A thin-layer method was used to study the diffusion, and final-concentration versus distance profiles were measured by using an optical absorption method. The Arrhenius plot exhibited 2 straight segments. The results for low temperatures (table 271) could be described by:
D (cm2/s) = 10.0 exp[-1.00(eV)/kT]
The results for high temperatures could be described by:
D (cm2/s) = 0.026 exp[-0.652(eV)/kT]
The diffusion coefficient for Cu exceeded the self-diffusion coefficient for Na by factors of 1000 to 10000. The data strongly suggested that, above 415C, most of the Cu impurity was interstitial.
N.H.Chan, W.J.Van Scriver: Physical Review B, 1975, 12[8], 3438-48
Table 271
Diffusivity of Cu in NaI Single Crystals
Temperature (C) | D (cm2/s) |
189.5 | 1.320 x 10-10 |
205.0 | 2.686 x 10-10 |
219.0 | 5.375 x 10-10 |
240.2 | 1.542 x 10-9 |
252.5 | 2.646 x 10-9 |
256.8 | 3.085 x 10-9 |
431.2 | 5.460 x 10-7 |
444.4 | 6.720 x 10-7 |
466.0 | 9.060 x 10-7 |
499.3 | 1.420 x 10-6 |
540.4 | 2.330 x 10-6 |
570.6 | 3.200 x 10-6 |