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
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) Ã…, <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
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) Ã…, <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
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
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