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Dopant-specific unzipping of carbon nanotubes for intact crystalline graphene nanostructures

Atomic level engineering of graphene-based materials is in high demand to enable customize structures and properties for different applications. Unzipping of the graphene plane is a potential means to this end, but uncontrollable damage of the two-dimensional crystalline framework during harsh unzip...

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Detalles Bibliográficos
Autores principales: Lim, Joonwon, Narayan Maiti, Uday, Kim, Na-Young, Narayan, Rekha, Jun Lee, Won, Sung Choi, Dong, Oh, Youngtak, Min Lee, Ju, Yong Lee, Gil, Hun Kang, Seok, Kim, Hyunwoo, Kim, Yong-Hyun, Ouk Kim, Sang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4735752/
https://www.ncbi.nlm.nih.gov/pubmed/26796993
http://dx.doi.org/10.1038/ncomms10364
Descripción
Sumario:Atomic level engineering of graphene-based materials is in high demand to enable customize structures and properties for different applications. Unzipping of the graphene plane is a potential means to this end, but uncontrollable damage of the two-dimensional crystalline framework during harsh unzipping reaction has remained a key challenge. Here we present heteroatom dopant-specific unzipping of carbon nanotubes as a reliable and controllable route to customized intact crystalline graphene-based nanostructures. Substitutional pyridinic nitrogen dopant sites at carbon nanotubes can selectively initiate the unzipping of graphene side walls at a relatively low electrochemical potential (0.6 V). The resultant nanostructures consisting of unzipped graphene nanoribbons wrapping around carbon nanotube cores maintain the intact two-dimensional crystallinity with well-defined atomic configuration at the unzipped edges. Large surface area and robust electrical connectivity of the synergistic nanostructure demonstrate ultrahigh-power supercapacitor performance, which can serve for AC filtering with the record high rate capability of −85° of phase angle at 120 Hz.