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Charge‐Transfer‐Controlled Growth of Organic Semiconductor Crystals on Graphene

Controlling the growth behavior of organic semiconductors (OSCs) is essential because it determines their optoelectronic properties. In order to accomplish this, graphene templates with electronic‐state tunability are used to affect the growth of OSCs by controlling the van der Waals interaction bet...

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Detalles Bibliográficos
Autores principales: Nguyen, Nguyen Ngan, Lee, Hyo Chan, Yoo, Min Seok, Lee, Eunho, Lee, Hansol, Lee, Seon Baek, Cho, Kilwon
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7080519/
https://www.ncbi.nlm.nih.gov/pubmed/32195079
http://dx.doi.org/10.1002/advs.201902315
Descripción
Sumario:Controlling the growth behavior of organic semiconductors (OSCs) is essential because it determines their optoelectronic properties. In order to accomplish this, graphene templates with electronic‐state tunability are used to affect the growth of OSCs by controlling the van der Waals interaction between OSC ad‐molecules and graphene. However, in many graphene‐molecule systems, the charge transfer between an ad‐molecule and a graphene template causes another important interaction. This charge‐transfer‐induced interaction is never considered in the growth scheme of OSCs. Here, the effects of charge transfer on the formation of graphene–OSC heterostructures are investigated, using fullerene (C(60)) as a model compound. By in situ electrical doping of a graphene template to suppress the charge transfer between C(60) ad‐molecules and graphene, the layer‐by‐layer growth of a C(60) film on graphene can be achieved. Under this condition, the graphene–C(60) interface is free of Fermi‐level pinning; thus, barristors fabricated on the graphene–C(60) interface show a nearly ideal Schottky–Mott limit with efficient modulation of the charge‐injection barrier. Moreover, the optimized C(60) film exhibits a high field‐effect electron mobility of 2.5 cm(2) V(−1) s(−1). These results provide an efficient route to engineering highly efficient optoelectronic graphene–OSC hybrid material applications.