It was demonstrated that H diffusion in hydrogenated amorphous material was trap-controlled. A 1.4eV barrier was measured for deep D emission to a transport level in D-doped amorphous material. It was shown that light-enhanced diffusion in this material was caused by the light-enhanced de-trapping of H, and not by heating of the sample. Estimates were obtained for the free-H diffusion coefficient (3 x 10-8cm2/s), the mean H displacement between deep trapping events (25nm), and for other parameters that affected the measured H diffusion coefficient in this material.
H.M.Branz, S.E.Asher, B.P.Nelson: Physical Review B, 1993, 47[12], 7061-6
Table 165
Diffusivity of D in Si
Source | T (C) | D (cm2/s) |
plasma | 350 | 3.4 x 10-15 |
plasma | 275 | 8.7 x 10-16 |
plasma | 225 | 3.1 x 10-16 |
plasma | 200 | 1.8 x 10-16 |
plasma | 200 | 1.7 x 10-16 |
plasma | 175 | 9.4 x 10-17 |
plasma | 175 | 8.3 x 10-17 |
plasma | 175 | 7.5 x 10-17 |
layer | 350 | 1.5 x 10-15 |
layer | 300 | 2.2 x 10-16 |
layer | 300 | 2.0 x 10-16 |
layer | 250 | 3.1 x 10-17 |