Karmakar Subrata, Ringne Anil, Kumar Nirjhar, Krishnan Ananth
Department of Electrical Engineering, Centre for NEMS and Nanophotonics (CNNP), Indian Institute of Technology Madras, Chennai, 600036, India.
Sci Rep. 2024 Dec 28;14(1):31499. doi: 10.1038/s41598-024-83191-z.
Transmission-type plasmonic phase metasurfaces utilizing the Pancharatnam-Berry (PB) phase require constant transmittivity with complete phase variation from 0 to 2π. Usually, this is achieved by rotating metallic nanoparticles in an otherwise uniform lattice arrangement. However, this rotation and the chosen lattice structure cause a significant change in the transmittivity, resulting in a lower intensity of light with certain phases and a higher intensity for other phases. Even though they are called full phase metasurfaces, their intensities can be near maximum or near minimum depending on the rotation and the lattice structure. We show that it is possible to achieve full phase constant transmittivity metasurfaces using the PB phase and the most elementary metallic anisotropic nanoparticles (elliptical) by inserting a thin metal sheet between the nanoparticles and the substrate. Without this metal sheet, while full phase control could be achieved by merely rotating the particles, the transmittivity varies by about 50% depending on the nanoparticles' orientation. With the metal sheet, full phase control from 0-2π with a transmittivity variation of only 13%, even in a square lattice, is demonstrated with simulations and experiments. We show that this is due to the annihilation of quadrupole resonances along with broader uniform dipole resonance in the case of the nanoparticles with the metal sheet below. We also show that precise phase control is possible by generating varieties of orbital angular momentum beams and complex beams in the visible spectrum using nanofabricated metasurfaces.
利用潘查拉特纳姆 - 贝里(PB)相位的透射型表面等离激元相位超表面需要在0到2π的完整相位变化过程中保持恒定的透过率。通常,这是通过在均匀晶格排列中旋转金属纳米颗粒来实现的。然而,这种旋转以及所选的晶格结构会导致透过率发生显著变化,使得某些相位的光强度较低,而其他相位的光强度较高。尽管它们被称为全相位超表面,但根据旋转和晶格结构的不同,其强度可能接近最大值或最小值。我们表明,通过在纳米颗粒和衬底之间插入一层薄金属片,利用PB相位和最基本的金属各向异性纳米颗粒(椭圆形),可以实现全相位恒定透过率的超表面。没有这片金属片时,虽然仅通过旋转颗粒就能实现全相位控制,但透过率会根据纳米颗粒的取向变化约50%。通过模拟和实验证明,有了这片金属片,即使在正方形晶格中,也能实现从0到2π的全相位控制,透过率变化仅为13%。我们表明,这是由于在下方带有金属片的纳米颗粒情况下,四极子共振的湮灭以及更宽的均匀偶极子共振。我们还表明,使用纳米制造的超表面在可见光谱中产生各种轨道角动量光束和复光束,可以实现精确的相位控制。