The diffusion of Sn in intrinsic Ge was studied, at temperatures ranging from 555 to 930C, by means of secondary ion mass spectrometry. The Sn was in-diffused, under vacuum conditions, from both the gas phase and from thin films. In both cases, the pure metal was used as a source of Sn. Within the above temperature range, the diffusivity of Sn as a function of temperature (table 3) could be expressed by:
D(cm2/s) = 840 exp[-3.26(eV)/kT]
On the basis of similarities between Sn diffusion and Ge self-diffusion, it was concluded that Sn in Ge diffused via a mono-vacancy mechanism.
M.Friesel, U.Södervall, W.Gust: Journal of Applied Physics, 1995, 78[9], 5351-5
Table 3
Diffusivity of Tin in Germanium
T (C) |
Method |
D (cm2/s)
|
930 |
gas phase |
2.22 x 10-11 |
900 | gas phase | 8.92 x 10-12 |
875 | gas phase | 3.73 x 10-12 |
850 | gas phase | 1.89 x 10-12 |
825 | gas phase | 8.32 x 10-13 |
800 | gas phase | 4.28 x 10-13 |
775 | gas phase | 1.71 x 10-13 |
750 | gas phase | 6.92 x 10-14 |
725 | gas phase | 1.95 x 10-14 |
700 | gas phase | 1.33 x 10-14 |
650 | gas phase | 1.57 x 10-15 |
615 | gas phase | 2.72 x 10-16 |
555 | gas phase | 1.19 x 10-17 |
900 | thin film | 7.84 x 10-12 |
750 | thin film | 6.57 x 10-14 |
700 | thin film | 1.12 x 10-14
|