Chiral Optical Tamm States at the Interface between an All-Dielectric Polarization-Preserving Anisotropic Mirror and a Cholesteric Liquid Crystal

As a new localized state of light, the chiral optical Tamm state exists at the interface between a polarization-retaining anisotropic mirror and a substance with optical activity. Considering a hybrid structure comprising a metal-free polarization-preserving mirror and a cholesteric liquid crystal,...

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Main Authors: Natalya V. Rudakova, Ivan V. Timofeev, Rashid G. Bikbaev, Maxim V. Pyatnov, Stepan Ya. Vetrov, Wei Lee
Format: Article
Language:English
Published: MDPI AG 2019-09-01
Series:Crystals
Subjects:
Online Access:https://www.mdpi.com/2073-4352/9/10/502
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author Natalya V. Rudakova
Ivan V. Timofeev
Rashid G. Bikbaev
Maxim V. Pyatnov
Stepan Ya. Vetrov
Wei Lee
author_facet Natalya V. Rudakova
Ivan V. Timofeev
Rashid G. Bikbaev
Maxim V. Pyatnov
Stepan Ya. Vetrov
Wei Lee
author_sort Natalya V. Rudakova
collection DOAJ
description As a new localized state of light, the chiral optical Tamm state exists at the interface between a polarization-retaining anisotropic mirror and a substance with optical activity. Considering a hybrid structure comprising a metal-free polarization-preserving mirror and a cholesteric liquid crystal, we highlight the high Q factor arising from the all-dielectric framework. The intensity of localized light decreases exponentially with increasing distance from the interface. The penetration of the field into the cholesteric liquid crystal is essentially prohibited for wavelengths lying in the photonic bandgap and close to the cholesteric pitch length. The dielectric mirror has its own photonic bandgap. The energy transfer along the interface can be effectively switched off by setting the tangential wave vector to zero. The spectral behavior of the chiral optical Tamm state is observed both as reflection and transmission resonance. This Fano resonance is analogous to the Kopp−Genack effect. Our analytics are well in line with precise calculations, which may pave a new route for the future development of intelligent design for laser and sensing applications.
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spelling doaj.art-3cee1f59f4314945abe4d5358d91d2f02022-12-22T04:23:40ZengMDPI AGCrystals2073-43522019-09-0191050210.3390/cryst9100502cryst9100502Chiral Optical Tamm States at the Interface between an All-Dielectric Polarization-Preserving Anisotropic Mirror and a Cholesteric Liquid CrystalNatalya V. Rudakova0Ivan V. Timofeev1Rashid G. Bikbaev2Maxim V. Pyatnov3Stepan Ya. Vetrov4Wei Lee5Kirensky Institute of Physics, Federal Research Center KSC SB RAS, Krasnoyarsk 660036, RussiaKirensky Institute of Physics, Federal Research Center KSC SB RAS, Krasnoyarsk 660036, RussiaKirensky Institute of Physics, Federal Research Center KSC SB RAS, Krasnoyarsk 660036, RussiaKirensky Institute of Physics, Federal Research Center KSC SB RAS, Krasnoyarsk 660036, RussiaKirensky Institute of Physics, Federal Research Center KSC SB RAS, Krasnoyarsk 660036, RussiaInstitute of Imaging and Biomedical Photonics, College of Photonics, National Chiao Tung University, Tainan 71150, TaiwanAs a new localized state of light, the chiral optical Tamm state exists at the interface between a polarization-retaining anisotropic mirror and a substance with optical activity. Considering a hybrid structure comprising a metal-free polarization-preserving mirror and a cholesteric liquid crystal, we highlight the high Q factor arising from the all-dielectric framework. The intensity of localized light decreases exponentially with increasing distance from the interface. The penetration of the field into the cholesteric liquid crystal is essentially prohibited for wavelengths lying in the photonic bandgap and close to the cholesteric pitch length. The dielectric mirror has its own photonic bandgap. The energy transfer along the interface can be effectively switched off by setting the tangential wave vector to zero. The spectral behavior of the chiral optical Tamm state is observed both as reflection and transmission resonance. This Fano resonance is analogous to the Kopp−Genack effect. Our analytics are well in line with precise calculations, which may pave a new route for the future development of intelligent design for laser and sensing applications.https://www.mdpi.com/2073-4352/9/10/502optical tamm statecholesteric liquid crystalpolarization-preserving anisotropic mirror
spellingShingle Natalya V. Rudakova
Ivan V. Timofeev
Rashid G. Bikbaev
Maxim V. Pyatnov
Stepan Ya. Vetrov
Wei Lee
Chiral Optical Tamm States at the Interface between an All-Dielectric Polarization-Preserving Anisotropic Mirror and a Cholesteric Liquid Crystal
Crystals
optical tamm state
cholesteric liquid crystal
polarization-preserving anisotropic mirror
title Chiral Optical Tamm States at the Interface between an All-Dielectric Polarization-Preserving Anisotropic Mirror and a Cholesteric Liquid Crystal
title_full Chiral Optical Tamm States at the Interface between an All-Dielectric Polarization-Preserving Anisotropic Mirror and a Cholesteric Liquid Crystal
title_fullStr Chiral Optical Tamm States at the Interface between an All-Dielectric Polarization-Preserving Anisotropic Mirror and a Cholesteric Liquid Crystal
title_full_unstemmed Chiral Optical Tamm States at the Interface between an All-Dielectric Polarization-Preserving Anisotropic Mirror and a Cholesteric Liquid Crystal
title_short Chiral Optical Tamm States at the Interface between an All-Dielectric Polarization-Preserving Anisotropic Mirror and a Cholesteric Liquid Crystal
title_sort chiral optical tamm states at the interface between an all dielectric polarization preserving anisotropic mirror and a cholesteric liquid crystal
topic optical tamm state
cholesteric liquid crystal
polarization-preserving anisotropic mirror
url https://www.mdpi.com/2073-4352/9/10/502
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