Acta Optica Sinica (Online), Volume. 2, Issue 7, 0709001(2025)
Configurable Optical Dirac Cavity Based on Topological Metasurfaces (Invited)
Fig. 1. Fundamental energy band pattern and mass term distribution of unit cell. (a) Geometries of trivial photonic crystal (left side of the solid line) and topological photonic crystal (right side of the solid line),
Fig. 2. Design and intrinsic mode distribution of optical Dirac cavity. (a) Drawing of designed configurable Dirac cavity, the mass term varies radially from inside to outside with the cavity center as a circle center and it is modulated by performing δ, the unperturbed cells are represented by yellow hexagons, the cells with the largest expansion are represented by red hexagons, and the outermost gray region is the air layer; (b)(c) band structure of topological unit cell at δ=0.053 and magnetic field (Hz) at Γ point carried by
Fig. 3. Distribution of energy bands and eigenmodes of constructed optical Dirac cavity for some unit cells. (a)(b) Energy band of topological unit cell B and magnetic field (Hz) at Γ point carried by px(py) and dxy(
Fig. 4. Eigenmodes of optical Dirac cavities with complex mass term distributions. (a)(b) Mass term function of
Fig. 5. Modal distributions of Dirac optical cavities, ①‒④ are four different forms of mass term distributions discussed in this paper. Column A is diagrams of cavity structure with spatial variations of mass terms, indicated by color changes of the mass terms, with the introduction of cavities and disorder and marked by black circles in the diagram; column B is the defective optical cavity after inversion of mass terms of counterpart column A. Defectiveness A and defectiveness B are electric field ∣E∣ distributions of far-field eigenmodes of defective optical cavities shown in A and B, respectively; modal distributions of perfect optical cavities after removal of the defects are given by the columns of without defect A and without defect B. (a)‒(f) Mass term distribution ①; (g)‒(l) mass term changes in step as shown in ②; (m)‒(o) mass term satisfies
Fig. 6. Coupling of optical cavities to spin-polarized boundary states.(a)(c)(e) General design of Dirac cavity with domain wall, and spin orientation and location of excitation source [(a) right circular polarization on the left side, (c) left circular polarization on the right side, and (e) left circular polarization on the left side]; (b)(d)(f) selectively oriented excitation of cavity mode corresponding to the system on the left
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Huiying Liang, Jiahao Hou, Tianyue Li, Shuming Wang. Configurable Optical Dirac Cavity Based on Topological Metasurfaces (Invited)[J]. Acta Optica Sinica (Online), 2025, 2(7): 0709001
Category: Micro-Nano Optics
Received: Dec. 23, 2024
Accepted: Feb. 14, 2025
Published Online: Apr. 10, 2025
The Author Email: Tianyue Li (leos4a@163.com), Shuming Wang (wangshuming@nju.edu.cn)
CSTR:32394.14.AOSOL240475