Impurity diffusion, and the isotope effect, for Co in -Fe were studied by using a serial radio-frequency sputter-microsectioning method and the radioactive tracers, 57Co and 60Co, at temperatures ranging from 859 to 1173K (table 51). A larger effect of magnetic spin ordering upon Co diffusion, than upon self-diffusion, in -Fe was observed. In ferromagnetic -Fe, the Co diffusion coefficient was equal to about 50% of the self-diffusion coefficient. Above the Curie temperature, the Arrhenius plot for Co diffusion approached the linear Arrhenius line, for self-diffusion, with increasing temperature; as if the latter was the asymptote of the former. The increase in the isotope effect coefficient, due to magnetic spin ordering, for Co diffusion in -Fe was found to be larger than that for self-diffusion. It was suggested that the increase in the migration energy of a Co atom, due to magnetic spin ordering, in -Fe was larger than that in the case of self-diffusion.
Y.Iijima, K.Kimura, C.G.Lee, K.Hirano: Materials Transactions, 1993, 34[1], 20-6
Table 51
Diffusivity of Co in -Fe
Temperature (K) | Diffusivity, D57(m2/s) | (D57/D57)-1 |
1173 | 2.16 x 10-15 | 0.01350 |
1160 | 1.74 x 10-15 | - |
1133 | 7.53 x 10-16 | 0.01173 |
1093 | 2.02 x 10-16 | - |
1075 | 1.12 x 10-16 | 0.01365 |
1053 | 4.46 x 10-17 | 0.01324 |
1043 | 3.31 x 10-17 | 0.01486 |
1030 | 1.33 x 10-17 | - |
1023 | 1.75 x 10-17 | 0.01772 |
1012 | 7.22 x 10-18 | - |
993 | 2.12 x 10-18 | 0.01550 |
973 | 8.94 x 10-19 | 0.01798 |
963 | 5.41 x 10-19 | - |
934 | 1.22 x 10-19 | 0.01679 |
914 | 4.07 x 10-20 | 0.01693 |
873 | 5.10 x 10-21 | 0.01700 |
859 | 2.57 x 10-21 | - |