Despite the large number of first principle studies9-11 performed, mainly aiming to elucidate the diffusion pathways of Li, few efforts have been made to accurately describe the bulk insertion at finite temperatures from first principles. Here we report an exhaustive Li-vacancy configurational density functional theory (DFT) investigation of Li1+xTi5O12 (0 ≥ x ≥ 9) performed with different Li on 16d arrangements. The results indicate that the configurational interactions allow phase segregation between 8a and 16c occupation on a sub nanometer length scale induced by the partial replacement of Li on the 16d sites. This intimate mixing of the 8a and 16c occupancy structurally appears as a solid solution, however it should be considered as a first order phase transition with a sub nanometer domain size, the existence of which is due to the very small energy associated with the coherent interfaces. Based on our predictions of a sub-nano phase separating system we investigate kinetic properties of these phase boundaries by molecular dynamic simulations. We initialized molecular dynamic calculations in supercells that contain two phases (Li4Ti5O12 and Li7Ti5O12) directly in contact with each other. The results clearly display ultra-fast interface kinetics that rationalizes the excellent rate performance of this material. Calculated activation barriers are in good agreement with NMR relaxation measurement. The interface width between the coexisting phases is basically the distance separating the 16c and 8a atomic positions creating mixed 16c/8a occupation condition very similar to a solid solution description. In retrospect, the current work not only explains the apparent phase separation vs.solid solution contradiction in literature, it also explains the excellent rate performance of this intriguing material.
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