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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匀化理论:有效   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 forpredicting the electromagnetic response of a metamaterial with non-magneticinclusions in the long wavelength limit, including spatial dispersion up to thesecond order. Specifically, by resorting to a suitable multiscale technique, weshow that medium effective permittivity tensor and the first and second ordertensors describing spatial dispersion can be evaluated by averaging suitablespatially rapidly-varying fields each satysifing electrostatic-like equationswithin the metamaterial unit cell. For metamaterials with negligiblesecond-order spatial dispersion, we exploit the equivalence of first-orderspatial dispersion and reciprocal bianisotropic electromagnetic response todeduce a simple expression for the metamaterial chirality tensor. Such anexpression allows us to systematically analyze the effect of the compositespatial symmetry properties on electromagnetic chirality. We find that even ifa metamaterial is geometrically achiral, i.e. it is indistinguishable from itsmirror image, it shows pseudo-chiral-omega electromagnetic chirality if therotation needed to restore the dielectric profile after the reflection iseither a $0^\circ$ or $90^\circ$ rotation around an axis orthogonal to thereflection plane. These two symmetric situations encompass two-dimensional andone-dimensional metamaterials with chiral response. As an example admittingfull analytical description, we discuss one-dimensional metamaterials whosesingle chirality parameter is shown to be directly related to the metamaterialdielectric profile by quadratures.
机译:我们从第一个原理开始,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。具体而言,通过诉诸合适的多尺度技术,我们表明可以通过平均每个满足超材料单元格内的静电式方程的空间快速变化的场平均,来评估中等有效介电常数张量以及描述空间色散的第一和第二阶张量。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相互各向异性的电磁响应的等效性来推导出超材料手性张量的简单表达式。这种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,即它与它的镜面图像是无法区分的,如果反射后恢复介电轮廓所需的旋转是$ 0 ^ \ circ $或$ 90 ^ \ circ,它也显示出伪手性-ω电磁手性。绕正交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。作为一个可以接受完整分析描述的例子,我们讨论了一维超材料,其单手性参数通过正交关系与超材料介电分布直接相关。

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