• Advanced Photonics
  • Vol. 4, Issue 1, 016002 (2022)
Quan Xu1, Xiaoqiang Su2、*, Xueqian Zhang1, Lijuan Dong2, Lifeng Liu2, Yunlong Shi2, Qiu Wang3, Ming Kang4, Andrea Alù5、6, Shuang Zhang7、8、*, Jiaguang Han1、9、*, and Weili Zhang10、*
Author Affiliations
  • 1Tianjin University, Center for Terahertz Waves and College of Precision Instrument and Optoelectronics Engineering, Key Laboratory of Optoelectronic Information Technology (Ministry of Education of China), Tianjin, China
  • 2Shanxi Datong University, Institute of Solid State Physics and College of Physics and Electronic Science, Shanxi Province Key Laboratory of Microstructure Electromagnetic Functional Materials, Datong, China
  • 3Wuhan University of Technology, School of Information Engineering, Wuhan, China
  • 4Tianjin Normal University, College of Physics and Materials Science, Tianjin, China
  • 5City University of New York, Advanced Science Research Center, Photonics Initiative, New York, United States
  • 6City University of New York, Graduate Center, Physics Program, New York, United States
  • 7University of Hong Kong, Faculty of Science, Department of Physics, Hong Kong, China
  • 8University of Hong Kong, Department of Electrical and Electronic Engineering, Hong Kong, China
  • 9Guilin University of Electronic Technology, Guangxi Key Laboratory of Optoelectronic Information Processing, School of Optoelectronic Engineering, Guilin, China
  • 10Oklahoma State University, School of Electrical and Computer Engineering, Stillwater, Oklahoma, United States
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    DOI: 10.1117/1.AP.4.1.016002 Cite this Article Set citation alerts
    Quan Xu, Xiaoqiang Su, Xueqian Zhang, Lijuan Dong, Lifeng Liu, Yunlong Shi, Qiu Wang, Ming Kang, Andrea Alù, Shuang Zhang, Jiaguang Han, Weili Zhang. Mechanically reprogrammable Pancharatnam–Berry metasurface for microwaves[J]. Advanced Photonics, 2022, 4(1): 016002 Copy Citation Text show less
    Schematics of the metasurface and its supercell. (a) The metasurface is formed by an array of supercells, arranged in a square lattice with a period of 43.5 mm. The PB phase response of each supercell is controlled by an addressable wireless signal and can be independently tuned over 28 phase levels. The metasurface can be reprogrammed to realize custom functionalities including metalensing, focused vortex beam generation, and holographic imaging by a proper design of the PB phase distribution. (b) The PB phase control in each supercell is achieved by transmitting the torque from a stepping motor to the PB meta-atoms through a set of gears.
    Fig. 1. Schematics of the metasurface and its supercell. (a) The metasurface is formed by an array of supercells, arranged in a square lattice with a period of 43.5 mm. The PB phase response of each supercell is controlled by an addressable wireless signal and can be independently tuned over 28 phase levels. The metasurface can be reprogrammed to realize custom functionalities including metalensing, focused vortex beam generation, and holographic imaging by a proper design of the PB phase distribution. (b) The PB phase control in each supercell is achieved by transmitting the torque from a stepping motor to the PB meta-atoms through a set of gears.
    PB phase response. (a) The top portion of the PB meta-atom is a pair of Archimedean spirals with the same geometric parameters: inner radius (1.9 mm), outer radius (4.3 mm), height (0.035 mm), width (0.4 mm), and number of turns (two turns). The pink and sky-blue dials schematically depict the PB phase control resolution and variation gradients for Rrr and Rll, respectively. (b), (c) Measured amplitudes of Rrr and Rll, respectively. (d), (e) Measured PB phase response of Rrr and Rll, respectively, versus different rotation angles.
    Fig. 2. PB phase response. (a) The top portion of the PB meta-atom is a pair of Archimedean spirals with the same geometric parameters: inner radius (1.9 mm), outer radius (4.3 mm), height (0.035 mm), width (0.4 mm), and number of turns (two turns). The pink and sky-blue dials schematically depict the PB phase control resolution and variation gradients for Rrr and Rll, respectively. (b), (c) Measured amplitudes of Rrr and Rll, respectively. (d), (e) Measured PB phase response of Rrr and Rll, respectively, versus different rotation angles.
    Realization of metalensing. (a), (d), (g) Required rotation profiles to realize different metalens operations for RCP waves. (b), (e), (h) Measured electric field intensities (|Rrr|2) at 7 GHz on the focal plane. (c), (f), (i) Horizontal cuts of the metalens focal spots, with FWHMs = 42, 44, and 44 mm, respectively.
    Fig. 3. Realization of metalensing. (a), (d), (g) Required rotation profiles to realize different metalens operations for RCP waves. (b), (e), (h) Measured electric field intensities (|Rrr|2) at 7 GHz on the focal plane. (c), (f), (i) Horizontal cuts of the metalens focal spots, with FWHMs = 42, 44, and 44 mm, respectively.
    Focused vortex beam generation. (a), (e), (i), (m) Required rotation profiles to generate focused vortex beams with the topological charges of l=1, 2, 3, 4, respectively. (b), (f), (j), (n) Measured electric intensity (|Rrr|2) distributions and (c), (g), (k), (o) measured phase (∠Rrr) distributions of different vortex beams, respectively, obtained at the focal plane. (d), (h), (l), (p) OAM amplitude |Sn| extracted from the measured complex amplitudes of different vortex beams, respectively.
    Fig. 4. Focused vortex beam generation. (a), (e), (i), (m) Required rotation profiles to generate focused vortex beams with the topological charges of l=1,  2,  3,  4, respectively. (b), (f), (j), (n) Measured electric intensity (|Rrr|2) distributions and (c), (g), (k), (o) measured phase (Rrr) distributions of different vortex beams, respectively, obtained at the focal plane. (d), (h), (l), (p) OAM amplitude |Sn| extracted from the measured complex amplitudes of different vortex beams, respectively.
    Holographic imaging. (a)–(d), (i)–(l) Required rotation profiles to generate holographic images of Chinese characters “天津大学” (Tianjin University) and “大同云冈” (Datong Yungang), respectively. (e)–(h), (m)–(p) Corresponding measured electric field intensities (|Rrr|2) of holographic images obtained at z=600 mm.
    Fig. 5. Holographic imaging. (a)–(d), (i)–(l) Required rotation profiles to generate holographic images of Chinese characters “天津大学” (Tianjin University) and “大同云冈” (Datong Yungang), respectively. (e)–(h), (m)–(p) Corresponding measured electric field intensities (|Rrr|2) of holographic images obtained at z=600  mm.
    Quan Xu, Xiaoqiang Su, Xueqian Zhang, Lijuan Dong, Lifeng Liu, Yunlong Shi, Qiu Wang, Ming Kang, Andrea Alù, Shuang Zhang, Jiaguang Han, Weili Zhang. Mechanically reprogrammable Pancharatnam–Berry metasurface for microwaves[J]. Advanced Photonics, 2022, 4(1): 016002
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