Monoatomically thin polarizable sheets
arXiv:1404.4842 · doi:10.1103/PhysRevD.89.125015
Abstract
We consider a flat lattice of dipoles modeled by harmonic oscillators interacting with the electromagnetic field in dipole approximation. Eliminating the variables from the coupled equations of motion, we come to effective Maxwell equations. These allow for taking the lattice spacing to zero. As a result, we obtain reflection coefficients for the scattering of electromagnetic waves off the sheet. These are a generalization of that known from the hydrodynamic model. For instance, we get a non trivial scattering for polarizability perpendicular to the sheet. Also we show that the case of a sheet polarizable parallel to the sheet can be obtained in a natural way from a plasma layer of finite thickness. As an alternative approach we discuss the elimination of the electromagnetic fields resulting in effective equations for the oscillators. These show, for , divergent behavior, resulting from the electrostatic interaction of the dipoles.
8 pages
References in corpus (2)
Cited by in corpus (6)
- generalized Robin boundary conditions and quantum vacuum fluctuations
- Comparison of hydrodynamic model of graphene with recent experiment on measuring the Casimir interaction
- Electromagnetic -function sphere
- Dirac lattices, zero-range potentials and self adjoint extension
- Casimir effect for Dirac lattices
- Casimir Self-Entropy of an Electromagnetic Thin Sheet