Photonics Research, Volume. 11, Issue 7, 1154(2023)
Switchable chiral mirror based on PIN diodes
Fig. 1. (a) Conventional mirror (metallic plate) reverses the handedness of incident CP waves. Here, we report switchable chiral mirrors that transform upon regulating voltage into (b) a handedness-preserving mirror, (c) a perfect absorber, and (d) an LCP/(e) an RCP mirror. Handedness-preserving mirrors reflect both CP waves without handedness change. In addition, the LCP/RCP mirror reflects the LCP/RCP wave without handedness reversal while absorbing the other CP waves. Moreover, the perfect absorber absorbs both LCP and RCP waves.
Fig. 2. Schematic diagram of the unit cell of the switchable chiral mirror. (a) The perspective view and (b) the front view of the structure. (c) PIN diode equivalent circuit. (d) View of the Via design. Vias I and II have no contact with the intermediate metal layer, and Via III is connected to the middle metal layer. (e) The front view of the middle metallic layer. (f) The bottom feeder design. The two thin metal wires are connected to separate electrodes, respectively.
Fig. 3. Simulated (a) absorption spectra, (b) reflection amplitudes (
Fig. 4. The surface current distributions of the switchable chiral mirror at the handedness preserving mirror state under the normal incidence of (a) LCP and (b) RCP waves at 13 GHz, respectively. The surface current distributions of the switchable chiral mirror at the absorber state under the normal incidence of (c) LCP and (d) RCP waves at 13 GHz, respectively. The surface current distributions of the switchable chiral mirror at the RCP mirror state under the normal incidence of (e) LCP and (f) RCP waves at 13 GHz, respectively. The surface current distributions of the switchable chiral mirror at the LCP mirror state under the normal incidence of (g) LCP and (h) RCP waves at 13 GHz, respectively. Arrows indicate electric dipoles corresponding to resonant currents excited by the CP waves of opposite handedness.
Fig. 5. The energy loss distributions on the structure surface at the handedness preserving mirror state under the normal incidence of (a) LCP and (b) RCP waves at 13 GHz, respectively. The energy loss distributions on the structure surface at the absorber state under the normal incidence of (c) LCP and (d) RCP waves at 13 GHz, respectively. The energy loss distributions on the structure surface at the RCP mirror state under the normal incidence of (e) LCP and (f) RCP waves at 13 GHz, respectively. The energy loss distributions on the structure surface at the LCP mirror state under the normal incidence of (g) LCP and (h) RCP waves at 13 GHz, respectively.
Fig. 6. Measured (a) absorption spectra, (b) reflection amplitudes, and (c) CD spectra of the handedness preserving mirror state at normal incidence. Measured (d) absorption spectra, (e) reflection amplitudes, and (f) CD spectra of the perfect absorber state at normal incidence. Measured (g) absorption spectra, (h) reflection amplitudes, and (i) CD spectra of the RCP mirror state at normal incidence. Measured (j) absorption spectra, (k) reflection amplitudes, and (l) CD spectra of the LCP mirror state at normal incidence.
Fig. 7. Photograph of the switchable chiral mirror prototype. (a) The measurement system, (b) the front view, and (c) the back view. All Vias I in a row are connected in a series on the backside of the dielectric substrate and connected to the top metal patch (not connected to the bottom metal patch). Feeder I provides voltage
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Zhibiao Zhu, Zhe Qin, He Wang, Lixin Jiang, Yongfeng Li, Wenjie Wang, Hongya Chen, Jiafu Wang, Yongqiang Pang, Shaobo Qu, "Switchable chiral mirror based on PIN diodes," Photonics Res. 11, 1154 (2023)
Category: Surface Optics and Plasmonics
Received: Jun. 21, 2022
Accepted: Jul. 31, 2022
Published Online: Jun. 16, 2023
The Author Email: Yongfeng Li (liyf217130@126.com)