Fast lithium-ion conductivity in the 'empty-perovskite' n = 2 Ruddlesden–Popper-type oxysulphide Y2Ti2S2O5. Issue 11 (23rd February 2021)

• Record Type: Journal Article
• Authors: McColl, Kit; Corà, Furio
• Is Part Of: Journal of materials chemistry. Volume 9:Issue 11(2021)
• Page Start: 7068
• Page End: 7084
• Publication Date: 2021-02-23
• Subjects: Materials -- Research -- Periodicals; Chemistry, Analytic -- Periodicals; Environmental sciences -- Research -- Periodicals; 543.0284
• DOI: 10.1039/d0ta11358a
• Languages: English
• ISSNs: 2050-7488

Abstract

Abstract : Lithium ions reside on a square network of sites in empty ReO3 -like units within the Li-ion anode material Y2 Ti2 S2 O5 and move with activation barriers of only 64 meV under dilute conditions, providing fast 2D mobility. Abstract : Materials with Wadsley–Roth (W–R) crystallographic shear and bronze-type structures display fast lithium (Li)-ion diffusion and are of interest as anode materials for high-power Li-ion batteries. Here we use density-functional-theory calculations to investigate Y2 Ti2 S2 O5, a Li-ion anode material that shares structural features with W–R phases. Y2 Ti2 S2 O5 is a layered Ruddlesden–Popper-type oxysulphide displaying a reversible capacity of 128 mA h g −1, with 60% capacity-retention at a charge rate of 20C in micrometer-sized electrode particles. The crystal structure contains an empty central layer of corner-sharing [TiO5 S] octahedra, equivalent to a (∞ × ∞ × 2) block of the ReO3 -like units that form Wadsley–Roth type phases. Intercalated Li + ions on this plane occupy distorted 'rectangular-planar' sites, and display 2D mobility with single-ion hopping barriers of 64 meV under dilute conditions. The insertion geometry of Li + is highly frustrated, giving rise to a smooth potential energy surface for Li-hopping and exceptionally low activation barriers. The [TiO5 S] units do not experience major distortions or correlated rotations during discharge, due to framework rigidity provided by [Y2 S2 ] 2+ rocksalt slabs, meaning the rectangular-planar-like geometry of Li + is retained across all states of charge. A tetragonal to orthorhombic to tetragonal phase change occurs upon lithiation, with a stable Li + ordering at x = 1.0 in Li x Y2 Ti2 S2 O5 . Li + –Li + repulsion has a significant effect on the cation ordering at all Li intercalation levels. Na + hopping barriers are >1.7 eV, while Mg 2+ ions can move with barriers of ∼607 meV, illustrating the how diffusion behaviour varies for ions of different size and charge within W–R-type frameworks. The exceptionally low activation barriers for Li-hopping and well-defined, rigid 2D diffusion plane makes Y2 Ti2 S2 O5 a valuable model system within which to understand Li + behaviour in high-rate electrode materials, such as the related Wadsley–Roth phases.