Previous point-defect calculations for this material were used to rationalize O diffusion in undoped, MgO-doped and TiO2-doped samples. The amphoteric nature of the oxide was emphasized by the prediction that O and Al diffusion would be dominated by O vacancies and Al interstitials, or by O interstitials and Al vacancies; depending upon whether
divalent or tetravalent impurities were present in greater abundance. The O diffusion data could be rationalized by using the calculated concentrations of O vacancies and O interstitials. The O vacancies appeared to be 2 to 2.5 times more mobile than O interstitials, whereas Al interstitials appeared to be 103 to 104 times more mobile than O vacancies. On the other hand, the calculations suggested that the migration energies of the O point defects were of the order of 4.5 to 5.9eV. It was not known whether these large values had any physical significance.
Oxygen Self-Diffusion in Corundum: a Conundrum. A.H.Heuer, K.P.D.Lagerlöf: Philosophical Magazine Letters, 1999, 79[8], 619-27
Table 10
Diffusion of O in the Grain Boundaries of Undoped Alumina
Temperature (C) | D (cm3/s) | D (cm2/s) |
1499 | 8.9 x 10-19 | 8.9 x 10-12 |
1540 | 9.7 x 10-18 | 9.7 x 10-11 |
1580 | 1.7 x 10-17 | 1.7 x 10-10 |
1629 | 3.1 x 10-17 | 3.1 x 10-10 |
1660 | 1.8 x 10-16 | 1.8 x 10-9 |
1689 | 6.0 x 10-16 | 6.0 x 10-9 |
1718 | 1.5 x 10-15 | 1.5 x 10-8 |