Structural origin of disorder-induced ion conduction in NaFePO4 cathode materials

Abstract

Most modern battery technologies depend on solid-state crystalline cathode materials. However, some of these materials are constrained by the low ionic conductivity of their most stable phases. An example of this is maricite (NaFePO4). Interestingly, experiments have shown that maricite can improve its rate capability through disordering (amorphization). However, experimental characterization of amorphous cathode materials remains a major challenge, hindering a clear understanding of the structural origin of the disorder-induced improvement in sodium-ion mobility. To address this, we here employ molecular dynamics simulations by first training a machine learning potential for NaFePO4 based on the atomic cluster expansion approach and a batch active learning potential parameterization scheme. This potential is then applied to explore the structural and dynamical properties of NaFePO4 glasses as cathode materials. Specifically, we investigate the effect of glass structure on sodium-ion diffusion, revealing the relative influences of short-range and medium-range order features. We find significant heterogeneity in sodium-ion diffusivity in the glass, with fast-conducting ions residing in less constrained atomic environments with fewer P and Fe neighbors. These more mobile ions are also surrounded by larger ring-type structures. Overall, the results and developed approach present promising avenues for developing high-performance glassy cathodes for next-generation batteries.

Graphical abstract: Structural origin of disorder-induced ion conduction in NaFePO4 cathode materials

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Article information

Article type
Paper
Submitted
20 Март. 2025
Accepted
30 Июнь 2025
First published
30 Июнь 2025

J. Mater. Chem. A, 2025, Advance Article

Structural origin of disorder-induced ion conduction in NaFePO4 cathode materials

R. Christensen, K. A. Persson and M. M. Smedskjaer, J. Mater. Chem. A, 2025, Advance Article , DOI: 10.1039/D5TA02295A

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