Abstract
The frequency-dependent spectrum of dual-beam-modulated photoconductivity reveals that various processes contribute to steady-state photoconductivity in undoped a-Si: H. These are
1. | electron thermal emission from doubly-occupied dangling bonds | ||||
2. | electron thermal emission from localized states of the conduction-band tail, and | ||||
3. | quenching of photoconductivity which proceeds by reducing the density of electrons trapped on dangling bonds. |
These results are obtained on the basis of a model which in particular allows the coefficient γ characterizing the generation rate dependence of photoconductivity (σpαfy p) to be related to the coefficients γi(i = 1—3) characterizing processes 1—3: γ = a 1γ1 + a 2γ2 — a 3γ3, where a i is a dimensionless parameter describing the relative contribution of process i. The temperature and the photogeneration rate dependences of these processes studied in the annealed and in the light-soaked states are used to identify the nature of the quenching process.