NUKLEONIKA 2006, 51(2):93-99
Ludwik Dąbrowski1, Alexander Andreev2, Mladen Georgiev2
1 Nuclear Methods of Solid State Physics Department,
Institute of Atomic Energy, 05-400 Otwock-Świerk, Poland
2 Condensed Matter Department, Institute of Solid State Physics,
Bulgarian Academy of Sciences, 72 Tsarigradsko Chaussee Str., 1784 Sofia, Bulgaria
Recent experimental data on the diffusion coefficient of carbon in a-iron
below liquid nitrogen temperature (LNT) question the classical approach to the observed temperature
dependence. As the temperature is lowered below LNT, the diffusion constant tends to a nearly
temperature-independent value rather than continuing its activated trend. The low temperature branch
is apparently characteristic of a quantum mechanical process dominated by tunneling in ground state.
Concomitantly we apply an occurrence-probability approach to describing the overall temperature
dependence as a single continuous rate. Within the adiabatic approximation the electronic eigenvalue
depending parametrically on the nuclear coordinates is taken to be the potential energy to control the
motion of the nuclei. The resulting rate involves all horizontal-tunneling energy-conserving elastic
transitions at the quantized energy levels of the migrating atom. A small though not negligible slope
in the temperature dependence as the temperature is raised below 100 K is dealt with by complementing
for the rate of a parallel one-phonon inelastic-tunneling process in excess to the basic elastic-tunneling
rate. Our combined approach agrees well with the experimental data. In particular, the frequency of
the coupled vibration is obtained virtually identical to the carbon vibrational frequency from
inelastic neutron scattering data. The migrational barrier is also found to be within the limits
expected for a-iron.