in intermediate temperature solid oxide fuel cellcitations
- 2011Growth and properties of III-V compound semiconductor heterostructure nanowirescitations
- 2011III-V semiconductor nanowires for optoelectronic device applicationscitations
- 2010Microstructural and chemical aspects of working-temperature aged Ca-doped CeO2citations
- 2009Carrier dynamics and quantum confinement in type II ZB-WZ InP nanowire homostructures
- 2009III-V compound semiconductor nanowires
- 2009Carrier Dynamics and Quantum Confinement in type II ZB-WZ InP Nanowire Homostructurescitations
- 2009Epitaxy of III-V semiconductor nanowires towards optoelectronic devices
- 2008High purity GaAs nanowires free of planar defectscitations
- 2003Multilayered carbon films for tribological applicationscitations
- 2002Structural disorder in ion-implanted AlxGa1-xNcitations
- 2001Effect of ion species on the accumulation of ion-beam damage in GaNcitations
- 2000Ion-beam-induced dissociation and bubble formation in GaNcitations
- 2000Surface disordering and nitrogen loss in GaN under ion bombardment
Places of action
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article
Pulsed Field Magnetization of Single-Grain Bulk YBCO Processed from Graded Precursor Powders
Abstract
<p>Large single-grain bulk higherature superconducting materials can trap high magnetic fields in comparison with conventional permanent magnets, making them ideal candidates to develop more compact and efficient devices, such as actuators, magnetic levitation systems, flywheel energy storage systems, and electric machines. However, macrosegregation of Y-211 inclusions in melt-processed Y-Ba-Cu-O (YBCO) limits the macroscopic critical current density of such bulk superconductors, and hence, the potential trapped field. A new fabrication technique using graded precursor powders has recently been developed by our research group, which results in a more uniform distribution of Y-211 particles, in order to further improve the superconducting properties and trapped field capability of such materials. In this paper, experimental results on the pulsed field magnetization of a graded single-grain YBCO bulk sample are presented. Pulsed fields of magnitude up to 5.5 T were applied to the sample, at temperatures of 40 and 65 K. The trapped field profiles indicate that magnetic flux enters the sample in a more uniform manner than standard YBCO samples, resulting in a higher overall trapped field and indicating the success of this processing technique to produce a more homogeneous sample.</p>