Effective dielectric constants of photonic crystal of aligned anisotropic cylinders and the optical response of a periodic array of carbon nanotubes

Effective dielectric constants of photonic crystal of aligned anisotropic cylinders and the optical response of a periodic array of carbon nanotubes

Date: October 25, 2005
Creator: Reyes, E.; Krokhin, Arkadii A. & Roberts, James A.
Description: This article discusses effective dielectric constants of photonic crystal of aligned anisotropic cylanders and the optical response of a periodic array of carbon nanotubes. Abstract: We calculate the static dielectric tensor of a periodic system of aligned anisotropic dielectric cylinders. Exact analytical formula for the effective dielectric constants for the H-eigenmodes is obtained for arbitrary 2D Bravais lattice and arbitrary cross section of anisotropic cylinders behaves like uniaxial or biaxial natural crystals. The developed theory of homogenization of anisotropic cylinders is applied for calculations of the dielectric properties of photonic crystals of carbon nanotubes.
Contributing Partner: UNT College of Arts and Sciences
Low-frequency index of refraction for a two-dimensional metallodielectric photonic crystal

Low-frequency index of refraction for a two-dimensional metallodielectric photonic crystal

Date: January 29, 2007
Creator: Krokhin, Arkadii; Reyes, E. & Gumen, L.
Description: In this article, the authors calculate analytically the effective index of refraction n(eff) of a periodic arrangement of nonmagnetic metallic cylinders in the low-frequency limit. At ω→0 the dielectric constant of the cylanders is singular, ᄐm(ω)≈-(ωp/ω)², allowing propagation in the plane of periodicity of a mode with the magnetic field parallel to the cylanders (H polarization). The in-plane electric field induces eddy currents, which are localized in a narrow skin layer. The authors show that the magnetic moment of the eddy current leads to diamagnetic response if the radius of the cylanders is larger than the skin depth δ-10⁻⁵ cm. Otherwise, the cylinders are transparent for the electromagnetic field and their magnetic moment can be neglected. Magnetization of the cylinders gives rise to distinct values of the quasistatic and static indices of refraction and explains a paradox with noncommuting limits ᄐm→∞ and ω→0.
Contributing Partner: UNT College of Arts and Sciences