= 2.33 ± 0.10 eV. Various early works determined the diffusion coefcients and sol-
ubility of carbon in Ni, Fe, and Cu [207–209]. The diffusion barriers can be extracted
via linear interpolation of the diffusion coefcient against inverse absolute tempera-
ture. Majica and Levenson [209] considered the barrier potentials to surface diffusion
in polycrystalline Ni (0.27 eV) using surface-sensitive Auger electron spectroscopy,
whereas Diamond and Wert [210] focused on the bulk diffusion in Ni (1.52 eV). Berry
[211] summarized various work on Ni, spanning multiple techniques, and provided a
good estimate for the bulk dif
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