Plasmonic‐Enhanced Polymer‐Stabilized Liquid Crystals Switching for Integrated Optical Attenuation

Author:

Jian Jialing123ORCID,Liu Ruizhe4,Ye Yuting23,Wu Jianghong23,Deng Qingyan23,Wei Maoliang4,Tang Yiheng23,Tang Renjie23,Sun Boshu23,Ma Hui4,Shi Yilin23,Zhong Chuyu4,Sun Chunlei23,Lin Hongtao4,Li Ming5,Li Lan236ORCID

Affiliation:

1. Zhejiang University Hangzhou 310027 China

2. Key Laboratory of 3D Micro/Nano Fabrication and Characterization of Zhejiang Province School of Engineering Westlake University Hangzhou 310030 China

3. Institute of Advanced Technology Westlake Institute for Advanced Study 18 Shilongshan Road Hangzhou 310024 China

4. State Key Laboratory of Brain‐Machine Intelligence College of Information Science and Electronic Engineering Zhejiang University Hangzhou 310027 China

5. State Key Laboratory on Integrated Optoelectronics Institute of Semiconductors Chinese Academy of Sciences Beijing 100083 China

6. Westlake Institute for Optoelectronics Hangzhou 311421 China

Abstract

AbstractLiquid crystals are widely used in photonics because of their profound electro–optic properties. However, the slow switching speeds (milliseconds) and the fluid nature of liquid crystals restrict their potential use in integrated photonics. In this work, polymer‐stabilized liquid crystals are utilized as the functional material to improve the response time with a polymer network that helps pre‐orientate the liquid crystal. Additionally, plasmonic slot structures are simultaneously employed to minimize the switch voltage by confining the optical field within the electrode spacing at subwavelength scales. Thanks to the large overlap of the optical and electric fields, the scattering states of the polymer‐stabilized liquid crystal can be effectively manipulated to modulate the loss of the propagating wave, resulting in strong optical attenuation in the integrated photonic platform. Specifically, a plasmonic enhanced polymer‐stabilized liquid crystal photonic device for operation at 1550 nm, which has a length of only 10 µm and shows an extinction ratio of 0.38 dB µm−1, with a power consumption of less than 6 µW and a response time ≈20 µs, resulting in a figure‐of‐merit of 0.012 mW.

Funder

National Natural Science Foundation of China

Westlake University

Publisher

Wiley

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