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Charge Transfer and Percolation in C 60 /Pentacene Field‐Effect Transistors
Author(s) -
Kyndiah Adrica,
Cramer Tobias,
Albonetti Cristiano,
Liscio Fabiola,
Chiodini Stefano,
Murgia Mauro,
Biscarini Fabio
Publication year - 2015
Publication title -
advanced electronic materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.25
H-Index - 56
ISSN - 2199-160X
DOI - 10.1002/aelm.201400036
Subject(s) - pentacene , materials science , ambipolar diffusion , optoelectronics , heterojunction , organic field effect transistor , organic semiconductor , organic electronics , transistor , field effect transistor , chemical physics , nanotechnology , layer (electronics) , electron , thin film transistor , chemistry , physics , voltage , quantum mechanics
Charge transfer at organic‐organic heterojunctions is fundamental to several organic electronics devices, including light‐emitting diodes, photovoltaic cells, light‐emitting transistors, and ambipolar field‐effect transistors. Here, probe charge transfer (CT) processes during the formation of an organic‐organic heterojunction are probed by performing in situ real‐time electrical characterization during the growth of pentacene/C 60 ambipolar transistors. N‐type C 60 channel formation follows two different percolation pathways, one being associated to linear C 60 structures growing along pentacene grain boundaries and the other to C 60 island percolation. Upon n‐channel formation a shift of pentacene p‐type transfer characteristics is observed, which is attributed to CT across the heterojunction interface as a result of Fermi level alignment. The findings allow estimation of the energy of thermally accessible CT‐states and their mobility along the interface. Finally, a model is proposed that relates the amount of transferred charge to details in the bilayer morphology and layer thicknesses. The model relies on the capacitive coupling between C 60 and pentacene in the accumulation layer, which is consistent with a single hole transport channel.