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Understanding the Optical Properties of Doped and Undoped 9-Armchair Graphene Nanoribbons in Dispersion.
Lindenthal, Sebastian; Fazzi, Daniele; Zorn, Nicolas F; El Yumin, Abdurrahman Ali; Settele, Simon; Weidinger, Britta; Blasco, Eva; Zaumseil, Jana.
Afiliação
  • Lindenthal S; Institute for Physical Chemistry, Heidelberg University, D-69120 Heidelberg, Germany.
  • Fazzi D; Department of Chemistry "Giacomo Ciamician", University of Bologna, 40126 Bologna, Italy.
  • Zorn NF; Institute for Physical Chemistry, Heidelberg University, D-69120 Heidelberg, Germany.
  • El Yumin AA; Institute for Physical Chemistry, Heidelberg University, D-69120 Heidelberg, Germany.
  • Settele S; Institute for Physical Chemistry, Heidelberg University, D-69120 Heidelberg, Germany.
  • Weidinger B; Institute for Molecular Systems Engineering and Advanced Materials and Institute of Organic Chemistry, Heidelberg University, D-69120 Heidelberg, Germany.
  • Blasco E; Institute for Molecular Systems Engineering and Advanced Materials and Institute of Organic Chemistry, Heidelberg University, D-69120 Heidelberg, Germany.
  • Zaumseil J; Institute for Physical Chemistry, Heidelberg University, D-69120 Heidelberg, Germany.
ACS Nano ; 17(18): 18240-18252, 2023 Sep 26.
Article em En | MEDLINE | ID: mdl-37695780
ABSTRACT
Graphene nanoribbons are one-dimensional stripes of graphene with width- and edge-structure-dependent electronic properties. They can be synthesized bottom-up in solution to obtain precise ribbon geometries. Here we investigate the optical properties of solution-synthesized 9-armchair graphene nanoribbons (9-aGNRs) that are stabilized as dispersions in organic solvents and further fractionated by liquid cascade centrifugation (LCC). Absorption and photoluminescence spectroscopy reveal two near-infrared absorption and emission peaks whose ratios depend on the LCC fraction. Low-temperature single-nanoribbon photoluminescence spectra suggest the presence of two different nanoribbon species. Based on density functional theory (DFT) and time-dependent DFT calculations, the lowest energy transition can be assigned to pristine 9-aGNRs, while 9-aGNRs with edge-defects, caused by incomplete graphitization, result in more blue-shifted transitions and higher Raman D/G-mode ratios. Hole doping of 9-aGNR dispersions with the electron acceptor F4TCNQ leads to concentration dependent bleaching and quenching of the main absorption and emission bands and the appearance of red-shifted, charge-induced absorption features but no additional emission peaks, thus indicating the formation of polarons instead of the predicted trions (charged excitons) in doped 9-aGNRs.
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Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: ACS Nano Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Revista: ACS Nano Ano de publicação: 2023 Tipo de documento: Article