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Arbitrary power-conserving field transformations with passive lossless omega-type bianisotropic metasurfaces

机译:具有被动无损耗的任意节电场变换   ω型双向各向异性表面

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摘要

We present a general theory for designing realistic omega-type bianisotropicmetasurfaces (O-BMSs), unlocking their full potential for moldingelectromagnetic fields. These metasurfaces, characterized by electric surfaceimpedance, magnetic surface admittance, and magnetoelectric couplingcoefficient, were previously considered for wavefront manipulation. However,previous reports mainly considered plane-wave excitations, and implementationsincluded cumbersome metallic features. In this work, we prove that any fieldtransformation which locally conserves real power can be implemented viapassive and lossless meta-atoms characterized by closed-form expressions; thisallows rigorous incorporation of arbitrary source and scatteringconfigurations. Subsequently, we show that O-BMS meta-atoms can be implementedusing an asymmetric stack of three impedance sheets, an appealing structure forprinted circuit board fabrication. Our formulation reveals that, as opposed toHuygens' metasurfaces (HMSs), which exhibit negligible magnetoelectriccoupling, O-BMSs are not limited to controlling the phase of transmittedfields, but can rather achieve high level of control over the amplitude andphase of reflected fields. This is demonstrated by designing O-BMSs forreflectionless wide-angle refraction, independent surface-wave guiding, and ahighly-directive low-profile antenna, verified with full-wave simulations. Thisstraightforward methodology facilitates development of O-BMS-based devices forcontrolling the near and far fields of arbitrary sources in complex scatteringconfigurations.
机译:我们提出了设计逼真的欧米伽型双同质变表面(O-BMS)的一般理论,从而释放了它们形成电磁场的全部潜力。这些具有电表面阻抗,磁表面导纳和磁电耦合系数特征的超表面以前曾被考虑用于波前操纵。然而,先前的报道主要考虑平面波激发,并且其实现包括繁琐的金属特征。在这项工作中,我们证明了可以通过以封闭形式表示为特征的无损和无损元原子来实现任何局部保留有功功率的场变换。这允许严格合并任意源和散射配置。随后,我们展示了可以使用三个阻抗片的不对称堆叠来实现O-BMS形原子,这是印制电路板制造的一种吸引人的结构。我们的公式表明,与惠更斯的磁电耦合微不足道的超表面(HMS)相反,O-BMS不仅限于控制传输场的相位,而且可以实现对反射场的幅度和相位的高度控制。通过设计用于无反射广角折射,独立表面波导管和高指向性低剖面天线的O-BMS(通过全波仿真验证),可以证明这一点。这种简单的方法便于开发基于O-BMS的设备,用于控制复杂散射配置中任意源的近场和远场。

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