The cation tracer diffusion coefficient of Ga was measured in (Co1-xGax)O as a function of dopant fraction, x, (0 to 0.03), log[O2 activity] (-7 to -0.67) and temperature (1100 to 1350C). For both diffusion coefficients, a non-linear dependence upon dopant fraction and a large effect of the Ga dopant upon the activity-dependence of the diffusion coefficients were found. The experimental observations were modelled in terms of a defect model which involved solute-vacancy pairs in 2 charge states, and triplets which comprised two Ga ions and a cation vacancy. By fitting the experimental data (table 59), a binding energy for neutral pairs, {Ga.V'}x, was found which was small in comparison to the thermal energy, whereas the binding energy for singly-charged pairs, {Ga.V"}', was equal to about 0.5eV. The binding energy for the triplets, {Ga.V"Ga.}x, decreased from 1.1eV at 1100C to 0.76eV at 1350C. The mobility of free vacancies was some 50% larger for V" than for V'.
R.Schmackpfeffer, M.Martin: Philosophical Magazine A, 1993, 68[4], 747-65
Table 58
Diffusion of 59Fe in (Co1-xFex)O
x | Temperature (C) | PO2 (atm) | D (cm2/s) |
0 | 1000 | 2.09 x 10-3 | 4.28 x 10-10 |
0.0055 | 1000 | 2.09 x 10-3 | 1.13 x 10-9 |
0.0090 | 1000 | 2.09 x 10-3 | 1.58 x 10-9 |
0.0148 | 1000 | 2.09 x 10-3 | 2.14 x 10-9 |
0 | 1202 | 2.1 x 10-1 | 9.74 x 10-9 |
0.0055 | 1202 | 2.1 x 10-1 | 1.34 x 10-8 |
0.0090 | 1202 | 2.1 x 10-1 | 1.54 x 10-8 |
0.0148 | 1202 | 2.1 x 10-1 | 1.92 x 10-8 |
0 | 1201 | 2.11 x 10-3 | 2.74 x 10-9 |
0.0055 | 1201 | 2.11 x 10-3 | 5.05 x 10-9 |
0.0090 | 1201 | 2.11 x 10-3 | 6.79 x 10-9 |
continued
x | Temperature (C) | PO2 (atm) | D (cm2/s) |
0.0148 | 1201 | 2.11 x 10-3 | 9.36 x 10-9 |
0 | 1201 | 1.21 x 10-7 | 6.40 x 10-10 |
0.0055 | 1201 | 1.21 x 10-7 | 2.43 x 10-9 |
0.0090 | 1201 | 1.21 x 10-7 | 3.21 x 10-9 |
0.0148 | 1201 | 1.21 x 10-7 | 5.19 x 10-9 |
0 | 1400 | 2.1 x 10-1 | 3.90 x 10-8 |
0.0055 | 1400 | 2.1 x 10-1 | 4.73 x 10-8 |
0.0090 | 1400 | 2.1 x 10-1 | 5.28 x 10-8 |
0.0148 | 1400 | 2.1 x 10-1 | 6.45 x 10-8 |
0 | 1401 | 2.11 x 10-3 | 1.37 x 10-8 |
0.0055 | 1401 | 2.11x 10-3 | 2.15 x 10-8 |
0.0090 | 1401 | 2.11 x 10-3 | 2.55 x 10-8 |
0.0148 | 1401 | 2.11 x 10-3 | 3.38 x 10-8 |
0 | 1402 | 1.42 x 10-6 | 4.33 x 10-9 |
0.0055 | 1402 | 1.42 x 10-6 | 8.98 x 10-9 |
0.0090 | 1402 | 1.42 x 10-6 | 1.16 x 10-8 |
0.0148 | 1402 | 1.42 x 10-6 | 1.69 x 10-8 |