Self-diffusion and impurity diffusion of fee metals using the five-frequency model and the Embedded Atom Method
10.1557/jmr.1989.0102
Crossref journal-article
Springer Science and Business Media LLC
Journal of Materials Research (297)
Abstract

The activation energies for self-diffusion of transition metals (Au, Ag, Cu, Ni, Pd, Pt) have been calculated with the Embedded Atom Method (EAM); the results agree well with available experimental data for both mono-vacancy and di-vacancy mechanisms. The EAM was also used to calculate activation energies for vacancy migration near dilute impurities. These energies determine the atomic jump frequencies of the classic “five-frequency formula,” which yields the diffusion rates of impurities by a mono-vacancy mechanism. These calculations were found to agree fairly well with experiment and with Neumann and Hirschwald's “Tm” model.

Bibliography

Adams, J. B., Foiles, S. M., & Wolfer, W. G. (1989). Self-diffusion and impurity diffusion of fee metals using the five-frequency model and the Embedded Atom Method. Journal of Materials Research, 4(1), 102–112.

Authors 3
  1. J. B. Adams (first)
  2. S. M. Foiles (additional)
  3. W. G. Wolfer (additional)
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Dates
Type When
Created 17 years, 10 months ago (Sept. 27, 2007, 5:39 a.m.)
Deposited 4 years, 6 months ago (Feb. 24, 2021, 4:42 p.m.)
Indexed 1 month ago (July 20, 2025, 6:46 p.m.)
Issued 36 years, 6 months ago (Feb. 1, 1989)
Published 36 years, 6 months ago (Feb. 1, 1989)
Published Online 14 years, 6 months ago (Jan. 31, 2011)
Published Print 36 years, 6 months ago (Feb. 1, 1989)
Funders 0

None

@article{Adams_1989, title={Self-diffusion and impurity diffusion of fee metals using the five-frequency model and the Embedded Atom Method}, volume={4}, ISSN={2044-5326}, url={http://dx.doi.org/10.1557/jmr.1989.0102}, DOI={10.1557/jmr.1989.0102}, number={1}, journal={Journal of Materials Research}, publisher={Springer Science and Business Media LLC}, author={Adams, J. B. and Foiles, S. M. and Wolfer, W. G.}, year={1989}, month=feb, pages={102–112} }