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