| People | Locations | Statistics |
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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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Palau, Anna
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (32/32 displayed)
- 2024Progress in superconducting REBa2Cu3O7 (RE = rare earth) coated conductors derived from fluorinated solutionscitations
- 2024Tuning the superconducting performance of YBa2Cu3O7-δ films through field-induced oxygen dopingcitations
- 2023On the Role of the Sr3−xCaxAl2O6 Sacrificial Layer Composition in Epitaxial La0.7Sr0.3MnO3 Membranescitations
- 2023On the Role of the Sr3−xCaxAl2O6 Sacrificial Layer Composition in Epitaxial La0.7Sr0.3MnO3 Membranescitations
- 2023Chemical Synthesis of La0.75Sr0.25CrO3 Thin Films for p-Type Transparent Conducting Electrodescitations
- 2022Investigation of diethanolamine (DEA) as a chelating agent in the fabrication of fluorine-free propionate route YBa2Cu3O7 (YBCO) thin filmscitations
- 2022Optimizing vortex pinning in YBa2Cu3O7-x superconducting films up to high magnetic fieldscitations
- 2022Investigation of diethanolamine (DEA) as a chelating agent in the fabrication of fluorine-free propionate route YBa 2 Cu 3 O 7 (YBCO) thin filmscitations
- 2022Influence of growth temperature on the pinning landscape of YBa 2 Cu 3 O 7− δ films grown from Ba-deficient solutionscitations
- 2022Influence of growth temperature on the pinning landscape of YBa<sub>2</sub>Cu<sub>3</sub>O<sub>7−</sub> <sub>δ</sub> films grown from Ba-deficient solutionscitations
- 2022Influence of growth temperature on the pinning landscape of YBa2Cu3O7−δ films grown from Ba-deficient solutionscitations
- 2021High Performance of Superconducting YBa2Cu3O7 Thick Films Prepared by Single-Deposition Inkjet Printingcitations
- 2021High Performance of Superconducting YBa2Cu3O7 Thick Films Prepared by Single-Deposition Inkjet Printing
- 2020Vortex pinning properties at dc and microwave frequencies of YBa2Cu3O7-x films with nanorods and nanoparticles
- 2020Nanoscale Correlations between Metal–Insulator Transition and Resistive Switching Eect in Metallic Perovskite Oxides
- 2020Suppression of superconductivity at the nanoscale in chemical solution derived YBa2Cu3O7−δ thin films with defective Y2Ba4Cu8O16 intergrowths
- 2020Nanoscale correlations between metal-insulator transition and resistive switching effect in metallic perovskite oxidescitations
- 2019Control of nanostructure and pinning properties in solution deposited YBa2Cu3O7−x nanocomposites with preformed perovskite nanoparticles
- 2019Control of nanostructure and pinning properties in solution deposited YBaCuO nanocomposites with preformed perovskite nanoparticles
- 2019Accelerated growth by flash heating of high critical current Trifluoroacetate solution derived epitaxial superconducting YBa2Cu3O7 filmscitations
- 2018Epitaxial superconducting GdBa2Cu3O7−δ /Gd2O3 nanocomposite thin films from advanced low-fluorine solutionscitations
- 2018Epitaxial YBa2Cu3O7−x nanocomposite films and coated conductors from BaMO3 (M = Zr, Hf) colloidal solutions
- 2017Epitaxial superconducting GdBa2Cu3O7−δ/Gd2O3 nanocomposite thin films from advanced low-fluorine solutions
- 2017Untangling surface oxygen exchange effects in YBa2Cu3O6+x thin films by electrical conductivity relaxationcitations
- 2017Untangling surface oxygen exchange effects in YBa2Cu3O6+x thin films by electrical conductivity relaxationcitations
- 2017Inkjet-printed chemical solution Y₂O₃ layers for planarization of technical substratescitations
- 2017Epitaxial superconducting GdBa2Cu3O7−δ /Gd2O3 nanocomposite thin films from advanced low-fluorine solutionscitations
- 2016Superconducting YBa 2 Cu 3 O 7–δ Nanocomposites Using Preformed ZrO 2 Nanocrystals: Growth Mechanisms and Vortex Pinning Propertiescitations
- 2016Encoding magnetic states in monopole-like configurations using superconducting dotscitations
- 2016Emerging Diluted Ferromagnetism in High- Tc Superconductors Driven by Point Defect Clusterscitations
- 2016Encoding Magnetic States in Monopole-Like Configurations Using Superconducting Dotscitations
- 2013Solution-derived YBa2Cu3O7 nanocomposite films with a Ba2YTaO6 secondary phase for improved superconducting propertiescitations
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article
Influence of growth temperature on the pinning landscape of YBa<sub>2</sub>Cu<sub>3</sub>O<sub>7−</sub> <sub>δ</sub> films grown from Ba-deficient solutions
Abstract
<jats:title>Abstract</jats:title><jats:p>Cuprate coated conductors are promising materials for the development of large-scale applications, having superior performance over other superconductors. Tailoring their vortex pinning landscape through nanostructure engineering is one of the major challenges to fulfill the specific application requirements. In this work, we have studied the influence of the growth temperature on the generation of intrinsic pinning defects in YBa<jats:sub>2</jats:sub>Cu<jats:sub>3</jats:sub>O<jats:sub>7−<jats:italic>δ</jats:italic></jats:sub> films grown by chemical solution deposition using low Ba precursor solutions. We have analysed the critical current density as a function of the temperature, applied magnetic field magnitude and orientation, <jats:italic>J</jats:italic><jats:sub>c</jats:sub>(<jats:italic>T,H,θ</jats:italic>), to elucidate the nature and strength of pinning sites and correlate the microstructure of the films with their superconducting performance. An efficient pinning landscape consisting of stacking faults and associated nanostrain is naturally induced by simply tuning the growth temperature without the need to add artificial pinning sites. Samples grown at an optimized temperature of 750 °C show very high self-field <jats:italic>J</jats:italic><jats:sub>c</jats:sub> values correlated with an overdoped state and improved <jats:italic>J</jats:italic><jats:sub>c</jats:sub>(<jats:italic>T,H,θ</jats:italic>) performances.</jats:p>