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Charge-Transfer Plasmon Polaritons at Graphene/α-RuCl(3) Interfaces
[Image: see text] Nanoscale charge control is a key enabling technology in plasmonics, electronic band structure engineering, and the topology of two-dimensional materials. By exploiting the large electron affinity of α-RuCl(3), we are able to visualize and quantify massive charge transfer at graphe...
Autores principales: | , , , , , , , , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2020
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7729890/ https://www.ncbi.nlm.nih.gov/pubmed/33166145 http://dx.doi.org/10.1021/acs.nanolett.0c03466 |
Sumario: | [Image: see text] Nanoscale charge control is a key enabling technology in plasmonics, electronic band structure engineering, and the topology of two-dimensional materials. By exploiting the large electron affinity of α-RuCl(3), we are able to visualize and quantify massive charge transfer at graphene/α-RuCl(3) interfaces through generation of charge-transfer plasmon polaritons (CPPs). We performed nanoimaging experiments on graphene/α-RuCl(3) at both ambient and cryogenic temperatures and discovered robust plasmonic features in otherwise ungated and undoped structures. The CPP wavelength evaluated through several distinct imaging modalities offers a high-fidelity measure of the Fermi energy of the graphene layer: E(F) = 0.6 eV (n = 2.7 × 10(13) cm(–2)). Our first-principles calculations link the plasmonic response to the work function difference between graphene and α-RuCl(3) giving rise to CPPs. Our results provide a novel general strategy for generating nanometer-scale plasmonic interfaces without resorting to external contacts or chemical doping. |
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