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Electric‐Field‐Controlled Dopant Distribution in Organic Semiconductors
Author(s) -
Müller Lars,
Rhim SeonYoung,
Sivanesan Vipilan,
Wang Dongxiang,
Hietzschold Sebastian,
Reiser Patrick,
Mankel Eric,
Beck Sebastian,
Barlow Stephen,
Marder Seth R.,
Pucci Annemarie,
Kowalsky Wolfgang,
Lovrincic Robert
Publication year - 2017
Publication title -
advanced materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 10.707
H-Index - 527
eISSN - 1521-4095
pISSN - 0935-9648
DOI - 10.1002/adma.201701466
Subject(s) - dopant , materials science , doping , thin film , kelvin probe force microscope , semiconductor , electric field , organic semiconductor , optoelectronics , nanotechnology , diffusion , analytical chemistry (journal) , chemical physics , organic chemistry , atomic force microscopy , chemistry , physics , quantum mechanics , thermodynamics
Stable electrical doping of organic semiconductors is fundamental for the functionality of high performance devices. It is known that dopants can be subjected to strong diffusion in certain organic semiconductors. This work studies the impact of operating conditions on thin films of the polymer poly(3‐hexylthiophene) (P3HT) and the small molecule Spiro‐MeOTAD, doped with two differently sized p‐type dopants. The negatively charged dopants can drift upon application of an electric field in thin films of doped P3HT over surprisingly large distances. This drift is not observed in the small molecule Spiro‐MeOTAD. Upon the dopants’ directional movement in P3HT, a dedoped region forms at the negatively biased electrode, increasing the overall resistance of the thin film. In addition to electrical measurements, optical microscopy, spatially resolved infrared spectroscopy, and scanning Kelvin probe microscopy are used to investigate the drift of dopants. Dopant mobilities of 10 −9 to 10 −8 cm 2 V −1 s −1 are estimated. This drift over several micrometers is reversible and can be controlled. Furthermore, this study presents a novel memory device to illustrate the applicability of this effect. The results emphasize the importance of dynamic processes under operating conditions that must be considered even for single doped layers.