Ionic transport in K2Ti6O13

Author:

Skurikhina Olha12ORCID,Gombotz Maria3ORCID,Senna Mamoru4ORCID,Fabián Martin1ORCID,Baláž Matej1ORCID,Da Silva Klebson Lucenildo5ORCID,Achimovičová Marcela1ORCID,Wilkening H. Martin R.3ORCID,Gadermaier Bernhard3ORCID

Affiliation:

1. Institute of Geotechnics, Slovak Academy of Sciences , Košice , Slovakia

2. Faculty of Materials, Metallurgy and Recycling, Technical University of Košice , Košice , Slovakia

3. Institute of Chemistry and Technology of Materials, Graz University of Technology , Graz , Austria

4. Department of Applied Chemistry , Faculty of Science and Technology, Keio University , Yokohama , Japan

5. Department of Physics , State University of Maringá , Maringá , Brazil

Abstract

Abstract The increasing demand for batteries forced the development of energy storage systems that rely on materials consisting of abundant elements in the Earth’s crust. Switching from Li+ to K+ as the main ionic charge carrier needs highly conducting potassium-bearing electrolytes to realize K+ ion batteries (PIBs). The knowledge gained from the design of Li-ion batteries (LIBs) and Na-ion batteries (NIBs) may conceptually inspire also the establishment of PIBs. Considering, for instance, the hexatitanates Na2Ti6O13, Li2Ti6O13, and H2Ti6O13, which were previously investigated as components for LIBs and NIBs, here we investigated ion dynamics in the K-analog K2Ti6O13. Ionic transport in polycrystalline samples of K2Ti6O13 was studied in a moisture-free atmosphere by broadband impedance spectroscopy in a temperature range from 20 °C to 450 °C. The current study aims at establishing a correlation between structural features of K2Ti6O13 and long-range ionic transport. As expected for K+ transport in K2Ti6O13 with its geometrically obstructed structure, the overall activation energy of ion transport in the ternary oxide takes a rather high value of 0.97(2) eV. Almost the same result (0.95(3) eV) is obtained for the migration activation energy, which we extracted from the analysis of crossover frequencies of the corresponding conductivity isotherms. By comparing our results with those of Na2Ti6O13 (0.82 eV), Li2Ti6O13 (0.65 eV), and H2Ti6O13, we clearly see how the size of the mobile cation correlates with both specific conductivities and activation energies. This comparison points to K+ being the main charge carrier in K2Ti6O13. It also helps in laying the foundations to derive the relevant structure-property relationships in this class of materials.

Publisher

Walter de Gruyter GmbH

Subject

Physical and Theoretical Chemistry

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