4 research outputs found

    Crystal Structure and Li-Ion Transport in Li<sub>2</sub>CoPO<sub>4</sub>F High-Voltage Cathode Material for Li-Ion Batteries

    No full text
    In this work, we provide a structural and computational investigation of the Li<sub>2</sub>CoPO<sub>4</sub>F high-voltage cathode material by means of neutron powder diffraction (SG <i>Pnma</i>, <i>a</i> = 10.4528(2) Å, <i>b</i> = 6.38667(10) Å, <i>c</i> = 10.8764(2) Å, <i>R</i><sub>F</sub> = 0.0145), crystal chemistry approaches (Voronoi–Dirichlet partitioning and bond valence sums mapping), and density functional theory. The material reveals low energy barriers (0.12–0.43 eV) of Li hopping and a possible 3D channel system for Li-ion migration. It is found that only one Li per formula unit can be extracted within the potential stability window of the commercially available electrolytes. The interrelation between dimensionality, topology and energetics of Li-ion diffusion and peculiarities of the Li<sub>2</sub>CoPO<sub>4</sub>F crystal structure are discussed in detail

    Crystal Structure and Li-Ion Transport in Li<sub>2</sub>CoPO<sub>4</sub>F High-Voltage Cathode Material for Li-Ion Batteries

    No full text
    In this work, we provide a structural and computational investigation of the Li<sub>2</sub>CoPO<sub>4</sub>F high-voltage cathode material by means of neutron powder diffraction (SG <i>Pnma</i>, <i>a</i> = 10.4528(2) Å, <i>b</i> = 6.38667(10) Å, <i>c</i> = 10.8764(2) Å, <i>R</i><sub>F</sub> = 0.0145), crystal chemistry approaches (Voronoi–Dirichlet partitioning and bond valence sums mapping), and density functional theory. The material reveals low energy barriers (0.12–0.43 eV) of Li hopping and a possible 3D channel system for Li-ion migration. It is found that only one Li per formula unit can be extracted within the potential stability window of the commercially available electrolytes. The interrelation between dimensionality, topology and energetics of Li-ion diffusion and peculiarities of the Li<sub>2</sub>CoPO<sub>4</sub>F crystal structure are discussed in detail

    Ionic Conductivity in Ti-Doped KFeO<sub>2</sub>: Experiment and Mathematical Modeling

    No full text
    The structure peculiarities of K<sub>0.9</sub>Fe<sub>0.9</sub>Ti<sub>0.1</sub>O<sub>2</sub> that favor the emergence of a superionic state have been studied using neutron powder diffraction data as a function of temperature. The migration paths in the structure of both undoped and doped potassium ferrite were modeled by topological (tiling) and DFT methods. It is shown that heating of the low-temperature phase leads to increase of the ionic conductivity thanks to widening the migration channels and the appearance of thermally induced cation vacancies. The calculated migration barrier is found to not exceed 0.3 eV/ion in all phases, which is consistent with the experimental data. Doping also increases the ionic conductivity, but up to about 10% of Ti only; then the experimental activation energy even increases. The DFT modeling shows that it can be caused by growth of the regions unavailable for the mobile cations; the regions are formed around the dopant atoms

    Ionic Conductivity in Ti-Doped KFeO<sub>2</sub>: Experiment and Mathematical Modeling

    No full text
    The structure peculiarities of K<sub>0.9</sub>Fe<sub>0.9</sub>Ti<sub>0.1</sub>O<sub>2</sub> that favor the emergence of a superionic state have been studied using neutron powder diffraction data as a function of temperature. The migration paths in the structure of both undoped and doped potassium ferrite were modeled by topological (tiling) and DFT methods. It is shown that heating of the low-temperature phase leads to increase of the ionic conductivity thanks to widening the migration channels and the appearance of thermally induced cation vacancies. The calculated migration barrier is found to not exceed 0.3 eV/ion in all phases, which is consistent with the experimental data. Doping also increases the ionic conductivity, but up to about 10% of Ti only; then the experimental activation energy even increases. The DFT modeling shows that it can be caused by growth of the regions unavailable for the mobile cations; the regions are formed around the dopant atoms
    corecore