2016
DOI: 10.1134/s0021364016180119
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Chiral optical Tamm states at the boundary of the medium with helical symmetry of the dielectric tensor

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Cited by 25 publications
(30 citation statements)
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“…This expression is more exact in comparison with the earlier obtained approximation (Equation (10) in [44]) and still there remains approximation. We have to use a unified angleχ between the cholesteric optical axis and HPM, hence the electric and magnetic polarizations are directed differently in a general case.…”
Section: The Case Of Unequal Anisotropies δ = δ µmentioning
confidence: 77%
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“…This expression is more exact in comparison with the earlier obtained approximation (Equation (10) in [44]) and still there remains approximation. We have to use a unified angleχ between the cholesteric optical axis and HPM, hence the electric and magnetic polarizations are directed differently in a general case.…”
Section: The Case Of Unequal Anisotropies δ = δ µmentioning
confidence: 77%
“…In other words, the cholesteric director, i.e., the unit vector of the preferred orientation of molecules, is constant in the interface-parallel cross-sections, and it uniformly rotates with increasing distance from the interface. Near the interface, a chiral optical Tamm state (COTS) is possible, described in [44] in the limit of low cholesteric anisotropy. This state can be represented as a superposition of two circularly polarized counter-propagating co-handed waves with their strengths rotating in time in opposite directions.…”
Section: Modelmentioning
confidence: 99%
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“…In [32,33], we found the localized state in the structure containing a cholesteric liquid crystal. Later, a chiral analog of the TPP in a cholesteric liquid crystal was established [34]. In this case, the polarization-preserving anisotropic mirror made of a metal-dielectric nanocomposite was used as a metallic layer [35].…”
Section: Introductionmentioning
confidence: 99%