PHYSICAL ORIGINS OF THE OMEGA(1.0)-DEPENDENT AND THE OMEGA(Q)-DEPENDENT (Q-APPROXIMATE-TO-1.3) CONTRIBUTIONS TO THE CONDUCTIVITY RELAXATIONOF GLASSY IONIC CONDUCTORS
Kl. Ngai et al., PHYSICAL ORIGINS OF THE OMEGA(1.0)-DEPENDENT AND THE OMEGA(Q)-DEPENDENT (Q-APPROXIMATE-TO-1.3) CONTRIBUTIONS TO THE CONDUCTIVITY RELAXATIONOF GLASSY IONIC CONDUCTORS, Journal of non-crystalline solids, 222, 1997, pp. 383-390
Contributions with the omega(1.0)-dependence and also the omega(q)-dep
endence (q approximate to 1.3) to the ac conductivity in glassy ionic
conductors are ubiquitous and have properties that differ from the ion
ic diffusion contribution. These different properties suggest that the
omega(1.0)-dependence contribution originates from the vibrational pa
rt of the ion motion which gives rise to a time-independent mean squar
e displacement related to the Debye-Waller factor. The omega(q)-depend
ent contribution to the ac conductivity is related to the omega(q-1)-d
ependent susceptibility on the low frequency side of the Boson peak wh
ich is observed experimentally by neutron scattering and Raman scatter
ing in glasses. With the ionic diffusion contribution already being we
ll-described by the coupling model, this work proposes that the physic
al origins of the various major contributions to the conductivity rela
xation of glassy ionic conductors are now at hand. (C) 1997 Elsevier S
cience B.V.