K. Chong, Lei Wang, I. Staude, Anthony James, J. Dominguez, G. Subramania, Sheng Liu, M. Decker, D. Neshev, I. Brener, Y. Kivshar
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A promising way to overcome these limitations is the use of metamaterial Huygens’ surfaces [2-4], i.e., reflection-less surfaces that can also provide full 360 degree phase coverage in transmission. Plasmonic implementations of Huygens’ surfaces for microwave [2] and the mid-infrared spectral range [3], where the intrinsic losses of the metals are negligible, have been suggested, however, these designs cannot be transferred to near-infrared or even visible frequencies because of the high dissipative losses of plasmonic structures at optical frequencies. Here, we demonstrate the first holographic metasurface utilizing the concept of all-dielectric Huygens’ surfaces thereby achieving record transmission efficiencies of approximately 82% at 1477nm wavelength. Our low-loss Huygens’ surface is realized by two-dimensional subwavelength arrays of loss-less silicon nanodisks with both electric and magnetic dipole resonances [4]. By controlling the intrinsic properties of the resonances, i.e. their relative electric and magnetic polarizabilities, quality factors and spectral position, we can design silicon nanodisks to behave as near-ideal Huygens’ particles. This allows us to realize all-dielectric Huygens’ surfaces providing full 360 degree phase coverage that lack dissipative losses and also suppress unwanted reflections without relying on cross-polarization schemes that additionally suffer from polarization-conversion losses. We now use such Huygens’ surfaces in order to create a highly-efficient phase masks for the generation of optical holograms. By varying only one geometrical parameter, namely the lattice periodicity that can be controlled easily during the fabrication process we can effectively generate arbitrary hologram images from a 4-level phase discretization. In order to design the arrangement of the pixels in the metasurfaces, we calculate the phase mask required for a hologram generating the letters ‘hv’ in the hologram plane. In the next step the Huygens’ hologram is fabricated on a back-side polished SOI wafer by electron-beam lithography followed by a reactive-ion etching process. Then, we measure the phase of the generated hologram using a home-built Mach-Zehnder interferometer and perform a phase retrieval process to compare the experimental phase with the designed phase. Finally, we record the holographic image in the hologram plane and demonstrate that the device functionality is completely polarization insensitive with a transmission efficiency of 82%, in contrast to all the earlier works utilizing geometric phase. References [1] Yu et al., Nat. Mater. 13, 139 (2014). [2] Pfeiffer et al., Phys. Rev. Lett. 110, 197401 (2013). [3] Monticone et al., Phys. Rev. Lett. 110, 203903 (2013). [4] Decker et al., Adv. Opt. 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Plasmonic implementations of Huygens’ surfaces for microwave [2] and the mid-infrared spectral range [3], where the intrinsic losses of the metals are negligible, have been suggested, however, these designs cannot be transferred to near-infrared or even visible frequencies because of the high dissipative losses of plasmonic structures at optical frequencies. Here, we demonstrate the first holographic metasurface utilizing the concept of all-dielectric Huygens’ surfaces thereby achieving record transmission efficiencies of approximately 82% at 1477nm wavelength. Our low-loss Huygens’ surface is realized by two-dimensional subwavelength arrays of loss-less silicon nanodisks with both electric and magnetic dipole resonances [4]. By controlling the intrinsic properties of the resonances, i.e. their relative electric and magnetic polarizabilities, quality factors and spectral position, we can design silicon nanodisks to behave as near-ideal Huygens’ particles. 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引用次数: 0
摘要
