The diffusivity of Mg in monocrystalline Co1-xO samples was studied, at temperatures ranging from 1000 to 1600C and O partial pressures ranging from 10-8 to 0.21atm, by using microprobe analysis and secondary ion mass spectrometry methods. It was found that the results (table 48) could be described by the expression:
D (cm2/s) = 0.014 exp[-1.95(eV)/kT]
for an O partial pressure of 0.21atm and temperatures of between 1000 and 1600C, and by the expression:
D (cm2/s) = 0.004 exp[-2.07(eV)/kT]
for an O partial pressure of 10-5atm, and temperatures of between 1060 and 1455C. The dependence of the diffusivity upon the O partial pressure was of the form:
log [D (cm2/s)] = 0.0035[log(PO2)]2 + 0.22 log(PO2) - 8.4
at a temperature of 1200C and for pressures of between 10-8 and 0.21atm. It was concluded that the effect of the partial pressure upon Mg impurity diffusion was greater than that upon Co self-diffusion. This was attributed to a preferential attractive interaction between VCo" and Mg.
H.Boussetta, C.Monty: Journal of the Physics and Chemistry of Solids, 1988, 49[4], 369-75
Table 48
Diffusion of Mg in CoO
Temperature (C) | PO2 (atm) | D (cm2/s) |
1005 | 2.1 x 10-1 | 2.7 x 10-10 |
1050 | 2.1 x 10-1 | 4.0 x 10-10 |
1062 | 1 x 10-5 | 9.0 x 10-11 |
1062 | 1.1 x 10-6 | 6.1 x 10-11 |
1098 | 2.1 x 10-1 | 9.6 x 10-10 |
1131 | 2.1 x 10-1 | 1.3 x 10-9 |
1200 | 2.1 x 10-1 | 2.8 x 10-9 |
1200 | 1 x 10-5 | 4.4 x 10-10 |
1200 | 2.65 x 10-3 | 1.1 x 10-9 |
1200 | 5.92 x 10-6 | 4.0 x 10-10 |
1200 | 2.04 x 10-6 | 3.4 x 10-10 |
1200 | 1.05 x 10-8 | 1.7 x 10-10 |
1220 | 2.1 x 10-1 | 3.3 x 10-9 |
1271 | 2.1 x 10-1 | 5.0 x 10-9 |
1340 | 1 x 10-5 | 1.9 x 10-9 |
1340 | 2 x 10-6 | 1.4 x 10-9 |
1347 | 2.1 x 10-1 | 1.0 x 10-8 |
1400 | 2.1 x 10-1 | 1.8 x 10-8 |
1455 | 4.65 x 100 | 2.3 x 10-9 |
1455 | 1 x 10-5 | 5.0 x 10-9 |
1500 | 2.1 x 10-1 | 3.8 x 10-8 |
1600 | 2.1 x 10-1 | 7.4 x 10-8 |