In our studies of coating properties and their relation to overpotential, we use ab initio density functional theory to show that the above phases, when crystalline, are very poor Li conductors except for specific directions in SiO2. We also propose an Ohmic continuum model for understanding the connection between the coating overpotential and Li solubility, diffusivity, coating thickness, and current density. We use this model and previous studies of Li in amorphous Al2O3 and AlF3 2 to predict that that Atomic Layer Deposited (ALD) Al2O3 coatings have a resistivity of 1789 MOhmm (106Ohmm), which value is qualitatively consistent with that extracted from multiple ALD experiments (ranges from 7.8 MOhmm to 913 MOhmm). The results of our Ohmic continuum model are summarized in the attached figure, which shows our predicted coating overpotential in terms of fundamental coating properties of Li solubility and diffusivity for key systems (amorphous Al2O3 and AlF3 and lithiated Li3.5Al2O3) under the condition of coating thickness L=1nm, current density Jactive = 0.046 mA/cm2(approximately a 1C rate) at room temperature.
In order to model the effects of interfaces on the Li energetics we explore the Li intercalation energy profile across an interface of two materials with very different bulk intercalation energies. The olivine-structured FePO4-MPO4 (M=Co, Ti, Mn) and layered-structured LiNiO2-TiO2interfaces provide model cases to understand the physics governing Li intercalation energetics across material interfaces. We find that across the interface from a high to low voltage material (i.e. low to high Li intercalation energy), the Li site energy remains constant in the high voltage material and decays approximately linearly in the low voltage region, approaching the Li site energy of the low voltage material. This effect indicates that the existence of a high intercalation voltage material at an interface can significantly enhance the Li intercalation voltage in a low voltage region over a 1-2 nm scale. We explore possible implications of this interfacial voltage enhancement for the design of novel cathode superlattice structures.
Figure Caption:
Fig. 1 Solubility and diffusivity dependence of potential drop across a room temperature thin coating film of L = 1 nm for a current of density Jactive = 0.046 mA/cm2(approximately a 1C rate) through the active coating surface.
References
1 Xu, S. et al. Lithium transport through lithium-ion battery cathode coatings. Journal of Materials Chemistry A 3, 17248-17272 (2015).
2 Hao, S. Q. & Wolverton, C. Lithium Transport in Amorphous Al2O3 and AlF3 for Discovery of Battery Coatings. J. Phys. Chem. C 117, 8009-8013, (2013).