Isotopically controlled heterostructures were used to study Ga self-diffusion by using secondary-ion mass spectrometry. This approach produced a near-ideal random walk situation that was free of perturbations arising from electric fields, mechanical stresses, or chemical potentials. It was found that the Ga self-diffusion coefficient in intrinsic material (table 16) could be described by:
D(cm2/s) = 43 exp[-4.24(eV)/kT]
over 6 orders of magnitude, at temperatures of between 800 and 1225C, under As-rich conditions. No significant doping effects were observed in samples with substrates that were doped with Te up to 4 x 1017/cm3 or with Zn up to 1019/cm3.
L.Wang, L.Hsu, E.E.Haller, J.W.Erickson, A.Fischer, K.Eberl, M.Cardona: Physical Review Letters, 1996, 76[13], 2342-5
Table 16
Diffusivity of Ga in GaAs
Temperature (C) | D (cm2/s) |
1230 | 3.3 x 10-13 |
1125 | 2.4 x 10-14 |
1095 | 1.1 x 10-14 |
1075 | 6.5 x 10-15 |
1025 | 2.0 x 10-15 |
975 | 2.6 x 10-16 |
950 | 2.4 x 10-16 |
925 | 3.8 x 10-17 |
900 | 2.8 x 10-17 |
845 | 5.3 x 10-18 |
795 | 6.9 x 10-19 |