Dipole excitation of collective modes in viscous two-dimensional electron systems
Vera Andreeva, Denis A. Bandurin, Mitchell Luskin, Dionisios, Margetis

TL;DR
This paper analyzes electromagnetic fields generated by a dipole over a viscous 2D electron system, identifying surface plasmon and diffusive modes, and exploring effects of magnetic fields and viscosities on these modes.
Contribution
It provides an exact solution to the coupled Maxwell and hydrodynamic equations for a 2D electron system, revealing the behavior of collective modes under various conditions.
Findings
Surface plasmon dominates intermediate-field region.
Diffusive mode peaks in near-field and decays quickly.
Magnetic field causes the diffusive mode to exhibit negative group velocity.
Abstract
We describe the structure of the time-harmonic electromagnetic field of a vertical Hertzian electric dipole source radiating over an infinite, translation invariant two-dimensional electron system. Our model for the electron flow takes into account the effects of shear and Hall viscosities as well as an external static magnetic field perpendicular to the sheet. We identify two wave modes, namely, a surface plasmon and a diffusive mode. In the presence of an external static magnetic field, the diffusive mode combines the features of both the conventional and Hall diffusion and may exhibit a negative group velocity. In our analysis, we solve exactly a boundary value problem for the time-harmonic Maxwell equations coupled with linearized hydrodynamic equations for the flat, two-dimensional material. By numerically evaluating the integrals for the electromagnetic field on the sheet, we find…
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