Abstract
The excess a.c. conductivity [sgrave]A(ω) = [sgrave](ω) - [sgrave](0) due to hopping processes in a disordered material is usually interpreted in terms of the ω5 law, s< 1, predicted by the pair approximation. However, recent data on [sgrave]A(ω) for amorphous germanium shows a roll-off behaviour as ω → 0; [sgrave]A(ω) falls off faster than ω5 below a characteristic frequency ωc which exhibits a strong temperature dependence. In the present work it has been found that the roll-off is obtained within the extended pair approximation (EPA)—it marks the onset of a.c. loss by subsets of sites contained in the infinite cluster determining [sgrave](0). Decreasing ω through ωc changes s from less than unity to 2. To within a scale factor, the EPA gives a good account of the observed frequency dependence of [sgrave]A(ω) and the temperature dependence of ωc.