可逆反射和镜面反射幅度可控的双通道超表面结构拓扑优化设计

None Shi Peng-Fei, None Ma Xin-Ying, None Xiang Chuan, None Zhao Hong-Ge, None Li Yuan, None Gao Ren-Jing, None Liu Shu-Tian
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摘要

对于斜入射电磁波,包括反向反射信道在内的双反射信道的产生对提高目标识别性能和导航性能具有重要意义。在双通道反射中,控制反向反射和镜面反射的比例是实现反射功率分配的关键。为了实现对各通道反射功率比例的控制,提出了一种双通道反射超表面微结构的拓扑优化设计方法。构建了包含反反射通道的双反射通道超表面的实现机理和物理模型,建立了反反射与镜面反射特定功率比的超表面微观结构拓扑优化模型。作为数值算例,针对10 GHz平面波在-30°入射角下的TE模式设计了一种反向反射与镜面反射功率比为1:1的双通道超表面反射器。所设计的超表面在反反射方向上具有较强的方向性,且两个方向的反射幅值相近。设计了反射率最大的反反射超表面。设计的超表面的反射率为0.093。无镜面反射和其他奇异反射,超表面强反射集中在-30°。主光束功率与全反射功率之比为0.900。仿真和实验结果验证了该方法的可行性。
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Topology optimization design of dual-channel metasurface structure with controllable amplitude of retroreflection and mirror reflection
For oblique incident electromagnetic waves, the generation of double reflection channels including retroreflection channel is of great significance to improve target recognition performance and navigation performance. In double channel reflection, controlling the proportion of retroreflection and specular reflection is the key to realize reflection power distribution. In order to realize the control of the proportion of the reflected power in each channel, a topology optimization method for designing the reflective metasurface microstructure with dual channel was proposed in this paper. The implementation mechanism and physical model of metasurface with dual reflection channel including retroreflection channel were constructed, and the topology optimization model of metasurface microstructure with specific power proportion of the retroreflection to specular reflection was established. As the numerical example, a dual channel metasurface reflector with a 1:1 ratio of retroreflection and specular reflection power was designed for a 10 GHz plane wave in the TE mode with -30 ° incident angle. The designed metasurface exhibited strong directionality in the retroreflective direction, and the reflection amplitude in both directions was similar. The retroreflective metasurface with the maximum retroreflection proportion was designed. The retroreflection proportion of the designed metasurface was 0.093. There was no specular reflection or other singular reflection, and the strong reflection on the metasurface was concentrated at -30 °. The ratio of the main beam power to the total reflection power was 0.900. The simulated and experimental results verified the feasibility of the proposed method.
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