Sp. Lau et al., CHANGES IN THE POOLE-FRENKEL COEFFICIENT WITH CURRENT-INDUCED DEFECT BAND CONDUCTIVITY OF HYDROGENATED AMORPHOUS-SILICON NITRIDE, Journal of non-crystalline solids, 230, 1998, pp. 533-537
Current induced conductivity in metal-semiconductor-metal thin film di
odes containing hydrogenated amorphous silicon-rich alloys is determin
ed by the concentration of silicon dangling bond states generated by t
he energy released during hole-electron recombination. This mechanism
enables a range of defect concentrations to be introduced and results
in a change in conductivity as carriers move between charged states in
a defect band. Using a-Si-x:H with band gaps in the ranges 2.3 to 2.9
eV, we have measured the field dependence of the conductivity after s
tressing for increasing times and defect densities. By using the relat
ionship between defect concentration and conductivity we have been abl
e to establish that the apparent Poole-Frenkel coefficient (beta(PF))
changes from beta(PF) to 1/2 beta(PF) in a gradual way as the number o
f defects increase in a given material. Furthermore, in the transition
region where beta(PF) changes from the classical to the anomalous val
ue, beta(PF) is linearly dependent on total number of defects. (C) 199
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