Dielectric matrix and plasmon dispersion in strongly coupled electronic bilayer liquids
arXiv:cond-mat/0410575 · doi:10.1103/PhysRevE.71.036401
Abstract
We develop a dielectric matrix and analyze plasmon dispersion in strongly coupled charged-particle bilayers in the quantum domain. The formulation is based on the classical quasi-localized charge approximation (QLCA) and extends the QLCA formalism into the quantum domain. Its development, which parallels that of 2D companion paper [Phys. Rev. E 70, 026406 (2004)] by three of the authors, generalizes the single-layer scalar formalism therein to a bilayer matrix formalism. Using pair correlation function data generated from diffusion Monte Carlo simulations, we calculate the dispersion of the in-phase and out-of-phase plasmon modes over a wide range of in-layer coupling values and layer spacings. The out-of-phase spectrum exhibits an exchange-correlation induced long-wavelength energy gap in contrast to earlier predictions of acoustic dispersion softened by exchange-correlations. The energy gap is similar to what has been previously predicted for classical charged-particle bilayers and subsequently confirmed by recent molecular dynamics computer simulations.
arXiv comment53 pages including 15 Figures with their captions. Submitted to Physical Review E
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Cited by in corpus (4)
- Dynamical correlations and collective excitations of Yukawa liquids
- Exchange and correlation effects on the plasmon dispersions and the Coulomb drag in low-density electron bilayers
- Collective excitations in electron-hole bilayers
- Collective excitations and quantum incompressibility in electron-hole bilayers