• Photonics Research
  • Vol. 11, Issue 2, 203 (2023)
Ruichao Zhu1, Jiafu Wang1、4、*, Yajuan Han1, Yuxiang Jia1, Tonghao Liu1, Tianshuo Qiu1, Sai Sui1, Yongfeng Li1, Mingbao Yan1, Shaobo Qu1, and Cheng-Wei Qiu2、3、5、*
Author Affiliations
  • 1Shaanxi Key Laboratory of Artificially-Structured Functional Materials and Devices, Air Force Engineering University, Xi’an 710051, China
  • 2Department of Electrical and Computer Engineering, National University of Singapore, Singapore 117583, Singapore
  • 3NUS Suzhou Research Institute (NUSRI), Suzhou 215000, China
  • 4e-mail: wangjiafu1981@126.com
  • 5e-mail: chengwei.qiu@nus.edu.sg
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    DOI: 10.1364/PRJ.475471 Cite this Article Set citation alerts
    Ruichao Zhu, Jiafu Wang, Yajuan Han, Yuxiang Jia, Tonghao Liu, Tianshuo Qiu, Sai Sui, Yongfeng Li, Mingbao Yan, Shaobo Qu, Cheng-Wei Qiu. Virtual metasurfaces: reshaping electromagnetic waves in distance[J]. Photonics Research, 2023, 11(2): 203 Copy Citation Text show less
    Schematic diagram of the virtual metasurface compared with the conventional one.
    Fig. 1. Schematic diagram of the virtual metasurface compared with the conventional one.
    Structure and network design: (a) geometrical parameter of unit in front view and side view; (b) phase response when the length changes from 0.9 to 3.7 mm, and the step length is 0.4 mm; (c) phase response after rotating the unit 90 deg; (d) amplitude of cross-polarized wave when the length changes from 0.9 to 3.7 mm, and the step length is 0.4 mm; (e) amplitude response after rotating the unit 90 deg.
    Fig. 2. Structure and network design: (a) geometrical parameter of unit in front view and side view; (b) phase response when the length changes from 0.9 to 3.7 mm, and the step length is 0.4 mm; (c) phase response after rotating the unit 90 deg; (d) amplitude of cross-polarized wave when the length changes from 0.9 to 3.7 mm, and the step length is 0.4 mm; (e) amplitude response after rotating the unit 90 deg.
    Design of focusing metasurfaces and generation of virtual meta-atoms: (a), (b) two phase profiles of metasurface with a 180 deg phase difference; (c), (d) generated focusing metasurfaces filled according to the phase profiles in (a) and (b); (e), (h) distributions of electric fields Ex on the XOZ plane; (f), (i) electric field intensity distribution on the XOY plane when Z=30 mm; (g), (j) phase distribution on the XOY plane when Z=30 mm.
    Fig. 3. Design of focusing metasurfaces and generation of virtual meta-atoms: (a), (b) two phase profiles of metasurface with a 180 deg phase difference; (c), (d) generated focusing metasurfaces filled according to the phase profiles in (a) and (b); (e), (h) distributions of electric fields Ex on the XOZ plane; (f), (i) electric field intensity distribution on the XOY plane when Z=30  mm; (g), (j) phase distribution on the XOY plane when Z=30  mm.
    Virtual metasurface design and verification: (a) focusing metasurfaces are spliced together according to the chessboard arrangement; (b) the intensity distribution of Ex on the focusing plane in chessboard arrangement; (c) the phase distribution of Ex on the focusing plane in chessboard arrangement; (d) the 3D far-field scattering beam of metasurface in chessboard arrangement.
    Fig. 4. Virtual metasurface design and verification: (a) focusing metasurfaces are spliced together according to the chessboard arrangement; (b) the intensity distribution of Ex on the focusing plane in chessboard arrangement; (c) the phase distribution of Ex on the focusing plane in chessboard arrangement; (d) the 3D far-field scattering beam of metasurface in chessboard arrangement.
