• Photonics Research
  • Vol. 12, Issue 3, 534 (2024)
Yicheng Li1、2、3, Shicheng Wan1、2、3, Shaoxuan Deng1、2, Zhengwei Deng1、2, Bo Lv1、2, Chunying Guan1、2, Jun Yang2、4、6, Andrey Bogdanov3、5, Pavel Belov3, and Jinhui Shi1、2、*
Author Affiliations
  • 1Key Laboratory of Photonic Materials and Devices Physics for Oceanic Applications, Ministry of Industry and Information Technology, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin 150001, China
  • 2Key Laboratory of In-Fiber Integrated Optics of Ministry of Education, College of Physics and Optoelectronic Engineering, Harbin Engineering University, Harbin 150001, China
  • 3School of Physics and Engineering, ITMO University, St. Petersburg 197101, Russia
  • 4School of Information Engineering, Guangdong University of Technology, Guangzhou 510008, China
  • 5Qingdao Innovation and Development Center, Harbin Engineering University, Qingdao 266000, China
  • 6e-mail: yangj@gdut.edu.cn
  • show less
    DOI: 10.1364/PRJ.510300 Cite this Article Set citation alerts
    Yicheng Li, Shicheng Wan, Shaoxuan Deng, Zhengwei Deng, Bo Lv, Chunying Guan, Jun Yang, Andrey Bogdanov, Pavel Belov, Jinhui Shi. Independent control of circularly polarized light with exceptional topological phase coding metasurfaces[J]. Photonics Research, 2024, 12(3): 534 Copy Citation Text show less

    Abstract

    Exceptional points, as degenerate points of non-Hermitian parity-time symmetric systems, have many unique physical properties. Due to its flexible control of electromagnetic waves, a metasurface is frequently used in the field of nanophotonics. In this work, we developed a parity-time symmetric metasurface and implemented the 2π topological phase surrounding an exceptional point. Compared with Pancharatnam-Berry phase, the topological phase around an exceptional point can achieve independent regulation of several circular polarization beams. We combined the Pancharatnam-Berry phase with the exceptional topological phase and proposed a composite coding metasurface to achieve reflection decoupling of different circular polarizations. This work provides a design idea for polarimetric coding metasurfaces in the future.
    r^=(r++r+r+r),

    View in Article

    (δx+iγx+GxxGxyGyxδy+iγy+Gyy)(pxpy)=(gxEixgyEiy),(B1)

    View in Article

    (ErxEry)r^(EixEiy)=iωη02a2(pxpy)(EixEiy),(B2)

    View in Article

    (iΓGxyGxyiΓ)(pxpy)SI(pxpy)=(gxEixgyEiy),(B3)

    View in Article

    (ErxEry)=[A(gx2(δy+iγy+Gyy)gxgyGxygxgyGxygy2(δx+iγx+Gxx))I](EixE˜iy),(B4)

    View in Article

    A=iωη02a2[(δx+iγx+Gxx)(δy+iγy+Gyy)Gxy2].(B5)

    View in Article

    (ErxEry)=(1gxgyAS)I(EixEiy)+gxgyA(iΓGxyGxyiΓ)(EixE˜iy).(B6)

    View in Article

    r^θ(R)=(r++θ(R)r+θ(R)r+θ(R)rθ(R))=M(θ)r^(R)M(θ).(C1)

    View in Article

    r^θ(R)=12(rxx+ryy)I^+i2(rxyryx)σ3+12(rxxryy)(ei2θσ++ei2θσ)+i2(rxy+ryx)(ei2θσ++ei2θσ).(C2)

    View in Article

    r+θ(R)=(rxxryy)+i(rxy+ryx)2ei2θ=r+0(R)ei2θ,(C3)

    View in Article

    r+θ(R)=(rxxryy)i(rxy+ryx)2ei2θ=r+0(R)ei2θ;(C4)

    View in Article

    φ[r±θ(R)]=φ[r±0(R)]±2θ.(C5)

    View in Article

    Yicheng Li, Shicheng Wan, Shaoxuan Deng, Zhengwei Deng, Bo Lv, Chunying Guan, Jun Yang, Andrey Bogdanov, Pavel Belov, Jinhui Shi. Independent control of circularly polarized light with exceptional topological phase coding metasurfaces[J]. Photonics Research, 2024, 12(3): 534
    Download Citation