It was recalled that the weak concentration dependence of Ni diffusion in this material had been interpreted as being evidence for Ni diffusion via next-nearest neighbour jumps. This seemed to be reasonable, in view of the comparatively high enthalpy of formation in this alloy. Quasi-elastic neutron scattering and back-scattering spectrometry were used to study the elementary diffusion jumps of Ni in NiGa single crystals which contained 50at%Ni, and in polycrystals which contained 57 or 62at%Ni. The weak concentration-dependence of the Ni diffusion coefficient was confirmed over a wide concentration range on the Ni-rich site of the phase diagram (table 26, figure 20). The diffusive jumps of Ni atoms were proved to involve jumps via nearest-neighbour (antistructure) sites. In the case of the near-stoichiometric compositions, it was possible to determine directly the residence times of Ni atoms, at antistructure sites, from quasi-elastic neutron scattering data. The results were concluded to indicate the existence of very high defect concentrations near to the melting point.
Nickel Diffusion in B2-NiGa Studied with Quasielastic Neutron Scattering. M.Kaisermayr, J.Combet, H.Ipser, H.Schicketanz, B.Sepiol, G.Vogl: Physical Review B, 2000, 61[18], 12038-44
Figure 20
Diffusion of Ni in NiGa
Table 26
Diffusivity of Ni in NiGa
Ni (at%) | Sample | Temperature (C) | D (m2/s) |
51.2 | monocrystalline | 990 | 1.12 x 10-12 |
51.2 | monocrystalline | 1060 | 2.31 x 10-12 |
51.2 | monocrystalline | 1130 | 5.12 x 10-12 |
52.5 | monocrystalline | 1060 | 2.32 x 10-12 |
57.2 | polycrystalline | 1130 | 5.44 x 10-12 |
61.9 | polycrystalline | 1040 | 3.14 x 10-12 |
61.9 | polycrystalline | 1150 | 7.42 x 10-12 |