The nucleation of dislocations, and their subsequent propagation during thin-film deposition, were studied by using 3-dimensional molecular dynamics methods. The case of W on a substrate of the same material was investigated. The substrate was under uniaxial compression along the [111] direction, with the thermodynamically favored (0¯11) surface horizontal. The simulation results indicated that nucleation began at a surface step where an atom was squeezed into the layer above; thus generating a half-dislocation loop at the surface. It could then either propagate into the film or become the base of a sessile dislocation loop. In the former case, the dislocation loop (with a Burgers vector of ½[1¯1¯1] on a (101) glide plane) propagated along the [1¯1¯1] direction at the surface and extended to about 2 atomic layers along the [111] direction. In the other case, the missing layer propagated along the [100] direction at the surface; extending to about 4
atomic layers along the [111] direction. In this case, the sessile dislocation had a Burgers vector of ½ [¯1¯1¯1] on the (011) plane.
Dislocation Nucleation and Propagation during Thin Film Deposition under Compression. W.C.Liu, S.Q.Shi, H.Huang, C.H.Woo: Computational Materials Science, 2002, 23[1-4], 155-65
Table 10
Diffusivity of Fe in Zr46.8Be27.5Ti8.2Cu7.5Ni10
Temperature (K) | Diffusivity (m2/s) |
513 | 2.14 x 10-24 |
534 | 2.60 x 10-23 |
554 | 1.15 x 10-22 |
574 | 6.13 x 10-22 |
593 | 3.88 x 10-21 |
613 | 2.92 x 10-20 |
630 | 1.51 x 10-19 |
643 | 4.22 x 10-19 |
658 | 1.66 x 10-18 |
672 | 5.98 x 10-18 |