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Defects, Dopants and Lithium Mobility in Li(9)V(3)(P(2)O(7))(3)(PO(4))(2)

Layered Li(9)V(3)(P(2)O(7))(3)(PO(4))(2) has attracted considerable interest as a novel cathode material for potential use in rechargeable lithium batteries. The defect chemistry, doping behavior and lithium diffusion paths in Li(9)V(3)(P(2)O(7))(3)(PO(4))(2) are investigated using atomistic scale s...

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Detalles Bibliográficos
Autores principales: Kuganathan, Navaratnarajah, Ganeshalingam, Sashikesh, Chroneos, Alexander
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5970228/
https://www.ncbi.nlm.nih.gov/pubmed/29802297
http://dx.doi.org/10.1038/s41598-018-26597-w
Descripción
Sumario:Layered Li(9)V(3)(P(2)O(7))(3)(PO(4))(2) has attracted considerable interest as a novel cathode material for potential use in rechargeable lithium batteries. The defect chemistry, doping behavior and lithium diffusion paths in Li(9)V(3)(P(2)O(7))(3)(PO(4))(2) are investigated using atomistic scale simulations. Here we show that the activation energy for Li migration via the vacancy mechanism is 0.72 eV along the c-axis. Additionally, the most favourable intrinsic defect type is Li Frenkel (0.44 eV/defect) ensuring the formation of Li vacancies that are required for Li diffusion via the vacancy mechanism. The only other intrinsic defect mechanism that is close in energy is the formation of anti-site defect, in which Li and V ions exchange their positions (1.02 eV/defect) and this can play a role at higher temperatures. Considering the solution of tetravalent dopants it is calculated that they require considerable solution energies, however, the solution of GeO(2) will reduce the activation energy of migration to 0.66 eV.