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