Abstract

Abstract In the theoretical analysis of transient photoconductivity data on amorphous semiconductors in terms of multiple trapping, a number of recent publications use the concept of a time-dependent demarcation energy E d(t) such that, at time t, the excess charge carriers occupying localized states between the mobility edge and this energy are in quasi-thermal equilibrium with the free carriers in extended states, while those occupying states with energies beyond E d(t) have had no time to leave such states. Results are reported of calculations of the occupancy of the localized states for a current transient of the form Ct –(1–α) that is often observed. The results show that such a simplistic interpretation of E d(t) involves appreciable numerical errors, so that the concept of a demarcation energy is only useful for the qualitative, rather than the quantitative, analysis of experimental results.

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