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Extra resources for A r(omega)-Weighted Imbedding Inequalities for A-Harmonic Tensors

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Initially, the dimer is positioned on a regular fcc site. Diffusion then proceeds via concerted motion on an hcp-bridge position towards the neighboring fcc-site. The observed diffusion path is the one predicted by Boisvert and Lewis based on total energy calculations [4]. From the observed jump frequencies we conclude that this process is even active at lower temperature, where it can contribute to mass transport and should not be neglected. Cluster Diffusion and Island Formation 23 0 ps 1 ps 2 ps 3 ps 4 ps 5 ps Figure 2.

For details we refer to [22] and forthcoming publications. Further simplifications may be used here. 1) is very weak for distances rij > 3σ, one can effectively cut-off the interactions and consider only particles in a corresponding neighborhood region when evaluating the PES of a particular event. The so-called frozen crystal approximation should be employed with care: in this scheme all coordinates but those of the moving atom are considered fixed, which significantly simplifies the saddle point search.

Ann. Rev. Mat. Res. 32 (2002), 297–319. [6] T. F. Sekerka, Phase field simulations of faceted growth for strong anisotropy of kinetic coefficient. J. Crystal Growth 254 (2003), 251–261. Epitaxial CVD of Si from Chlorosilanes 39 [7] H. G. Willis, I. F. Jensen, Computational chemistry predictions of reaction processes in organometallic vapor phase epitaxy. Prog. Cryst. Growth Charact. 35 (1997), 117–147. F. T. Rodgers, R. Venkataramani, Multiscale modeling of thin film growth. Current Opinion in Solid State & Materials Science 6 (1998), 562–569.

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