Abstract

Liquid crystal (LC) cells that are coated with metamaterials are fabricated in this work. The LC directors in the cells are aligned by rubbed polyimide layers, and make angles θ of 0°, 45°, and 90° with respect to the gaps of the split-ring resonators (SRRs) of the metamaterials. Experimental results display that the resonance frequencies of the metamaterials in these cells increase with an increase in θ, and the cells have a maximum frequency shifting region of 18 GHz. Simulated results reveal that the increase in the resonance frequencies arises from the birefringence of the LC, and the LC has a birefringence of 0.15 in the terahertz region. The resonance frequencies of the metamaterials are shifted by the rubbing directions of the polyimide layers, so the LC cells coated with the metamaterials are passively tunable terahertz filters. The passively tunable terahertz filters exhibit promising applications on terahertz communication, terahertz sensing, and terahertz imaging.

Highlights

  • Metamaterials have attracted much attention due to their unusual electromagnetic resonance [1,2,3,4,5,6,7]

  • This work fabricated the metamaterial-coated Liquid crystal (LC) cells with the LC directors that make the angles of 0◦, 45◦, and 90◦ with respect to the gaps of the SRRs of the metamaterials

  • They are used to study the effect of the rubbing directions of the PI layers of the cells on the electromagnetic resonance of the metamaterials

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Summary

Introduction

Metamaterials have attracted much attention due to their unusual electromagnetic resonance [1,2,3,4,5,6,7]. Chen et al deposited a dual frequency LC layer on a terahertz metamaterial [6]. The dual frequency LC layer that is deposited on the terahertz metamaterial can be used to develop electrically controllable terahertz filters. The resonance frequency of the terahertz metamaterial is red-shifted by 11.4 (12.6) GHz at the irradiation of terahertz waves with TE (TM) polarization as a voltage that is applied to the LC layer increases from zero to 10 V.

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