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Order–disorder transition in nano-rutile TiO 2 anodes: a high capacity low-volume change Li-ion battery material
Nano-sized particles of rutile TiO2 is a promising material for cheap high-capacity anodes for Li-ion batteries. It is well-known that rutile undergoes an irreversible order–disorder transition upon deep discharge. However, in the disordered state, the LixTiO2 material retains a high reversible ion-...
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Published in: | Nanoscale 2019-01, Vol.11 (25) |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | Nano-sized particles of rutile TiO2 is a promising material for cheap high-capacity anodes for Li-ion batteries. It is well-known that rutile undergoes an irreversible order–disorder transition upon deep discharge. However, in the disordered state, the LixTiO2 material retains a high reversible ion-storage capacity of >200 mA h g-1. Despite the promising properties of the material, the structural transition and evolution during the repeated battery operation has so far been studied only by diffraction-based methods, which only provide insight into the part that retains some long-range order. Here, we utilize a combination of ex situ and operando total scattering with pair distribution function analysis and transmission electron microscopy to investigate the atomic-scale structures of the disordered LixTiO2 forming upon the discharge of nano-rutile TiO2 as well as to elucidate the phase behavior in the material during the repeated charge–discharge process. Our investigation reveals that nano-rutile upon Li-intercalation transforms into a composite of ~5 nm domains of a layered LixTiO2 α-NaFeO2-type structure with ~1 nm LixTiO2 grain boundaries with a columbite-like structural motif. During repeated charge–discharge cycling, the structure of this composite is retained and stores Li through a complete solid–solution transition with a remarkably small volume change of only 1 vol% |
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ISSN: | 2040-3364 2040-3372 |
DOI: | 10.1039/c9nr01228a |