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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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Heitjans, Paul
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (21/21 displayed)
- 2023Lithium Niobate for Fast Cycling in Li-ion Batteries: Review and New Experimental Resultscitations
- 2018Ion dynamics in a new class of materials: nanoglassy lithium alumosilicates
- 2017Structure and ion dynamics of mechanosynthesized oxides and fluorides
- 2016Single-crystal neutron diffraction on γ-LiAlO2: structure determination and estimation of lithium diffusion pathway
- 2016A novel low-temperature solid-state route for nanostructured cubic garnet Li 7 La 3 Zr 2 O 12 and its application to Li-ion battery
- 2016Solid-state diffusion and NMR
- 2015Synthesis and Electrochemical Behavior of Nanostructured Copper Particles on Graphite for Application in Lithium Ion Batteries
- 2015A simple and straightforward mechanochemical synthesis of the far-from-equilibrium zinc aluminate, ZnAl2O4, and its response to thermal treatment
- 2014Theoretical study of Li migration in lithium-graphite intercalation compounds with dispersion-corrected DFT methodscitations
- 2012The ionic conductivity in lithium-boron oxide materials and its relation to structural, electronic and defect propertiescitations
- 2012Self-diffusion of lithium in amorphous lithium niobate layers
- 2011Structure and dynamics of the fast lithium ion conductor "li 7La3Zr2O12"
- 2010Mössbauer Spectroscopy for Studying Chemical Reactions
- 2010Ion Transport Properties of the Inverse Perovskite BaLiF3 Prepared by High-Energy Ball Milling
- 2009Li Ion diffusion in nanocrystalline and nanoglassy LiAISi2O 6 and LiBO2 - Structure dynamics relations in two glass forming compounds
- 2007Enhanced conductivity at the interface of Li2O:B2O3 nanocompositescitations
- 2007Enhanced conductivity at the interface of Li2O:B2O3 nanocomposites: Atomistic models
- 2005Ion hopping in crystalline and glassy spodumene LiAlSi2O6: Li7 spin-lattice relaxation and Li7 echo NMR spectroscopy
- 2005Fast dynamics of H2O in hydrous aluminosilicate glasses studied with quasielastic neutron scattering
- 2005Solid-State Diffusion and NMR
- 2000Nanocrystalline versus microcrystalline Lo2O:B2O 3 composites: Anomalous ionic conductivities and percolation theory
Places of action
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article
Ion Transport Properties of the Inverse Perovskite BaLiF3 Prepared by High-Energy Ball Milling
Abstract
For many applications such as advanced energy storage systems, chemical sensors or electrochromic devices fast ionic conduction plays an important role. In many cases, see e.g., Refs. [1-3], nanocrystalline ceramics with crystallite diameters smaller than 50 nm show an enhanced ion conductivity compared to their coarse-grained counterparts, i.e., single crystals or materials with µm-sized particles. This observation can be explained by their large fraction of structurally disordered interfacial regions providing fast migration pathways for the ions [2,3]. Mechanical treatment of µm-sized particles in a high-energy ball mill represents a simple technique to obtain large quantities of a nanocrystalline material. In addition to that it is also possible to synthesize ceramics directly by ball milling [3]. In many cases this leads to metastable, non-equilibrium compounds which cannot be prepared following conventional synthesis methods [4,5]. In the present paper, BaLiF3, the only known inverted perovskite of the AMF3 compounds [6], was prepared by high-energy ball milling using a Fritsch P7 planetary mill (premium line). An equimolar mixture of LiF and BaF2 with an overall mass of 2 g was treated in a 45 mL zirconia vial with 140 balls of the same material for 3 h at a rotational speed of 600 rpm. As verified by X-ray diffraction highly pure BaLiF3 is obtained which shows an average crystallite size d of about 30 nm. d was estimated