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