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Straight Photonic Nodal Lines with Quadrupole Berry Curvature Distribution and Superimaging “Fermi Arcs”

Dongyang Wang, Biao Yang, Ruo-Yang Zhang, Wen-Jie Chen, Z. Q. Zhang, Shuang Zhang, and C. T. Chan
Phys. Rev. Lett. 129, 043602 – Published 22 July 2022
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Abstract

In periodic systems, nodal lines are loops in the three-dimensional momentum space with each point on them representing a band degeneracy. Nodal lines exhibit rich topological features, as they can take various configurations such as rings, links, chains, and knots. These line nodes are generally protected by mirror or PT symmetry and frequently accompanied by drumhead surface states. Here, we propose and demonstrate a novel type of photonic straight nodal lines in a D2D metacrystal, which are protected by an unusual rotoinversion time (roto-PT) symmetry. These nodal lines are located at the central axis and hinges of the Brillouin zone. They appear as quadrupole sources of Berry curvature flux in contrast to the Weyl points, which are monopoles. Interestingly, topological surface states exist at all three cutting surfaces, as guaranteed by π-quantized Zak phases along all three directions. As frequency changes, the surface state equifrequency contours evolve from closed to open and become straight lines at a critical transition frequency, at which diffractionless surface wave propagations are experimentally demonstrated, paving the way toward development of superimaging topological devices.

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  • Received 18 February 2022
  • Accepted 6 July 2022

DOI:https://doi.org/10.1103/PhysRevLett.129.043602

© 2022 American Physical Society

Physics Subject Headings (PhySH)

Atomic, Molecular & OpticalCondensed Matter, Materials & Applied Physics

Authors & Affiliations

Dongyang Wang1, Biao Yang1,2, Ruo-Yang Zhang1, Wen-Jie Chen3, Z. Q. Zhang1, Shuang Zhang4,5,*, and C. T. Chan1,†

  • 1Department of Physics, Hong Kong University of Science and Technology, Hong Kong, China
  • 2College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
  • 3School of Physics and State Key Laboratory of Optoelectronic Materials and Technologies, Sun Yat-Sen University; Guangzhou 510275, China
  • 4Department of Physics, The University of Hong Kong; Hong Kong, China
  • 5Department of Electrical and Electronic Engineering, The University of Hong Kong, Hong Kong, China

  • *Corresponding author. shuzhang@hku.hk
  • Corresponding author. phchan@ust.hk

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Issue

Vol. 129, Iss. 4 — 22 July 2022

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Images

  • Figure 1
    Figure 1

    Quadratic straight nodal lines protected by roto-PT symmetry. (a) Schematic of the metacrystal unit. Periodicities along x/y/z directions are a=b=4mm and c=3mm. The sizes of the resonator are L1=L2=3mm, Lc=3.5mm (cross bar), and Lz=1.5mm. In PCB fabrication, the metallic resonator is implemented with copper, and the supporting substrate is made of F4B with ϵ2. (b) Band structure for the metacrystal; degenerate lines can be found along MA and ΓZ. The 3D band dispersion of nodal lines is shown as the inset. (c) Straight nodal lines in the BZ with a 0/2π encircling Berry phase. (d) Quadratic dispersions verified for the points marked in (b). They transform into linear by breaking S4z symmetry (L1=2.8mm, L2=3mm). (e) The Zak phases along kx, ky, and kz directions are found as π at the indicated positions.

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  • Figure 2
    Figure 2

    Quadrupoles of Berry curvature. (a) The quadrupole in-plane Berry curvature for the second band at kz=0.5π/c; green arrows represent the directions. (b) Distribution of Zak phase ϕz for a quadrant of the BZ [indicated with a box in (a)], which varies along the indicated arrows. (c) The winding of the Zak phase in (b) implies the in-plane Berry curvature flux. (d) The Zak phase winding indicates the quadrupolar shape of Ω, and the winding range reflects the strength.

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  • Figure 3
    Figure 3

    Characterizing the straight nodal lines on the (001) surface. (a) Schematic of a metacrystal with a truncated surface on the xy plane. (b) Surface BZ for the (001) surface with the straight nodal lines’ projection. (c) The calculated kz-projected band dispersions and experimental measurements with a PEC boundary. (d) Calculated and experimentally measured projected bands along Γ¯M¯; surface modes are indicated with red color. (e) Measured EFCs of surface modes on the top surface.

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  • Figure 4
    Figure 4

    Superimaging with topological Fermi arcs. (a) Schematic of the metacrystal orientation for surface Fermi-arc propagation measurement. (b) Measured Ez field pattern with corner source excitation, and the surface waves are collimated and directed toward the y direction. (c) The experimentally retrieved flat EFCs of the surface wave at f=15.9GHz. (d) Configuration for superimaging demonstration. (e),(f) Measured real part and amplitude of the surface wave at f=15.9GHz.

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