Electron-electron interactions and plasmon dispersion in graphene

Plasmons in two-dimensional electron systems with nonparabolic bands, such as graphene, feature strong dependence on electron-electron interactions. We use a many-body approach to relate plasmon dispersion at long wavelengths to Landau Fermi-liquid interactions and quasiparticle velocity. An identic...

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Main Authors: Shtyk, A., Feigelman, M., Levitov, Leonid
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Language:en_US
Published: American Physical Society 2014
Online Access:http://hdl.handle.net/1721.1/88762
https://orcid.org/0000-0002-4268-731X
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author Shtyk, A.
Feigelman, M.
Levitov, Leonid
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Shtyk, A.
Feigelman, M.
Levitov, Leonid
author_sort Shtyk, A.
collection MIT
description Plasmons in two-dimensional electron systems with nonparabolic bands, such as graphene, feature strong dependence on electron-electron interactions. We use a many-body approach to relate plasmon dispersion at long wavelengths to Landau Fermi-liquid interactions and quasiparticle velocity. An identical renormalization is shown to arise for the magnetoplasmon resonance. For a model with N ≫ 1 fermion species, this approach predicts a power-law dependence for plasmon frequency vs carrier concentration, valid in a wide range of doping densities, both high and low. Gate tunability of plasmons in graphene can be exploited to directly probe the effects of electron-electron interaction.
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spelling mit-1721.1/887622022-09-29T16:18:26Z Electron-electron interactions and plasmon dispersion in graphene Shtyk, A. Feigelman, M. Levitov, Leonid Massachusetts Institute of Technology. Department of Physics Levitov, Leonid Plasmons in two-dimensional electron systems with nonparabolic bands, such as graphene, feature strong dependence on electron-electron interactions. We use a many-body approach to relate plasmon dispersion at long wavelengths to Landau Fermi-liquid interactions and quasiparticle velocity. An identical renormalization is shown to arise for the magnetoplasmon resonance. For a model with N ≫ 1 fermion species, this approach predicts a power-law dependence for plasmon frequency vs carrier concentration, valid in a wide range of doping densities, both high and low. Gate tunability of plasmons in graphene can be exploited to directly probe the effects of electron-electron interaction. MIT Skoltech Initiative 2014-08-18T16:15:03Z 2014-08-18T16:15:03Z 2013-12 2013-02 Article http://purl.org/eprint/type/JournalArticle 1098-0121 1550-235X http://hdl.handle.net/1721.1/88762 Levitov, L., A. Shtyk, and M. Feigelman. “Electron-Electron Interactions and Plasmon Dispersion in Graphene.” Phys. Rev. B 88, no. 23 (December 2013). © 2013 American Physical Society https://orcid.org/0000-0002-4268-731X en_US http://dx.doi.org/10.1103/PhysRevB.88.235403 Physical Review B Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. application/pdf American Physical Society American Physical Society
spellingShingle Shtyk, A.
Feigelman, M.
Levitov, Leonid
Electron-electron interactions and plasmon dispersion in graphene
title Electron-electron interactions and plasmon dispersion in graphene
title_full Electron-electron interactions and plasmon dispersion in graphene
title_fullStr Electron-electron interactions and plasmon dispersion in graphene
title_full_unstemmed Electron-electron interactions and plasmon dispersion in graphene
title_short Electron-electron interactions and plasmon dispersion in graphene
title_sort electron electron interactions and plasmon dispersion in graphene
url http://hdl.handle.net/1721.1/88762
https://orcid.org/0000-0002-4268-731X
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