The incorporation of H was studied under various electrochemical conditions, including anodization in fluoride solutions (where porous Si formed). The results suggested that there was a large near-surface H concentration, while simulations showed that the maximum penetration depth was governed by the volume diffusion of H and by material removal. The diffusion coefficients were found to depend upon the electrochemical conditions, and ranged from 10-13 to 10-11cm2/s.
P.Allongue, C.H.De Villeneuve, L.Pinsard, M.C.Bernard: Applied Physics Letters, 1995, 67[7], 941-3
Table 163
Diffusivity of H in Doped Amorphous Si
B | P | T (C) | D (cm2/s) |
0.01 | - | 272 | 9.7 x 10-14 |
0.01 | - | 201 | 1.7 x 10-15 |
0.001 | - | 301 | 1.4 x 10-13 |
0.001 | - | 255 | 1.2 x 10-14 |
0.001 | - | 156 | 3.0 x 10-17 |
0.0001 | - | 273 | 1.4 x 10-14 |
0.0001 | - | 199 | 1.5 x 10-16 |
0.001 | 0.0001 | 272 | 2.5 x 10-15 |
0.001 | 0.0001 | 200 | 3.2 x 10-17 |
- | 0.001 | 300 | 2.8 x 10-15 |
- | 0.001 | 201 | 2.0 x 10-17 |
- | 0.0001 | 272 | 6.1 x 10-16 |
- | 0.0001 | 199 | 6.6 x 10-18 |
- | 0.00001 | 272 | 2.0 x 10-16 |
- | 0.00001 | 240 | 3.7 x 10-17 |