Advanced Functional Materials · 2009 · 33 citations · 37 references
EngineeringElectrical EngineeringMaterials ScienceElectronic MaterialsSemiconductor DevicesSemiconductor MaterialsCarrier TransportCharge Carrier TransportField-effect TransistorsOrganic SemiconductorsSemiconductor InterfacesSemiconductor PhysicsCarrier Transport In Organic SemiconductorsCharge Transport MechanismsDielectric-semiconductor InterfacesElectron TransferOrganic DielectricsOrganic ElectronicsOrganic Field-effect TransistorsPhotoinduced Charge Transfer
Abstract 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.
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General observation of n-type field-effect behaviour in organic semiconductors
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