Abstract

The modes formed by two coupled chiral optical Tamm states localized at the interfaces between a photonic cholesteric liquid crystal conjugated with polarization-preserving anisotropic mirrors have been analytically and numerically investigated. These modes are only excited at the diffracting polarization of incident light. As the cholesteric layer thickness decreases, the spectral splitting of the localized state frequency is predicted. The splitting value depends on the crystal layer thickness. At the nondiffracting circular polarization, the localized modes are not excited, and the system becomes similar to the Fabry–Pérot cavity containing an anisotropic helical structure.

Highlights

  • The optical Tamm state (OTS) attracts the attention of researches among various surface localized optical states

  • Cholesteric liquid crystals (CLCs) thicknesses, the transmittance peak corresponding to the OTS was observed for this polarization

  • Since the light fell from the left and the CLC had a high reflectivity, the field was localized stronger on the left CLC boundary

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Summary

Introduction

The optical Tamm state (OTS) attracts the attention of researches among various surface localized optical states. The field decay inside the photonic crystal is caused by the Bragg reflection condition Such a localized mode at the interface between two materials can be excited by both TE and TM linear polarizations at any light incidence angle. In contrast to scalar photonic-crystal materials or distributed Bragg reflectors, CLCs have only band gap at the normal incidence of light. This band gap only exists for light with the diffracting circular polarization coinciding with the twisting of a cholesteric helix. Obtaining a Tamm plasmon localized between the CLC and metallic layer or the OTS localized between the CLC and distributed Bragg reflector is a challenging problem We examine the coupling between two chiral OTSs localized at both CLC boundaries

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