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Surface plasmon at a metal-dielectric interface with an epsilon-near-zero transition layer

Kevin Roccapriore1,2, Andrey Bozhko1, Gleb Nazarikov3,4, Vladimir Drachev1,3,*, and Arkadii Krokhin1,†

  • 1Department of Physics, University of North Texas, P.O. Box 311427, Denton, Texas 76203, USA
  • 2Center for Nanophase Materials Sciences, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 3Skolkovo Institute of Science and Technology, 3 Nobel Street, Moscow 143026 Russia
  • 4Department of Electrical Engineering, Eindhoven University of Technology, 5600 MB Eindhoven, The Netherlands

  • *vladimir.drachev@unt.edu
  • †Arkadii.Krokhin@unt.edu

Phys. Rev. B 103, L161404 – Published 13 April, 2021

DOI: https://doi.org/10.1103/PhysRevB.103.L161404

Abstract

A metal-dielectric interface is usually modeled by a zero-width layer, where dielectric permittivity suffers a discontinuity jump. In reality, there is a narrow transition region, which includes an epsilon-near-zero (ENZ) layer. We show that due to a continuous dielectric function the dispersion of the surface plasmon is modified. The energy of the surface plasmon radiates through the ENZ layer, giving rise to additional radiative losses. Direct evidence of the effects related to the transition layer is given by the observation of plasmonic resonance in the presence of a strong electric field normal to the metal film. The electric field affects the electron density within the transition layer that leads to a measurable shift of the plasmonic resonance.

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