The diffusion of Ti in monocrystalline samples was studied at temperatures ranging from 621 to 747K. Ion-beam sputtering and secondary ion mass spectrometry were used to determine concentration depth profiles. It was found that the results could be described by the expressions:
D (m2/s) = 3.7 x 10-5 exp[-1.99(eV)/kT]
These results were consistent with previous high-temperature data. A curvature of the overall Arrhenius plot was attributed to a contribution which arose from divacancies at high temperatures.
A.Almazouzi, M.P.Macht, V.Naundorf, G.Neumann: Physica Status Solidi A, 1998, 167[1], 15-28
Table 94
Interdiffusion in the Sn/Cu System
Temperature (C) | D (m2/s) |
77 | 5.96 x 10-22 |
120 | 4.60 x 10-21 |
150 | 6.63 x 10-21 |
200 | 2.23 x 10-20 |
250 | 5.32 x 10-20 |