Semiclassical theory for plasmons in spatially inhomogeneous media
K. J. A. Reijnders, T. Tudorovskiy, M. I. Katsnelson

TL;DR
This paper introduces a semi-analytical semiclassical approach to describe bulk plasmons in spatially inhomogeneous media, extending Lindhard theory to smoothly varying charge densities, applicable to quantum plasmonic systems.
Contribution
A novel semiclassical (WKB) method for plasmons in inhomogeneous media that generalizes Lindhard theory using phase space symbols and effective Hamiltonian equations.
Findings
Derives spatially varying Lindhard theory expressions.
Provides quantization of plasmon energy levels.
Applicable to quantum plasmonic nanostructures.
Abstract
Recent progress in experimental techniques has made the quantum regime in plasmonics accessible. Since plasmons correspond to collective electron excitations, the electron-electron interaction plays an essential role in their theoretical description. Within the Random Phase Approximation, this interaction is incorporated through a system of equations of motion, which has to be solved self-consistently. For homogeneous media, an analytical solution can be found using the Fourier transform, giving rise to Lindhard theory. When the medium is spatially inhomogeneous, this is no longer possible and one often uses numerical approaches, which are however limited to smaller systems. In this paper, we present a novel semi-analytical approach for bulk plasmons in inhomogeneous media based on the semiclassical (or WKB) approximation, which is applicable when the charge density varies smoothly. By…
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