Abstract
Within the framework of elastic anisotropy, caused in a phononic crystal due to low crystallographic symmetry, we adopt a model structure, already introduced in the case of photonic metamaterials, and by analogy, we study the effect of birefringence and acoustical activity in a phononic crystal. In particular, we investigate its low-frequency behavior and comment on the factors which determine chirality by reference to this model.
Highlights
Within the framework of elastic anisotropy, caused in a phononic crystal due to low crystallographic symmetry, we adopt a model structure, already introduced in the case of photonic metamaterials, and by analogy, we study the effect of birefringence and acoustical activity in a phononic crystal
Acoustical activity occuring in natural crystals as a first-order spatial dispersion effect has been theoretically studied and presented by Portigal et al.[2]
A low-symmetry phononic structure will definitely introduce a sufficient elastic anisotropy which will eventually lead to what is known as acoustic birefringence.[7]
Summary
Within the framework of elastic anisotropy, caused in a phononic crystal due to low crystallographic symmetry, we adopt a model structure, already introduced in the case of photonic metamaterials, and by analogy, we study the effect of birefringence and acoustical activity in a phononic crystal. A low-symmetry phononic structure will definitely introduce a sufficient elastic anisotropy which will eventually lead to what is known as acoustic birefringence.[7]
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