Electrically turning periodic structures in cholesteric layer with conical–planar boundary conditions

Abstract Electro-optical cell based on the cholesteric liquid crystal is studied with unique combination of the boundary conditions: conical anchoring on the one substrate and planar anchoring on another one. Periodic structures in cholesteric layer and their transformation under applied electric fi...

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Autores principales: Oxana Prishchepa, Mikhail Krakhalev, Vladimir Rudyak, Vitaly Sutormin, Victor Zyryanov
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Lenguaje:EN
Publicado: Nature Portfolio 2021
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Acceso en línea:https://doaj.org/article/0676eacbfa6144f8a6836b205e9e1428
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spelling oai:doaj.org-article:0676eacbfa6144f8a6836b205e9e14282021-12-02T15:51:12ZElectrically turning periodic structures in cholesteric layer with conical–planar boundary conditions10.1038/s41598-021-87854-z2045-2322https://doaj.org/article/0676eacbfa6144f8a6836b205e9e14282021-04-01T00:00:00Zhttps://doi.org/10.1038/s41598-021-87854-zhttps://doaj.org/toc/2045-2322Abstract Electro-optical cell based on the cholesteric liquid crystal is studied with unique combination of the boundary conditions: conical anchoring on the one substrate and planar anchoring on another one. Periodic structures in cholesteric layer and their transformation under applied electric field are considered by polarizing optical microscopy, the experimental findings are supported by the data of the calculations performed using the extended Frank elastic continuum approach. Such structures are the set of alternating over- and under-twisted defect lines whose azimuthal director angles differ by $$180^\circ$$ 180 ∘ . The $$U^+$$ U + and $$U^-$$ U - -defects of periodicity, which are the smooth transition between the defect lines, are observed at the edge of electrode area. The growth direction of defect lines forming a diffraction grating can be controlled by applying a voltage in the range of $$0\le \, V \le 1.3$$ 0 ≤ V ≤ 1.3  V during the process. Resulting orientation and distance between the lines don’t change under voltage. However, at $$V>1.3$$ V > 1.3  V $$U^+$$ U + -defects move along the defect lines away from the electrode edges, and, finally, the grating lines collapse at the cell’s center. These results open a way for the use of such cholesteric material in applications with periodic defect structures where a periodicity, orientation, and configuration of defects should be adjusted.Oxana PrishchepaMikhail KrakhalevVladimir RudyakVitaly SutorminVictor ZyryanovNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 11, Iss 1, Pp 1-10 (2021)
institution DOAJ
collection DOAJ
language EN
topic Medicine
R
Science
Q
spellingShingle Medicine
R
Science
Q
Oxana Prishchepa
Mikhail Krakhalev
Vladimir Rudyak
Vitaly Sutormin
Victor Zyryanov
Electrically turning periodic structures in cholesteric layer with conical–planar boundary conditions
description Abstract Electro-optical cell based on the cholesteric liquid crystal is studied with unique combination of the boundary conditions: conical anchoring on the one substrate and planar anchoring on another one. Periodic structures in cholesteric layer and their transformation under applied electric field are considered by polarizing optical microscopy, the experimental findings are supported by the data of the calculations performed using the extended Frank elastic continuum approach. Such structures are the set of alternating over- and under-twisted defect lines whose azimuthal director angles differ by $$180^\circ$$ 180 ∘ . The $$U^+$$ U + and $$U^-$$ U - -defects of periodicity, which are the smooth transition between the defect lines, are observed at the edge of electrode area. The growth direction of defect lines forming a diffraction grating can be controlled by applying a voltage in the range of $$0\le \, V \le 1.3$$ 0 ≤ V ≤ 1.3  V during the process. Resulting orientation and distance between the lines don’t change under voltage. However, at $$V>1.3$$ V > 1.3  V $$U^+$$ U + -defects move along the defect lines away from the electrode edges, and, finally, the grating lines collapse at the cell’s center. These results open a way for the use of such cholesteric material in applications with periodic defect structures where a periodicity, orientation, and configuration of defects should be adjusted.
format article
author Oxana Prishchepa
Mikhail Krakhalev
Vladimir Rudyak
Vitaly Sutormin
Victor Zyryanov
author_facet Oxana Prishchepa
Mikhail Krakhalev
Vladimir Rudyak
Vitaly Sutormin
Victor Zyryanov
author_sort Oxana Prishchepa
title Electrically turning periodic structures in cholesteric layer with conical–planar boundary conditions
title_short Electrically turning periodic structures in cholesteric layer with conical–planar boundary conditions
title_full Electrically turning periodic structures in cholesteric layer with conical–planar boundary conditions
title_fullStr Electrically turning periodic structures in cholesteric layer with conical–planar boundary conditions
title_full_unstemmed Electrically turning periodic structures in cholesteric layer with conical–planar boundary conditions
title_sort electrically turning periodic structures in cholesteric layer with conical–planar boundary conditions
publisher Nature Portfolio
publishDate 2021
url https://doaj.org/article/0676eacbfa6144f8a6836b205e9e1428
work_keys_str_mv AT oxanaprishchepa electricallyturningperiodicstructuresincholestericlayerwithconicalplanarboundaryconditions
AT mikhailkrakhalev electricallyturningperiodicstructuresincholestericlayerwithconicalplanarboundaryconditions
AT vladimirrudyak electricallyturningperiodicstructuresincholestericlayerwithconicalplanarboundaryconditions
AT vitalysutormin electricallyturningperiodicstructuresincholestericlayerwithconicalplanarboundaryconditions
AT victorzyryanov electricallyturningperiodicstructuresincholestericlayerwithconicalplanarboundaryconditions
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