光学超表面是先进波前研究的一个突破性概念。这些“设计师元表面”[1]的关键在于它们提供了完整的360度相位覆盖,并且它们的局部相位可以精确控制。在光学薄平面上对相位、振幅和偏振的局部控制将导致集成光学、平面显示、能量收集和中红外光子学等领域的新型平面光学元件,具有更高的性能和功能。然而,反射和/或吸收损耗以及低偏振转换效率是实现实际应用所需的高传输效率的根本障碍。克服这些限制的一个有希望的方法是使用超材料惠更斯表面[2-4],即无反射表面,也可以在传输中提供完整的360度相位覆盖。惠更斯表面的等离子体实现用于微波[2]和中红外光谱范围[3],其中金属的本征损耗可以忽略不计,然而,由于等离子体结构在光学频率的高耗散损耗,这些设计不能转移到近红外甚至可见频率。在这里,我们展示了第一个利用全介电惠更斯表面概念的全息超表面,从而在1477nm波长下实现了约82%的传输效率。我们的低损耗惠更斯表面是由具有电偶极子共振和磁偶极子共振的无损耗硅纳米片的二维亚波长阵列实现的[4]。通过控制共振的固有特性,即它们的相对电极化率和磁极化率、质量因子和光谱位置,我们可以设计出接近理想惠更斯粒子的硅纳米片。这使我们能够实现全介电惠更斯表面,提供完整的360度相位覆盖,缺乏耗散损耗,也抑制了不必要的反射,而不依赖于额外遭受偏振转换损耗的交叉极化方案。我们现在使用这样的惠更斯表面来创建一个高效的相位掩模,用于生成光学全息图。通过改变一个几何参数,即在制作过程中易于控制的晶格周期性,我们可以有效地从4级相位离散中生成任意全息图像。为了设计元表面上像素的排列,我们计算了全息图在全息图平面上产生字母“hv”所需的相位掩模。下一步,惠更斯号的全息图通过电子束光刻和反应蚀刻工艺在背面抛光的SOI晶圆上制作。然后,我们使用自制的Mach-Zehnder干涉仪测量生成的全息图的相位,并进行相位恢复过程以比较实验相位和设计相位。最后,我们将全息图像记录在全息图平面上,并证明了该器件的功能是完全偏振不敏感的,传输效率为82%,与之前所有利用几何相位的工作形成对比。[1]余等,自然科学学报,13,139(2014)。[2]李春华,李春华。Rev. Lett. 110, 197401(2013)。[3]李春华,李春华,李春华。Rev. Lett. 110, 203903(2013)。[4]李建军,李建军,李建军,等。生物医学工程学报,2015,32(4):555 - 557。
Optical metasurfaces have developed as a breakthrough concept for advanced wave-front. Key to these “designer metasurfaces”[1] is that they provide full 360 degree phase coverage and that their local phase can be precisely controlled. The local control of phase, amplitude and polarization on an optically thin plane will lead to a new class of flat optical components in the areas of integrated optics, flat displays, energy harvesting and mid-infrared photonics, with increased performance and functionality. However, reflection and/or absorption losses as well as low polarization-conversion efficiencies pose a fundamental obstacle for achieving high transmission efficiencies that are required for practical applications. A promising way to overcome these limitations is the use of metamaterial Huygens’ surfaces [2-4], i.e., reflection-less surfaces that can also provide full 360 degree phase coverage in transmission. Plasmonic implementations of Huygens’ surfaces for microwave [2] and the mid-infrared spectral range [3], where the intrinsic losses of the metals are negligible, have been suggested, however, these designs cannot be transferred to near-infrared or even visible frequencies because of the high dissipative losses of plasmonic structures at optical frequencies. Here, we demonstrate the first holographic metasurface utilizing the concept of all-dielectric Huygens’ surfaces thereby achieving record transmission efficiencies of approximately 82% at 1477nm wavelength. Our low-loss Huygens’ surface is realized by two-dimensional subwavelength arrays of loss-less silicon nanodisks with both electric and magnetic dipole resonances [4]. By controlling the intrinsic properties of the resonances, i.e. their relative electric and magnetic polarizabilities, quality factors and spectral position, we can design silicon nanodisks to behave as near-ideal Huygens’ particles. This allows us to realize all-dielectric Huygens’ surfaces providing full 360 degree phase coverage that lack dissipative losses and also suppress unwanted reflections without relying on cross-polarization schemes that additionally suffer from polarization-conversion losses. We now use such Huygens’ surfaces in order to create a highly-efficient phase masks for the generation of optical holograms. By varying only one geometrical parameter, namely the lattice periodicity that can be controlled easily during the fabrication process we can effectively generate arbitrary hologram images from a 4-level phase discretization. In order to design the arrangement of the pixels in the metasurfaces, we calculate the phase mask required for a hologram generating the letters ‘hv’ in the hologram plane. In the next step the Huygens’ hologram is fabricated on a back-side polished SOI wafer by electron-beam lithography followed by a reactive-ion etching process. Then, we measure the phase of the generated hologram using a home-built Mach-Zehnder interferometer and perform a phase retrieval process to compare the experimental phase with the designed phase. Finally, we record the holographic image in the hologram plane and demonstrate that the device functionality is completely polarization insensitive with a transmission efficiency of 82%, in contrast to all the earlier works utilizing geometric phase. References [1] Yu et al., Nat. Mater. 13, 139 (2014). [2] Pfeiffer et al., Phys. Rev. Lett. 110, 197401 (2013). [3] Monticone et al., Phys. Rev. Lett. 110, 203903 (2013). [4] Decker et al., Adv. Opt. Mater. 3, 813 (2015).