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

-