Two-dimensional plasmons in the random impedance network model of disordered thin-film nanocomposites
arXiv:1710.00949 · doi:10.1103/PhysRevB.97.184204
Abstract
Random impedance networks are widely used as a model to describe plasmon resonances in disordered metal-dielectric nanocomposites. In order to study thin films, two-dimensional networks are often used despite the fact that such networks correspond to a two-dimensional electrodynamics [J.P. Clerc et al, J. Phys. A 29, 4781 (1996)]. In the present work, we propose a model of two-dimensional systems with three-dimensional Coulomb interaction and show that this model is equivalent to a planar network with long-range capacitive connections between sites. In a case of a metal film, we get a known dispersion of plane-wave two-dimensional plasmons. In the framework of the proposed model, we study the evolution of resonances with decreasing of metal filling factor. In the subcritical region with metal filling lower than the percolation threshold , we observe a gap with Lifshitz tails in the spectral density of states (DOS). In the supercritical region , the DOS demonstrates a crossover between plane-wave two-dimensional plasmons and resonances associated with small clusters.
arXiv comment8 pages, 3 figures, revtex; references added
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