Planar confinement, diffusion, and surface segregation results were reported for Si which had been δ-doped into GaAs. In the case of gas-source molecular beam epitaxy, the Si diffusion (table 25) as a function of the reciprocal annealing temperature exhibited an unique 2-component Arrhenius form in which the activation energies differed by the fundamental GaAs band-gap energy of 1.5eV.
J.E.Cunningham, T.H.Chiu, B.Tell, W.Jan: Journal of Vacuum Science and Technology B, 1990, 8[2], 157-9
Table 25
Diffusivity of Si in GaAs
Temperature (C) | D (cm2/s) |
960 | 7.5 x 10-15 |
955 | 4.7 x 10-15 |
895 | 4.4 x 10-15 |
900 | 2.0 x 10-15 |
795 | 2.0 x 10-15 |
790 | 1.1 x 10-15 |
695 | 1.0 x 10-15 |
695 | 5.1 x 10-16 |
645 | 1.9 x 10-16 |
590 | 7.8 x 10-17 |
535 | 4.9 x 10-17 |
605 | 3.7 x 10-17 |
485 | 2.0 x 10-17 |
590 | 1.9 x 10-17 |
555 | 8.2 x 10-18 |
515 | 1.0 x 10-18 |