太赫兹超表面计算全息

刘星博,王球,许全,等. 太赫兹超表面计算全息[J]. 光电工程,2020,47(5):190674. doi: 10.12086/oee.2020.190674
引用本文: 刘星博,王球,许全,等. 太赫兹超表面计算全息[J]. 光电工程,2020,47(5):190674. doi: 10.12086/oee.2020.190674
Liu X B, Wang Q, Xu Q, et al. Metasurface-based computer generated holography at terahertz frequencies[J]. Opto-Electron Eng, 2020, 47(5): 190674. doi: 10.12086/oee.2020.190674
Citation: Liu X B, Wang Q, Xu Q, et al. Metasurface-based computer generated holography at terahertz frequencies[J]. Opto-Electron Eng, 2020, 47(5): 190674. doi: 10.12086/oee.2020.190674

太赫兹超表面计算全息

  • 基金项目:
    广西自动检测技术与仪器重点实验室基金项目(YQ18205)
详细信息
    作者简介:
    通讯作者: 许全(1990-),男,博士,助理教授,主要从事太赫兹超表面的研究。E-mail:quanxu@tju.edu.cn
  • 中图分类号: TB877; O438.1

Metasurface-based computer generated holography at terahertz frequencies

  • Fund Project: Supported by Guangxi Key Laboratory of Automatic Detecting Technology and Instruments (YQ18205)
More Information
  • 全息术是一种三维成像技术,它已经被应用于多种实际场景。随着计算机科学与技术的迅猛发展,计算全息由于其方便和灵活的特性,已经成为一种广泛应用的全息成像方法。本文回顾了我们近期基于超表面的太赫兹计算全息研究进展。其中,作为全息板的超表面展示出了超越传统光学器件的独特性能。首先,利用超表面实现了对于全息板每个像素的相位振幅同时且独立的调控,进而实现了高质量全息成像。这种新的电磁波操控能力也带来了新的全息成像效果,如利用介质超表面实现了全息像沿传播方向上的连续变化。其次,对超表面在不同偏振态下的响应进行设计,分别实现了线偏振态与频率复用、圆偏振态复用、以及基于表面波的偏振复用超表面全息术。此外,本文提出了依赖于温度变化而主动可控的超表面全息术,为今后计算全息术的设计与实现提供了新的方案,也推动了超表面在实际应用方面的发展。

  • Overview: We review our recent progress in metasurface-based terahertz computer generated holography in which metasurfaces act as the holograms and show novel advantages.

    To get better quality of holographic image, the unit should modulate both amplitude and phase of incidence rather than just one of them. Based on the different resonance modes caused by parallel polarization incidence and perpendicular polarization incidence, a series of different C-shape split-ring resonators (CSRRs) are designed which have different modulating effects with each other in y-polarized transmittance and phase shift spectra under x-polarized normal incidence.

    Although a fine hologram can be composed by CSRRs, its energy efficiency is low. To solve this problem, we resort to the all-dielectric metasurface. Its units are silicon pillar resonators which not only own the high energy efficiency but also can modulate both amplitude and phase of incidence like CSRRs.

    To improve utilization efficiency of holograms, the multiplexed metasuface is one of the ideal solutions. The multiplexed holograms can increase information capacity of imaging system and make it more simplified. For these reasons, some multiplexed meta-holograms emerged in our works.

    Firstly, a meta-hologram which is a linear polarization and frequency multiplexed one is designed. On the hologram, two sets of CSRRs which work at different frequencies are arranged and a pattern like checkerboard formed. Due to special design some CSRRs do not work when others do. Based on CSRRs working at different frequencies and the special arrangement, the linear polarization and frequency multiplexed hologram is achieved.

    Secondly, a circular polarization multiplexed hologram is realized. There are two types of units on it which are L-type DSRRs (double-split ring resonators) and R-type DSRRs respectively and they response to the left-handed or right-handed circular polarization only. Based on the Pancharatnam-Berry phase and a modified Gerchberg-Saxton algorithm, the hologram shows different holographic images under left-handed and right-handed circular polarization incidence, respectively.

    Thirdly, a surface plasmon holography which is polarization multiplexed is also achieved. On these holograms, slit-pair resonators act as the pixels. The holographic images are composed by a series of surface plasmon which excited by different pixels. The initial phase of surface plasmon from pixels is depended on the origin of the slit-pair resonator and the polarization of incidence.

    Finally, a thermally dependent active control meta-hologram is also designd and demonstrated in experiment. There are two sets of units on it which are passive units and active units. They are CSRRs and V-CSRRs (vanadium dioxide integrated CSRRs) which are CSRRs contained vanadium dioxide in their gaps. Based on the phase transition effect of vanadium dioxide andreasonable arrangement of passive and active units and destructive interference images showed by them, the hologram shows different holographic images in low and high temperatures, respectively.

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  • 图 1  C形谐振环结构单元和成像原理[37]

    Figure 1.  Basic functional units and the design of hologram[37]

    图 2  全介质单元结构和振幅相位调制原理[44]

    Figure 2.  Illustration of the basic functional unit cells[44]

    图 3  含有平移效果的全息板和对应的全息像[44]

    Figure 3.  Illustration of the meta-hologram with controlled shifting along the z-axis[44]

    图 4  偏振和频率复用全息板的单元结构与仿真出射波强度分布[45]

    Figure 4.  Illustration of the four basic functional subpixels and their simulated electric field responses[45]

    图 5  全息板在不同偏振入射和不同频率的情况下成像[45]

    Figure 5.  Schematic illustration of the polarization and frequency selective meta-hologram's functionality[45]

    图 6  反射式手性圆偏振复用全息成像[41]

    Figure 6.  Reflective chiral meta-holography[41]

    图 7  表面波全息板设计与点全息像呈现[46]

    Figure 7.  Surface plasmon hologram designing scheme and holographic results of an exemplary single-point profile[46]

    图 8  圆偏振光表面波全息成像[46]

    Figure 8.  Spin-switchable surface plasmon holography[46]

    图 9  线偏振光表面波全息成像[46]

    Figure 9.  Linear polarization switchable surface plasmon holography[46]

    图 10  温度主动可控全息板的单元结构及其透射响应[47]

    Figure 10.  Schematic of the metasurface unit cells and their transmission responses[47]

    图 11  主动可控全息板设计[47]

    Figure 11.  Design mechanism of the proposed thermal dynamic meta-hologram[47]

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收稿日期:  2019-11-05
修回日期:  2020-01-09
刊出日期:  2020-05-01

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