2017
DOI: 10.1063/1.4973824
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Hopping charge transport in amorphous semiconductors with the spatially correlated exponential density of states

Abstract: Hopping charge transport in amorphous semiconductors having spatially correlated exponential density of states has been considered. Average carrier velocity is exactly calculated for the quasi-equilibrium (nondispersive) transport regime. We suggest also a heuristic approach for the consideration of the carrier velocity for the nonequilibrium dispersive regime.

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Cited by 4 publications
(16 citation statements)
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“…In general, the exact origin of trap states at any given depth is not known. It is typical for the sub-bandgap DOS profile to appear exponential over a range of energies [9,11,45] although without any clear physical reason. In the case of conjugated polymers, one important source of site energy distribution is conformational disorder due to variation in intrachain torsion and the resulting variations in the extent of π-conjugation along the polymer backbone.…”
Section: Introductionmentioning
confidence: 99%
“…In general, the exact origin of trap states at any given depth is not known. It is typical for the sub-bandgap DOS profile to appear exponential over a range of energies [9,11,45] although without any clear physical reason. In the case of conjugated polymers, one important source of site energy distribution is conformational disorder due to variation in intrachain torsion and the resulting variations in the extent of π-conjugation along the polymer backbone.…”
Section: Introductionmentioning
confidence: 99%
“…Nontrivial approximate value of ∆D could be calculated by the saddle point method for κ → 1 in close analogy with the calculation of v in Ref. 22 but, unfortunately, this region is unphysical due to the divergence of Z 4 (x, y, z). It is interesting to note that Eq.…”
Section: A General Considerationmentioning
confidence: 95%
“…A suitable method to introduce spatial correlation in the exponentially distributed random energy landscape has been suggested in Ref. 22. There is a well known representation for the exponentially distributed random variable which employs two auxiliary independent identically distributed random Gaussian variables X and Y having zero mean and unit variance σ 2 = 1.…”
Section: Random Energy U (X)mentioning
confidence: 99%
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