The mobilities of individual adatoms, and of various structural elements of the O/Cu system, were analyzed on the basis of scanning tunnelling microscopic data. A value of about x 10-14cm2/s was estimated for the self-diffusivity of Cu on the base (110) surface at 300K. This was deduced from the motion of steps. The supply of Cu adatoms by evaporation from steps, rather than the migration of individual Cu adatoms on the terraces was the rate-limiting process in the so-called added-row reconstruction process.
J.Wintterlin, R.Schuster, D.J.Coulman, G.Ertl, R.J.Behm: Journal of Vacuum Science and Technology B, 1991, 9[2], 902-8
Table 40
Diffusivity of Be in Cu Crystals
Temperature (K) | Annealing Ambient | D (m2/s) |
583 | vacuum | 3.00 x 10-22 |
597 | vacuum | 6.97 x 10-22 |
603 | vacuum | 9.36 x 10-22 |
605 | vacuum | 1.00 x 10-21 |
615 | vacuum | 2.28 x 10-21 |
642 | vacuum | 1.21 x 10-20 |
651 | Ar/H2 | 1.56 x 10-20 |
654 | Ar/H2 | 2.13 x 10-20 |
654 | vacuum | 1.80 x 10-20 |
655 | vacuum | 2.27 x 10-20 |
682 | vacuum | 6.07 x 10-20 |
702 | vacuum | 1.70 x 10-19 |
705 | Ar/H2 | 1.73 x 10-19 |
718 | Ar/H2 | 3.93 x 10-19 |
730 | vacuum | 7.05 x 10-19 |
730 | vacuum | 6.82 x 10-19 |
751 | Ar/H2 | 1.50 x 10-18 |
774 | Ar/H2 | 5.00 x 10-18 |
800 | Ar/H2 | 1.30 x 10-17 |