Local metamaterials and transition layers

TL;DR

This paper clarifies the concept of local acoustic metamaterials, characterizes their wave properties via conic and quadric EFCs, and introduces transition layers for accurate scattering predictions.

Contribution

It provides a detailed analysis of local acoustic metamaterials' EFC geometries and introduces a simple Drude-layer model for precise scattering calculations.

Findings

EFCs are conics in 2D and quadrics in 3D for local media.

Hyperbolas indicate negative properties in 2D; hyperboloids in 3D.

Transition layers improve scattering prediction accuracy to within 2%.

Abstract

In this paper, we elucidate the concept of local acoustic metamaterials. These are composites which exhibit equi-frequency contours (EFC) which correspond to those expected of homogeneous local acoustic media. We show that EFCs for local acoustic media are conics in 2-dimension and quadrics in 3-dimension. In 2-D, the sure signature of negative properties is if the conic is a hyperbola and in 3-D, the sure signature is the presence of hyperboloids. We note that metamaterial coupling (Willis coupling) has the potential of translating these conics and quadrics in the wave-vector plane but that it does not fundamentally change the shape of these geometries. The local effective properties assigned to a composite in such cases are dispersive (frequency dependent) and they satisfy causality considerations. We finally also show that such properties truly characterize the composite in the sense that they can be used to solve scattering problems involving different samples of the composite. We show that this is made possible through the consideration of transition layers. While the sharp-interface model incurs scattering errors exceeding 20\% at oblique angles, the Drude-layer model restores agreement to within 2\% without requiring integral-equation or multi-mode expansions, thereby offering a simple yet highly efficient route to accurate scattering predictions in resonant local acoustic metamaterials.