Acoustic dispersion in a two-dimensional dipole system
Kenneth I. Golden, Gabor J. Kalman, Zoltan Donko, Peter Hartmann

TL;DR
This paper calculates the acoustic dispersion in a 2D strongly coupled dipole system, demonstrating that correlations, not RPA, determine the long-wavelength sound velocity across classical and quantum regimes.
Contribution
It introduces a correlation-based approach to determine acoustic dispersion in 2D dipole systems, extending understanding beyond RPA limitations.
Findings
Long-wavelength acoustic phase velocity depends on particle correlations.
The velocity varies linearly with the dipole moment p.
The oscillation frequency remains invariant from classical to quantum regimes.
Abstract
We calculate the full density response function, and from it the long-wavelength acoustic dispersion for a two-dimensional system of strongly coupled point dipoles interacting through a 1/r^3 potential at arbitrary degeneracy. Such a system has no RPA limit and the calculation has to include correlations from the outset. We follow the Quasi-Localized Charge (QLC) approach, accompanied by Molecular Dynamics (MD) simulations. Similarly to what has been recently reported for the closely spaced classical electron-hole bilayer [G. J. Kalman et al. Phys. Rev. Lett. 98, 236801 (2007)] and in marked contrast to the RPA, we report a long-wavelength acoustic phase velocity that is wholly maintained by particle correlations and varies linearly with the dipole moment p. The oscillation frequency, calculated both in an extended QLC approximation and in the Singwi-Tosi-Land-Sjolander approximation,…
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