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Na2RuO3: A Model to Study the Extra Capacity of a2mO3 Type Cathodes

Monday, 20 June 2016
Riverside Center (Hyatt Regency)
B. Mortemard de Boisse, G. Liu, J. Ma, S. Nishimura, S. C. Chung (Department of Chem. System Eng., The University of Tokyo), H. Kiuchi (Department of Appl. Chem., The University of Tokyo), Y. Harada (ISSP, The University of Tokyo), J. Kikkawa (National Institute for Materials Science), K. Yoshio (The University of Electro-Communications, Tokyo), M. Okubo, and A. Yamada (Department of Chem. System Eng., The University of Tokyo)
Li-ion batteries power almost all of today’s portable electronics as well as electric and hybrid vehicles thanks to their important energy density. However their high cost tend to prevent larger-scale application such as in power grids. On the other hand, Na is abundant, easily accessible and therefore cheaper than Li. As a consequence, Na-ion batteries draw a lot of attention since the 2000s.

Even though NaxMO2 (x ≤ 1, M = transition metal) materials have been studied for a long time as positive electrode candidates, the available capacity is still limited. Partial substitution of M by Na+ is an appealing strategy to overcome this issue: the excess Na+ ions in the MO2 layer could participate in the (de)intercalation process while lowering the weight of the battery, thus greatly enhancing the gravimetric capacity. This strategy, applied to Li-ion batteries for many years, is still poorly transferred to Na-ion battery materials.

In order to establish a model for the study of Na2MO3 – and A2MO3 in general –, we prepared two polymorphs of O3-Na2RuO3 distinguished by the honeycomb-like ordering of the [Ru2/3Na1/3]O2 layers [1,2]. In both samples, we found that Na in the interlayer and in the [Ru2/3Na1/3]O2 layers is accessible. In ordered-Na2RuO3, the honeycomb ordering triggers the spontaneous formation of an ilmenite-type intermediate which facilitates highly reversible oxygen redox chemistry, associated to a large extra capacity (Figure 1) as well as noticeable structural stability upon cycling making it, to our knowledge, the first AxMO3 to do so.

Figure 1. Galvanostatic cycling curves for (a) disordered and (b) ordered O3-Na2RuO3 (first cycle highlighted in blue). The insets represent the coordination environment of Na at x = 1.