Experimental data, which revealed the essential features of atomic H that had been incorporated from various sources at low temperatures, were presented. Appropriate conditions for hydrogenation were chosen, and the H diffusivity (table 49) was found to be described by:
D(cm2/s) = 2 x 10-5exp[-0.49(eV)/kT]
The Peculiarities of Deep Level Defect Passivation in Si by Atomic Hydrogen. S.V.Koveshnikov, S.V.Nosenko, E.B.Yakimov: Physica Status Solidi A, 1990, 120[2], 391-5
Table 50
Diffusivity of D and H in Si
Diffusant | Temperature (K) | D (cm2/s) |
D | 270 | 3.7 x 10-12 |
D | 265 | 2.2 x 10-12 |
D | 260 | 1.6 x 10-12 |
D | 255 | 1.2 x 10-12 |
D | 250 | 6.6 x 10-13 |
D | 245 | 4.7 x 10-13 |
D | 240 | 1.9 x 10-13 |
D | 235 | 1.8 x 10-13 |
D | 230 | 8.2 x 10-14 |
D | 225 | 5.4 x 10-14 |
H | 270 | 7.6 x 10-12 |
H | 265 | 5.7 x 10-12 |
H | 260 | 2.7 x 10-12 |
H | 255 | 1.9 x 10-12 |
H | 245 | 6.0 x 10-13 |
H | 240 | 3.7 x 10-13 |
H | 235 | 2.8 x 10-13 |
H | 230 | 1.2 x 10-13 |
H | 220 | 4.0 x 10-14 |