2002
DOI: 10.1103/physrevlett.88.096803
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Real-Space Measurement of the Potential Distribution Inside Organic Semiconductors

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Cited by 12 publications
(16 citation statements)
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“…2,6,[22][23][24]26,28,29,[34][35][36][37][38]42,43,[53][54][55][56] These molecules have attracted attention in the context of charge transport as materials for molecular electronic device applications. Aromatic molecules, whose conductivity occurs via the π-system, can behave as either electron donors or acceptors, depending on their functionalization.…”
Section: Introductionmentioning
confidence: 99%
“…2,6,[22][23][24]26,28,29,[34][35][36][37][38]42,43,[53][54][55][56] These molecules have attracted attention in the context of charge transport as materials for molecular electronic device applications. Aromatic molecules, whose conductivity occurs via the π-system, can behave as either electron donors or acceptors, depending on their functionalization.…”
Section: Introductionmentioning
confidence: 99%
“…2 virtually inaccessible. 4,8,9 For a device that is connected to external terminals, the condition J = 0 by definition applies at zero bias. However, since the charge density in the vicinity of the contact is much higher than the densities associated with space-charge limited conduction ͑SCLC͒, it is reasonable to take the onset of SCLC, which occurs when flatband is reached in the bulk of the device, as a first-order approximation for the flatband condition ͓Fig.…”
mentioning
confidence: 99%
“…The characteristic plateau and the threshold behavior have been observed for a series of molecular and conjugated-polymer organic materials. [6][7][8][9]26 Alvarado et al 6 have proposed that these thresholds mark the onset of charge-carrier injection into positive (negative) polaronic states, P + ͑P − ͒, at an energy E P + ͑E P − ͒ of the organic material, whereas the width of the plateau corresponds to E g,sp . Moreover, they argue that a necessary condition for the determination of barrier heights for hole and electron injection at organic/metal interfaces is that the electric field at the tip apex be high enough to induce dominant carrier injection from the tip, with a negligible injection of charges of opposite polarity from the counter electrode.…”
Section: Methodsmentioning
confidence: 99%
“…Our results extend and unify earlier interpretations of experimental data that are valid for either a very sharp 6 or a relatively blunt tip. 8 The relevance of these results is emphasized by the fact that many organic semiconductors exhibit a strong tendency to form highly inhomogeneous layers. [10][11][12] As the length scale of these inhomogeneities is typically between a few nanometers and 1 m, [10][11][12] scanning probes are essential tools in the study of organic semiconductor thin films.…”
Section: Introductionmentioning
confidence: 99%
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