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Near-Field Electromagnetic Analysis of Perfect Black Fresnel Zone Plates Using Radial Polarization

机译:理想黑菲涅尔波带片的径向极化近场电磁分析

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We analyze the near-field focalization properties of perfect black Fresnel Zone Plates (FZPs) through the exact solutions of Maxwell equations for radially polarized fields obtained by means of Luneburg vector diffraction theory. The electromagnetic fields are computed assuming Hermite-Gauss and Bessel-Gauss beams as boundary conditions at the FZP plane $z=0$, which allows us to demonstrate that the total intensity is necessarily focused at $z=0$ and thus there is not much improvement of the intensity resolution at the focal plane. On the other hand, the Poynting vector exhibits multiple vortices and saddle points in the near-field region while its $z$ component vanishes at the FZP axis and has a large focal depth as well as several residual contributions outside the focal region. These facts suggest that perfect black FZPs do not focus radially polarized fields at the designed focal length when such length is comparable to the wavelength (or smaller). Our results are very similar to the ones obtained for phase FZPs and they are in good agreement with FDTD simulations.
机译:我们通过利用Luneburg矢量衍射理论获得的径向偏振场的麦克斯韦方程组的精确解,分析了完美的黑色菲涅耳带状平板(FZPs)的近场聚焦特性。计算电磁场时假设Hermite-Gauss和Bessel-Gauss束为FZP平面$ z = 0 $的边界条件,这使我们能够证明总强度必定集中在$ z = 0 $上,因此没有焦平面处的强度分辨率大大提高。另一方面,Poynting向量在近场区域表现出多个涡旋和鞍点,而其$ z $分量在FZP轴上消失,并且具有较大的焦点深度以及焦点区域之外的一些剩余贡献。这些事实表明,完美的黑色FZP不能将径向偏振场聚焦在设计的焦距上,而该长度与波长相当(或更小)。我们的结果与相位FZP的结果非常相似,并且与FDTD仿真非常吻合。

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