The mechanism of near-surface isotope diffusion was investigated by using the edge source method. The activation energy for the localized surface diffusion of 57Co on the (110) NiO surface was 139kJ/mol, as compared with those for grain boundary and volume diffusion (180 and 227kJ/mol, respectively). The surface diffusion of Co2+ ions at 800C appeared to be between 1 and 2 orders of magnitude faster than grain boundary diffusion, and 6 orders or magnitude faster than volume diffusion. The effect of point
defects upon the near-surface diffusion of 57Co was very similar to the effect upon volume diffusion. It was concluded that similar mechanisms were involved in both near-surface and lattice diffusion.
V.S.Stubican: Philosophical Magazine A, 1993, 68[4], 809-18
Table 153
Grain-Boundary Diffusion of 57Co in NiO
Temperature (C) | PO2 (atm) | D (cm2/s) | sDĪ“ (cm3/s) |
500 | 1 | 3.6 x 10-18 | 2.0 x 10-19 |
600 | 1 | 2.4 x 10-16 | 8.7 x 10-18 |
700 | 1 | 6.6 x 10-15 | 1.1 x 10-16 |
700 | 10-11 | 9.5 x 10-16 | 1.2 x 10-18 |
800 | 1 | 9.7 x 10-14 | 4.8 x 10-16 |