Abdelrahman Mohamed Ismail, Slivina Evgeniia, Rockstuhl Carsten, Fernandez-Corbaton Ivan
Institute of Theoretical Solid State Physics, Karlsruhe Institute of Technology, 76131, Karlsruhe, Germany.
Aix Marseille Univ, CNRS, Centrale Marseille, Institut Fresnel, 13013, Marseille, France.
Sci Rep. 2021 Jan 18;11(1):1721. doi: 10.1038/s41598-020-80347-5.
Systems with a discrete rotational symmetry [Formula: see text] where [Formula: see text] that also have electromagnetic duality symmetry exhibit zero backscattering. The impact of breaking one of the two symmetries on the emerging backscattering has not yet been systematically studied. Here, we investigate the effect that perturbatively breaking each of the two symmetries has on the backscattering off individual objects and 2D arrays. We find that the backscattering off electromagnetically-small prisms increases with the parameters that determine the symmetry breaking, and that the increase of the backscattering due to the progressive breaking of one of the symmetries can be related to the other symmetry. Further exploration of the interplay between the two symmetries reveals that, in systems lacking enough rotational symmetry, the backscattering can be almost-entirely suppressed for a given linear polarization by deliberately breaking the duality symmetry. This duality breaking can be interpreted as an effective increase of the electromagnetic degree of rotational symmetry for that linear polarization.
具有离散旋转对称性[公式:见正文](其中[公式:见正文])且还具有电磁对偶对称性的系统表现出零后向散射。打破这两种对称性之一对出现的后向散射的影响尚未得到系统研究。在此,我们研究微扰地打破这两种对称性中的每一种对单个物体和二维阵列后向散射的影响。我们发现,电磁小棱镜的后向散射随着确定对称性破缺的参数而增加,并且由于其中一种对称性的逐步破缺导致的后向散射增加可能与另一种对称性有关。对这两种对称性之间相互作用的进一步探索表明,在缺乏足够旋转对称性的系统中,通过故意打破对偶对称性,对于给定的线性极化,后向散射几乎可以完全被抑制。这种对偶性破缺可以解释为该线性极化的电磁旋转对称度的有效增加。