    Verification that the far-field scattering modulation is realized by the VM rather than the entity metasurface: (a) virtual metasurface is aligned with the obstacle (a metal plate with spaced apertures); (b) the phase profile of entity metasurface; (c) the intensity distribution of Ex on the focusing plane in chessboard arrangement with the obstacle; (d) the phase distribution of Ex on the focusing plane in chessboard arrangement with the obstacle; (e) the 3D far-field scattering beam of metasurface in chessboard arrangement with the obstacle; (f) the 3D far-field scattering beam of entity metasurface; (g) the 3D far-field scattering beam of entity metasurface with obstacle.
    Fig. 5. Verification that the far-field scattering modulation is realized by the VM rather than the entity metasurface: (a) virtual metasurface is aligned with the obstacle (a metal plate with spaced apertures); (b) the phase profile of entity metasurface; (c) the intensity distribution of Ex on the focusing plane in chessboard arrangement with the obstacle; (d) the phase distribution of Ex on the focusing plane in chessboard arrangement with the obstacle; (e) the 3D far-field scattering beam of metasurface in chessboard arrangement with the obstacle; (f) the 3D far-field scattering beam of entity metasurface; (g) the 3D far-field scattering beam of entity metasurface with obstacle.
    Sample fabrication and performance verification: (a) the photographs of TFMTs; (b) the photographs of spliced TFMTs according to checkerboard configuration and the samples with obstacle; (c) near-field measurement environment; (d) far-field measurement environment; (e), (f) the electric field distributions in XOZ cross sections of the 0 and 1 focusing metasurfaces; (g) the electric field distributions in XOY cross sections of the virtual metasurface with checkerboard configuration; (h) the measured far-field radiation patterns under the chessboard arrangement when φ=45° and φ=−45° on orthogonal diagonal lines; (i) the measured far-field radiation patterns under the chessboard arrangement with obstacle when φ=45° and φ=−45° on orthogonal diagonal lines.
    Fig. 6. Sample fabrication and performance verification: (a) the photographs of TFMTs; (b) the photographs of spliced TFMTs according to checkerboard configuration and the samples with obstacle; (c) near-field measurement environment; (d) far-field measurement environment; (e), (f) the electric field distributions in XOZ cross sections of the 0 and 1 focusing metasurfaces; (g) the electric field distributions in XOY cross sections of the virtual metasurface with checkerboard configuration; (h) the measured far-field radiation patterns under the chessboard arrangement when φ=45° and φ=45° on orthogonal diagonal lines; (i) the measured far-field radiation patterns under the chessboard arrangement with obstacle when φ=45° and φ=45° on orthogonal diagonal lines.
    Fitting performance of neural network.
    Fig. 7. Fitting performance of neural network.
    Theoretical formation path of focus and more aperture sizes: (a) theoretical formation path of focus; (b) 3D far-field result with obstacle when HR=20 mm and Rhole=19 mm; (c) 3D far-field result with obstacle when HR=25 mm and Rhole=16 mm; (d) 3D far-field result with obstacle when HR=30 mm and Rhole=13 mm.
    Fig. 8. Theoretical formation path of focus and more aperture sizes: (a) theoretical formation path of focus; (b) 3D far-field result with obstacle when HR=20  mm and Rhole=19  mm; (c) 3D far-field result with obstacle when HR=25  mm and Rhole=16  mm; (d) 3D far-field result with obstacle when HR=30  mm and Rhole=13  mm.
    Cross profile comparison between the existence of obstacles and the absence of obstacles: (a) comparison of entity metasurface; (b) comparison of VM.
    Fig. 9. Cross profile comparison between the existence of obstacles and the absence of obstacles: (a) comparison of entity metasurface; (b) comparison of VM.
    Ruichao Zhu, Jiafu Wang, Yajuan Han, Yuxiang Jia, Tonghao Liu, Tianshuo Qiu, Sai Sui, Yongfeng Li, Mingbao Yan, Shaobo Qu, Cheng-Wei Qiu. Virtual metasurfaces: reshaping electromagnetic waves in distance[J]. Photonics Research, 2023, 11(2): 203
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