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 |
|
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
Organizations | Location | People |
---|
article
The ionic conductivity in lithium-boron oxide materials and its relation to structural, electronic and defect properties
Abstract
<p>We review recent theoretical studies on ion diffusion in (Li<sub>2</sub>O)<sub>x</sub>(B<sub>2</sub>O<sub>3</sub>)<sub>1x</sub>compounds and at the interfaces of Li<sub>2</sub>O :B<sub>2</sub>O<sub>3</sub>nanocomposite. The investigations were performed theoretically using DFT and HF/DFT hybrid methods with VASP and CRYSTAL codes. For the pure compound B<sub>2</sub>O<sub>3</sub>, it was theoretically confirmed that the low-pressure phase B<sub>2</sub>O<sub>3</sub>I has space group P3<sub>1</sub>21. For the first time, the structure, stability and electronic properties of various low-index surfaces of trigonal B<sub>2</sub>O<sub>3</sub>I were investigated at the same theoretical level. The (101) surface is the most stable among the considered surfaces. Ionic conductivity was investigated systematically in Li<sub>2</sub>O, LiBO<sub>2</sub>, and Li<sub>2</sub>B<sub>4</sub>O<sub>7</sub>solids and in Li<sub>2</sub>O:B<sub>2</sub>O<sub>3</sub>nanocomposites by calculating the activation energy (E<sub>A</sub>) for cation diffusion. The Li<sup>+</sup>ion migrates in an almost straight line in Li<sub>2</sub>O bulk whereas it moves in a zig-zag pathway along a direction parallel to the surface plane in Li<sub>2</sub>O surfaces. For LiBO<sub>2</sub>, the migration along the c direction (E<sub>A</sub>=0.55eV) is slightly less preferable than that in the xy plane (E<sub>A</sub>=0.430.54eV). In Li<sub>2</sub>B<sub>4</sub>O<sub>7</sub>, the Li<sup>+</sup>ion migrates through the large triangular faces of the two nearest oxygen five-vertex polyhedra facing each other where E<sub>A</sub>is in the range of 0.270.37eV. A two-dimensional model system of the Li<sub>2</sub>O :B<sub>2</sub>O<sub>3</sub>interface region was created by the combination of supercells of the Li<sub>2</sub>O (111) surface and the B<sub>2</sub>O<sub>3</sub>(001) surface. It was found that the interface region of the Li<sub>2</sub>O :B<sub>2</sub>O<sub>3</sub>nanocomposite is more defective than Li<sub>2</sub>O bulk, which facilitates the conductivity in this region. In addition, the activation energy (E<sub>A</sub>) for local hopping processes is smaller in the Li<sub>2</sub>O :B...