A metamaterial with frequency dependent double negative effective properties
is constructed from a sub-wavelength periodic array of coated rods. Explicit
power series are developed for the dispersion relation and associated Bloch
wave solutions. The expansion parameter is the ratio of the length scale of the
periodic lattice to the wavelength. Direct numerical simulations for finite
size period cells show that the leading order term in the power series for the
dispersion relation is a good predictor of the dispersive behavior of the
metamaterial.
We examine the composition of the $L^{\infty}$ norm with weakly convergent
sequences of gradient fields associated with the homogenization of second order
divergence form partial differential equations with measurable coefficients.
Here the sequences of coefficients are chosen to model heterogeneous media and
are piecewise constant and highly oscillatory. We identify local representation
formulas that in the fine phase limit provide upper bounds on the limit
superior of the $L^{\infty}$ norms of gradient fields.
We obtain a convergent power series expansion for the first branch of the
dispersion relation for subwavelength plasmonic crystals consisting of
plasmonic rods with frequency-dependent dielectric permittivity embedded in a
host medium with unit permittivity. The expansion parameter is $\eta=2\pi
d/\lambda$, where $\lambda$ is a fixed wavelength and $d$ is the period of the
crystal, and the plasma frequency scales inversely to $d$, making the
dielectric permittivity in the rods large and negative.
We obtain a convergent power series expansion for the first branch of the
dispersion relation for subwavelength plasmonic crystals consisting of
plasmonic rods with frequency-dependent dielectric permittivity embedded in a
host medium with unit permittivity. The expansion parameter is $\eta=2\pi
d/\lambda$, where $\lambda$ is a fixed wavelength and $d$ is the period of the
crystal, and the plasma frequency scales inversely to $d$, making the
dielectric permittivity in the rods large and negative.
In this paper, we derive the general integral representation formulas (IRFs)
for the strain field and for the effective elasticity tensor of two-component
elastic composites. The information about the contrast is represented by a
rank-four tensor in the integrand while the information about the microgeometry
is included in the Stieltjes measure of the IRF. The relation between the IRFs
presented in this paper and those previously derived by various authors is also
explicitly established.