| 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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Spreitzer, Matjaž
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (18/18 displayed)
- 2024Characterization and Mechanical Properties of Sintered Clay Minerals
- 2024Thermally Stable Capacitive Energy-Density and Colossal Electrocaloric and Pyroelectric Effects of Sm-Doped Pb(Mg 1/3 Nb 2/3 )O 3 –PbTiO 3 Thin Filmscitations
- 2023Epitaxial oxides on semiconductors: growth perspectives and device applications
- 2023Non-stoichiometry and its implications for the properties of PMN–PT thin filmscitations
- 2023Thermoelectric properties of pseudobrookite-based ceramics prepared from natural Fe-Ti-rich heavy mineral sand concentratecitations
- 2023Thermoelectric properties of pseudobrookite-based ceramics prepared from natural Fe-Ti-rich heavy mineral sand concentratecitations
- 2023Removal of copper and iron from ethanolic solutions by an anion exchange resin and its implication to rare-earth magnet recyclingcitations
- 2023Perpendicular magnetic anisotropy at room-temperature in sputtered a-Si/Ni/a-Si layered structure with thick Ni (nickel) layerscitations
- 2022The paradigm of the filler's dielectric permittivity and aspect ratio in high-k polymer nanocomposites for energy storage applicationscitations
- 2022Novel lead-free BCZT-based ceramic with thermally-stable recovered energy density and increased energy storage efficiencycitations
- 2022A flexible self-poled piezocomposite nanogenerator based on H 2 (Zr 0.1 Ti 0.9 ) 3 O 7 nanowires and polylactic acid biopolymercitations
- 2022Large imprint in epitaxial 0.67Pb(Mg<sub>1/3</sub>Nb<sub>2/3</sub>)O<sub>3</sub>-0.33PbTiO<sub>3</sub> thin films for piezoelectric energy harvesting applicationscitations
- 2022The paradigm of the filler's dielectric permittivity and aspect ratio in high- k polymer nanocomposites for energy storage applicationscitations
- 2022Solvothermal synthesis of zinc- and gallium-substituted cobalt ferrite nanoparticles
- 2021Synthesis, structure and electrochemical performance of NiMn2O4
- 2021The influence of heteroatoms on physicochemical properties of cobalt ferrite nanoparticles
- 2021Dielectric properties of upside-down SrTiO3/Li2MoO4 composites fabricated at room temperaturecitations
- 2021Innovative Gold/Cobalt Ferrite Nanocomposite: Physicochemical and Cytotoxicity Propertiescitations
Places of action
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article
Dielectric properties of upside-down SrTiO3/Li2MoO4 composites fabricated at room temperature
Abstract
n this paper, ceramic upside-down lithium molybdate-strontium titanate (LMO-ST) composites fabricated at room temperature are described. Room temperature fabrication (RTF) is a promising alternative to the time- and energy-consuming high-temperature sintering of electroceramics, which involves mixing of the initial phases, molding with a steel dye, pressing, and drying, while in the last two phases the action of densification takes place. The LMO-ST composites are based on a high ratio of filler ST, coupled with the corresponding LMO binder. Part of the binder is admixed to the ceramic particles and additional part is added as a saturated aqueous solution, which crystallizes during pressing and drying, leading to its deposition on the surface of the filler particles. As a result, sufficient binding with 76—84% relative density was achieved. The deeper insight into the method was provided by various processing aspects and corresponding microstructural investigations. The particle size distribution, pressure, pressing time, ultrasonic treatment, drying time and processing conditions were optimized to obtain improved functional properties of the LMO-ST composites. The results of this study with relative permittivity in the range of 65—78 and dielectric loss tangent values of 0.002—0.05 can attract considerable attention for the use of LMO-ST composites in the industry of electroceramics.