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3D versus 2D Electrolyte–Semiconductor Interfaces in Rylenediimide‐Based Electron‐Transporting Water‐Gated Organic Field‐Effect Transistors
Author(s) -
Prescimone Federico,
Benvenuti Emilia,
Natali Marco,
Lorenzoni Andrea,
Dinelli Franco,
Liscio Fabiola,
Milita Silvia,
Chen Zhihua,
Mercuri Francesco,
Muccini Michele,
Facchetti Antonio,
Toffanin Stefano
Publication year - 2020
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.202000638
Subject(s) - semiconductor , materials science , electron mobility , organic semiconductor , transistor , field effect transistor , electrolyte , optoelectronics , organic electronics , chemical physics , nanotechnology , electrode , chemistry , voltage , quantum mechanics , physics
Water‐gated organic field‐effect transistors (WGOFETs) are relevant devices for use in the fields of biosensors and biosystems. However, real applications require very stringent performance in terms of electrochemical stability and charge mobility to the organic semiconductor in contact with an aqueous environment. Here, a comparative study of two small‐molecule electron‐transporting perylenediimide semiconductors, which differ only in the N ‐substituents named PDIF‐CN 2 and PDI8‐CN 2 is reported. The two materials present similar solid‐state arrangements but, while the PDI8‐CN 2 shows a more 3D growth modality and electron mobility independent of the semiconductor layer thickness (≈10 −4 cm 2 V −1 s −1 ), the PDIF‐CN 2 has an almost‐2D growth modality and the mobility increases with the semiconductor film thickness, reaching a maximum value of ≈5 × 10 −3 cm 2 V −1 s −1 at 30 nm. Above this thickness, the PDIF‐CN 2 switches to a more 3D growth modality, and the mobility drops by one order of magnitude. XRR analysis indicates that a PDIF‐CN 2 film can be modeled as a dense layered structure in which each layer is decoupled from the others due to the presence of fluorocarbon‐chains. The availability of additional pathways for charge transport from buried layers and the 2D versus 3D growth can explain the mobility dependence on the film thickness.

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