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Nonlocal homogenization theory in metamaterials: Effective electromagnetic spatial dispersion and artificial chirality

机译:超材料中的非局部均质化理论:有效的电磁空间色散和人工手性

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摘要

We develop, from first principles, a general and compact formalism for predicting the electromagnetic response of a metamaterial with nonmagnetic inclusions in the long-wavelength limit, including spatial dispersion up to the second order. Specifically, by resorting to a suitable multiscale technique, we show that the effective medium permittivity tensor and the first- and second-order tensors describing spatial dispersion can be evaluated by averaging suitable spatially rapidly varying fields, each satisfying electrostatic-like equations within the metamaterial unit cell. For metamaterials with negligible second-order spatial dispersion, we exploit the equivalence of first-order spatial dispersion and reciprocal bianisotropic electromagnetic response to deduce a simple expression for the metamaterial chirality tensor. Such an expression allows us to systematically analyze the effect of the composite spatial symmetry properties on electromagnetic chirality. We find that even if a metamaterial is geometrically achiral, i.e., it is indistinguishable from its mirror image, it shows pseudo-chiral-omega electromagnetic chirality if the rotation needed to restore the dielectric profile after the reflection is either a 0° or 90° rotation around an axis orthogonal to the reflection plane. These two symmetric situations encompass two-dimensional and one-dimensional metamaterials with chiral response. As an example admitting full analytical description, we discuss one-dimensional metamaterials whose single chirality parameter is shown to be directly related to the metamaterial dielectric profile by quadratures.
机译:我们从第一个原理发展出一种通用而紧凑的形式主义,用于预测超材料在长波长范围内具有非磁性夹杂物的电磁响应,包括直至第二阶的空间色散。具体来说,通过诉诸合适的多尺度技术,我们表明,可以通过平均合适的空间快速变化的场来评估有效的介电常数张量以及描述空间色散的一阶和二阶张量,每个场均满足超材料中的类静电方程晶胞。对于具有可忽略的二阶空间色散的超材料,我们利用一阶空间色散和倒数的各向异性电磁响应的等效性来推导超材料手性张量的简单表达式。这样的表达使我们能够系统地分析复合空间对称性对电磁手性的影响。我们发现,即使超材料在几何上是非手性的,即与它的镜像是无法区分的,如果反射后恢复介电轮廓所需的旋转为0°或90°,则它会显示伪手性-ω电磁手性。绕垂直于反射平面的轴旋转。这两个对称情况包括具有手性响应的二维和一维超材料。作为接受完整分析描述的示例,我们讨论一维超材料,其一元手性参数通过正交关系显示与超材料介电分布直接相关。

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