The 66th JSAP Spring Meeting, 2019

Presentation information

Poster presentation

1 Interdisciplinary Physics and Related Areas of Science and Technology » 1.4 Energy conversion, storage, resources and environment

[11p-PA3-1~10] 1.4 Energy conversion, storage, resources and environment

Mon. Mar 11, 2019 1:30 PM - 3:30 PM PA3 (PA)

1:30 PM - 3:30 PM

[11p-PA3-4] Lithium, Sodium and Magnesium Insertion in Brookite TiO2: a Comparative Computational Study

Daniel Koch1, 〇Sergei Manzhos1 (1.Ntl Uni of Singapore)

Keywords:titanium dioxide, metal ion battery, ab initio modeling

Phases of titania have been actively explored as active electrode materials for Li, Na, and Mg ion batteries. Rationalization of performance and rational selection of optimal titania phases for a specific type of battery is assisted by ab initio simulations. Previously, we compared Li, Na, and Mg interaction with anatase, rutile, B and amorphous TiO2 [1]. Here, we provide ab initio modeling results on the energetics and mechanism of Li, Na, and Mg interactions with the brookite phase. Recently the brookite phase has been gaining attention; specifically, structural similarity of this phase and amorphous titanium dioxide was reported [2]. Given that amorphization has been shown to enhance voltages [1], which can potentially make titania interesting as a cathode, a comparative study including brookite is useful. The computed low-concentration insertion energies and the corresponding voltages, however, suggest poor electrochemical performance of brookite in comparison to e.g. ‘layered’ titania phases such as B-TiO2. We argue that this behavior could be explained by local electronic structure leading to higher voltages in amorphous compounds, since the lattice strains induced by intercalation in brookite are not sufficient to explain the poor binding energies with the inserted Li, Na, and Mg. We also observe that, similarly to the previously reported magnetic ordering in e.g. potassium- or sodium-inserted V2O5, each electron donated by the intercalant is delocalized over a nearly linear Ti-O-Ti fragment close to the insertion site, mediated by antiferromagnetic interaction of the two d-type states with an oxygen p-state in between.
[1] F. Legrain, O. I. Malyi, S. Manzhos, J. Power Sources, 278, 197 (2015).
[2] J. Mavracic et al., J. Phys. Chem. Lett. 9, 2985 (2018).