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,...
Main Authors: | , , , , , |
---|---|
Format: | Article |
Language: | English |
Published: |
MDPI AG
2019-09-01
|
Series: | Crystals |
Subjects: | |
Online Access: | https://www.mdpi.com/2073-4352/9/10/502 |
_version_ | 1798005128555397120 |
---|---|
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. |
first_indexed | 2024-04-11T12:34:17Z |
format | Article |
id | doaj.art-3cee1f59f4314945abe4d5358d91d2f0 |
institution | Directory Open Access Journal |
issn | 2073-4352 |
language | English |
last_indexed | 2024-04-11T12:34:17Z |
publishDate | 2019-09-01 |
publisher | MDPI AG |
record_format | Article |
series | Crystals |
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 |
work_keys_str_mv | AT natalyavrudakova chiralopticaltammstatesattheinterfacebetweenanalldielectricpolarizationpreservinganisotropicmirrorandacholestericliquidcrystal AT ivanvtimofeev chiralopticaltammstatesattheinterfacebetweenanalldielectricpolarizationpreservinganisotropicmirrorandacholestericliquidcrystal AT rashidgbikbaev chiralopticaltammstatesattheinterfacebetweenanalldielectricpolarizationpreservinganisotropicmirrorandacholestericliquidcrystal AT maximvpyatnov chiralopticaltammstatesattheinterfacebetweenanalldielectricpolarizationpreservinganisotropicmirrorandacholestericliquidcrystal AT stepanyavetrov chiralopticaltammstatesattheinterfacebetweenanalldielectricpolarizationpreservinganisotropicmirrorandacholestericliquidcrystal AT weilee chiralopticaltammstatesattheinterfacebetweenanalldielectricpolarizationpreservinganisotropicmirrorandacholestericliquidcrystal |