z-logo
Premium
Monitoring the Channel Formation in Organic Field‐Effect Transistors via Photoinduced Charge Transfer
Author(s) -
Singh Thokchom Birendra,
Koeppe Robert,
Sariciftci Niyazi Serdar,
Morana Mauro,
Brabec Christoph J.
Publication year - 2009
Publication title -
advanced functional materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 6.069
H-Index - 322
eISSN - 1616-3028
pISSN - 1616-301X
DOI - 10.1002/adfm.200801438
Subject(s) - materials science , organic field effect transistor , dielectric , optoelectronics , semiconductor , organic semiconductor , gate dielectric , transistor , field effect transistor , benzocyclobutene , charge carrier , phthalocyanine , monolayer , nanotechnology , electrical engineering , voltage , engineering
Conducting channel formation in organic field‐effect transistors (OFETs) is considered to happen in the organic semiconductor layer very close to the interface with the gate dielectric. In the gradual channel approximation, the local density of accumulated charge carriers varies as a result of applied gate bias, with the majority of the charge carriers being localized in the first few semiconductor monolayers close to the dielectric interface. In this report, a new concept is employed which enables the accumulation of charge carriers in the channel by photoinduced charge transfer. An OFET employing C 60 as a semiconductor and divinyltetramethyldisiloxane‐bis(benzocyclobutene) as the gate dielectric is modified by a very thin noncontinuous layer of zinc‐phthalocyanine (ZnPc) at the semiconductor/dielectric interface. With this device geometry, it is possible to excite the phthalocyanine selectively and photogenerate charges directly at the semiconductor/dielectric interface via photoinduced electron transfer from ZnPc onto C 60 . Thus the formation of a gate induced and a photoinduced channel in the same device can be correlated.

This content is not available in your region!

Continue researching here.

Having issues? You can contact us here