4.8 Article

Photonic Higher-Order Topological Insulator with Enlarged Non-Trivial Bandgaps

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LASER & PHOTONICS REVIEWS
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WILEY-V C H VERLAG GMBH
DOI: 10.1002/lpor.202300384

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bulk-boundary correspondence; higher-order hinge states; higher-order topological insulator; non-trivial bandgaps; photonic crystals

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This paper proposes a photonic higher-order topological insulator with a simple multilayer structure. By inserting a metallic pillar, the three-dimensional bandgap is extended, allowing for distinguishable topological modes. The lattice is reconfigurable, and introducing geometrical defects supports vertical disclination states.
The emergence of higher-order topological insulators (HOTIs) has greatly expanded the family of topological materials. While the co-dimensional bulk-boundary correspondence is observed in platforms, such as acoustics and photonics, realizing three-dimensional (3D) photonic HOTIs is relatively challenging due to the complex properties of electromagnetic waves such as polarizations, scattering, and refractive index. In this paper, a photonic HOTI with a simple multilayer structure that supports higher-order hinge states is proposed. By inserting a central metallic pillar in the unit cell, the 3D bandgap can be well extended, enabling pure and distinguishable surface and hinge modes. The lattice is reconfigurable and flexible, allowing for hinge and surface waves to be generated by controlling the geometrical length of sub-lattices. The idea of distinguished higher-order hinge modes is also extended to enlarged higher-orbital bandgaps. Furthermore, by introducing a central disclination in this photonic model, the one-dimensional (1D) vertical disclination mode is obtained which is not seen in existing photonic HOTIs. The findings open the door for a high-performance topological optical apparatus that features efficient one-way light propagation and energy concentration. A photonic higher-order topological insulator with a piling framework hosting hinge states is proposed. By inserting a metallic pillar in the lattice, the three-dimensional bandgap is extended, enabling distinguishable topological modes at lower- and higher-orbital bandgaps. Also, the introduction of geometrical defects makes this reconfigurable architecture supporting vertical disclination state, allowing for multimode waves to be generated at varying dimensions.image

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