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Emission-limited charge-carrier injection in the dark from a metal into a random organic dielectric has been studied via Monte Carlo simulations. The dielectric has been modelled in terms of a regular lattice of point sites featuring a Gaussian distribution of energies to represent disorder. The essential input parameters are the zero-field energy barrier for injection (), the variance () of the distribution of the hopping states, electric field, and temperature. By varying the jump distance the unimportance of long-range tunneling transitions has been established. Therefore, Fowler-Nordheim type j (F) charcteristics at high fields have to be considered accidental. The dependence of the injection yield resembles that of Richardson-Schottky (RS) thermionic emission. Quantitative differences are noted, however, concerning the RS coefficient and the temperature dependence. The latter tends to saturate at low temperatures, which is a signature of hopping among sites distributed in energy.
Wolf et al. (Mon,) studied this question.
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