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Related Experiment Video

Updated: Jun 3, 2026

Design, Fabrication, and Experimental Characterization of Plasmonic Photoconductive Terahertz Emitters
10:54

Design, Fabrication, and Experimental Characterization of Plasmonic Photoconductive Terahertz Emitters

Published on: July 8, 2013

Terahertz surface plasmons in optically pumped graphene structures.

A A Dubinov1, V Ya Aleshkin, V Mitin

  • 1Computational Nanoelectronics Laboratory, University of Aizu, Aizu-Wakamatsu, Japan.

Journal of Physics. Condensed Matter : an Institute of Physics Journal
|March 29, 2011
PubMed
Summary
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Optically pumped graphene structures can amplify terahertz surface plasmons (SPs) when conductivity becomes negative. This finding is crucial for developing advanced graphene-based terahertz lasers and devices.

Area of Science:

  • Condensed Matter Physics
  • Optoelectronics
  • Nanotechnology

Background:

  • Surface plasmons (SPs) are electromagnetic waves coupled to electron oscillations at material surfaces.
  • Graphene's unique electronic properties make it a promising material for manipulating SPs.
  • Optical pumping can alter graphene's conductivity, potentially leading to novel optical phenomena.

Purpose of the Study:

  • To investigate the behavior of terahertz (THz) SPs in optically pumped single-graphene layer (SGL) and multiple-graphene layer (MGL) structures.
  • To determine the conditions under which THz SP damping can be overcome by amplification.
  • To compare the SP amplification potential of SGL and MGL structures.

Main Methods:

  • Theoretical analysis of SP propagation in optically pumped graphene.

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Last Updated: Jun 3, 2026

Design, Fabrication, and Experimental Characterization of Plasmonic Photoconductive Terahertz Emitters
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Published on: July 8, 2013

Determination of the Excitation and Coupling Rates Between Light Emitters and Surface Plasmon Polaritons
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Determination of the Excitation and Coupling Rates Between Light Emitters and Surface Plasmon Polaritons

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  • Calculation of dynamic conductivity considering interband population inversion.
  • Modeling of SP gain in SGL and MGL configurations.
  • Main Results:

    • Negative dynamic conductivity in the THz range was achieved in SGL and MGL structures under strong optical pumping.
    • This negative conductivity leads to the amplification of THz SPs, overcoming damping.
    • SP gain is significantly influenced by the number of graphene layers, with an optimal number for maximization.

    Conclusions:

    • Optically pumped graphene structures can exhibit THz SP amplification, a key effect for active THz devices.
    • The observed SP gain is substantial and can exceed that in dielectric waveguide structures.
    • Tailoring the number of graphene layers is essential for optimizing SP gain in graphene-based THz devices.