The migration of Be in monocrystalline samples was studied, at temperatures of between 583 and 800K, by using sputter-sectioning and secondary ion mass spectroscopy techniques. It was found that the diffusivity (table 40) obeyed an Arrhenius-type equation. The results could be described in terms of an electrostatic model for impurity diffusion in noble metals, assuming that the Be behaved like a divalent metal. A slight curvature of the Arrhenius plot was attributed to a contribution which was made by divacancies.
A.Almazouzi, M.P.Macht, V.Naundorf, G.Neumann: Physica Status Solidi A, 1992, 133[2], 305-15
Table 38
Diffusivity Parameters for 195Au in Cu
Tilt Angle (º) | Temperature (K) | sδDo (m3/s) | E (kJ/mol) |
33.21 | 661-872 | 2.1 x 10-15 | 72.9 |
35.10 | 661-780 | 3.9 x 10-15 | 73.8 |
35.19 | 661-780 | 4.9 x 10-16 | 60.2 |
35.88 | 661-872 | 9.0 x 10-16 | 63.9 |
36.00 | 661-868 | 1.3 x 10-15 | 67.5 |
36.26 | 661-872 | 6.9 x 10-15 | 80.3 |
36.53 | 661-872 | 1.2 x 10-14 | 87.3 |
36.67 | 661-872 | 7.3 x 10-16 | 61.9 |
37.57 | 661-1030 | 5.0 x 10-17 | 43.2 |
37.74 | 661-780 | 9.6 x 10-17 | 45.3 |
38.12 | 661-872 | 2.5 x 10-16 | 54.3 |
39.26 | 661-780 | 2.0 x 10-15 | 68.5 |