The pressure dependence of diffusion in the high-temperature body-centered cubic phase of Zr was studied by using radio-tracer techniques. The activation volumes for 95Nb diffusion were equal to 0.161 Ω at 1423K and 0.193 Ω at 1273K. The small activation volumes indicated a large relaxation of the vacancy. This in turn reflected the inherent weakness, of the body-centered cubic lattice, with regard to shear in the <111> direction. These results (table 279) provided an explanation for the absence of positron trapping in group-IV transition metals.
P.Knorr, J.Jun, W.Lojkowski, C.Herzig: Physical Review B, 1998, 57[1], 334-40
Table 278
Diffusion of Hf in Polycrystalline Ultra-Pure or Fe-Doped -Zr
Sample | Temperature (K) | D (m2/s) |
ultra-pure | 1111.0 | 1.1 x 10-19 |
Fe-doped | 1110.9 | 1.1 x 10-17 |
ultra-pure | 1052.6 | 7.6 x 10-20 |
ultra-pure | 1000.0 | 8.2 x 10-21 |
ultra-pure | 934.2 | 5.3 x 10-22 |
Fe-doped | 933.4 | 1.1 x 10-18 |
ultra-pure | 873.0 | 2.5 x 10-23 |