The DOI matches its Crossref record; 11 of the 11 references it cites were found in a registry or an index.
Graphene Plasmonics for Terahertz to Mid-Infrared Applications
Open accessAbstract
In recent years, we have seen a rapid progress in the field of graphene plasmonics, motivated by graphene's unique electrical and optical properties, tunability, long-lived collective excitation and its extreme light confinement. Here, we review the basic properties of graphene plasmons: their energy dispersion, localization and propagation, plasmon-phonon hybridization, lifetimes and damping pathways. The application space of graphene plasmonics lies in the technologically significant, but relatively unexploited terahertz to mid-infrared regime. We discuss emerging and potential applications, such as modulators, notch filters, polarizers, mid-infrared photodetectors, and mid-infrared vibrational spectroscopy, among many others.
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Cites
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Cited by
Photodetectors based on graphene, other two-dimensional materials and hybrid systems
Koppens, F. H. L., Mueller, T., Avouris, P., Ferrari, A. C., Vitiello, M. S., & Polini, M. (2014) · Nature Nanotechnology · doi:10.1038/nnano.2014.215 · Cited by 3,828
Self-citationPolaritons in layered two-dimensional materials
Low, T., Chaves, A., Caldwell, J. D., Kumar, A., Fang, N. X., Avouris, P., Heinz, T. F., Guinea, F., Martin-Moreno, L., & Koppens, F. (2017) · Nature Materials · doi:10.1038/nmat4792 · Cited by 1,317
Self-citationMatter manipulation with extreme terahertz light: Progress in the enabling THz technology
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Metadata
- Authors
- Low, T., & Avouris, P.
- Venue
- ACS Nano
- Publisher
- American Chemical Society (ACS)
- Published
- 2014-01-31
- Volume
- 8
- Issue
- 2
- Pages
- 1086-1101
- ISSN
- 1936-0851 (ISSN-L)
- 1936-086X
- OpenAlex
- W2069009927
- Cited by
- 1,480
- References
- 11
- FWCI
- 72.17
- Type
- journal article
- Language
- en
- Open access
- green
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Contains information from the Semantic Scholar Academic Graph Datasets, made available under the ODC Attribution License (ODC-BY 1.0).
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