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Charge storage in oxygen deficient phases of TiO(2): defect Physics without defects

Defects in semiconductors can exhibit multiple charge states, which can be used for charge storage applications. Here we consider such charge storage in a series of oxygen deficient phases of TiO(2), known as Magnéli phases. These Magnéli phases (Ti(n)O(2n−1)) present well-defined crystalline struct...

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Detalles Bibliográficos
Autores principales: Padilha, A. C. M., Raebiger, H., Rocha, A. R., Dalpian, G. M.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4929474/
https://www.ncbi.nlm.nih.gov/pubmed/27364139
http://dx.doi.org/10.1038/srep28871
Descripción
Sumario:Defects in semiconductors can exhibit multiple charge states, which can be used for charge storage applications. Here we consider such charge storage in a series of oxygen deficient phases of TiO(2), known as Magnéli phases. These Magnéli phases (Ti(n)O(2n−1)) present well-defined crystalline structures, i.e., their deviation from stoichiometry is accommodated by changes in space group as opposed to point defects. We show that these phases exhibit intermediate bands with an electronic quadruple donor transitions akin to interstitial Ti defect levels in rutile TiO(2). Thus, the Magnéli phases behave as if they contained a very large pseudo-defect density: ½ per formula unit Ti(n)O(2n−1). Depending on the Fermi Energy the whole material will become charged. These crystals are natural charge storage materials with a storage capacity that rivals the best known supercapacitors.