Table 2. Calculated Intrinsic Li3 Vacancy Diffusion Barriers for the NN Hops as Shown in Figure 3, Assuming the Vacancy Occupies the Central Ionic Positiona.
| barrier
(eV) |
||||
|---|---|---|---|---|
| class | pathway | d (Å) | forward | reverse |
| xy-plane above | VLi3–1 → VLi1 | 2.91 | 0.51 | 0.45 |
| VLi3–1 → VLi1 | 2.91 | 0.51 | 0.45 | |
| VLi3–1 → VLi2 | 2.92 | 0.47 | 0.41 | |
| xy-plane below | VLi3–1 → VLi1 | 2.91 | 0.51 | 0.45 |
| VLi3–1 → VLi1 | 2.91 | 0.51 | 0.45 | |
| VLi3–1 → VLi2 | 2.92 | 0.47 | 0.41 | |
Distances presented in the table were calculated from the perfect crystal reported by Kataoka et al.14 There were three possible hops each in the xy-planes above and below the xy-plane.