Domain reorientation due to smectic layer instability in high tilt angle-based surface stabilized ferroelectric liquid crystal cell
High tilt angle (45 °) ferroelectric liquid crystal ( F L C) in surface stabilized geometry, having no chiral smectic A ( S m A ∗) phase, has been studied for the reorientation of the smectic layers near the transition temperature ( T c). The electro-optical studies have shown the stripe domain form...
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creator | Yadav, Neha Kumar, Suraj Choudhary, Amit Thakur, Anil K. Rajesh Singh, Surinder P. Biradar, Ashok M. |
description | High tilt angle (45
°) ferroelectric liquid crystal (
F
L
C) in surface stabilized geometry, having no chiral smectic A (
S
m
A
∗) phase, has been studied for the reorientation of the smectic layers near the transition temperature (
T
c). The electro-optical studies have shown the stripe domain formation in which the liquid crystal molecules are aligned along the rubbing direction, but the smectic layers are tilted away from the rubbing direction at room temperature. In such high tilt angle
F
L
C
s, the molecular alignment and smectic layer formation start from bottom and top rubbed grooves at
T
c. The domain formation of the FLC takes place in the middle of the top and bottom surfaces due to the frustration of the dipolar interaction. The smectic layer switching is observed by optical microscopy and confirmed by the dielectric spectroscopy method near
T
c of
S
m
C
∗ and chiral nematic phases. Domain switching has shown a larger switching angle than the molecular tilt angle within the smectic layer. These studies are expected to be significant for understanding the smectic layer structure and the domain switching process, which may pave the way for large optical switching devices. |
doi_str_mv | 10.1063/5.0198434 |
format | Article |
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°) ferroelectric liquid crystal (
F
L
C) in surface stabilized geometry, having no chiral smectic A (
S
m
A
∗) phase, has been studied for the reorientation of the smectic layers near the transition temperature (
T
c). The electro-optical studies have shown the stripe domain formation in which the liquid crystal molecules are aligned along the rubbing direction, but the smectic layers are tilted away from the rubbing direction at room temperature. In such high tilt angle
F
L
C
s, the molecular alignment and smectic layer formation start from bottom and top rubbed grooves at
T
c. The domain formation of the FLC takes place in the middle of the top and bottom surfaces due to the frustration of the dipolar interaction. The smectic layer switching is observed by optical microscopy and confirmed by the dielectric spectroscopy method near
T
c of
S
m
C
∗ and chiral nematic phases. Domain switching has shown a larger switching angle than the molecular tilt angle within the smectic layer. These studies are expected to be significant for understanding the smectic layer structure and the domain switching process, which may pave the way for large optical switching devices.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/5.0198434</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Ferroelectric materials ; Ferroelectricity ; Grooves ; Liquid crystals ; Optical microscopy ; Optical switching ; Room temperature ; Rubbing ; Surface stability ; Transition temperature</subject><ispartof>Journal of applied physics, 2024-04, Vol.135 (15)</ispartof><rights>Author(s)</rights><rights>2024 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c287t-e27ac7c3edc121ccd8985eb6ef122d7123bfee47a22ebab26ad2e2baa2a72fbf3</cites><orcidid>0000-0001-6670-6207 ; 0000-0002-5713-8217 ; 0000-0002-5913-0657</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Yadav, Neha</creatorcontrib><creatorcontrib>Kumar, Suraj</creatorcontrib><creatorcontrib>Choudhary, Amit</creatorcontrib><creatorcontrib>Thakur, Anil K.</creatorcontrib><creatorcontrib>Rajesh</creatorcontrib><creatorcontrib>Singh, Surinder P.</creatorcontrib><creatorcontrib>Biradar, Ashok M.</creatorcontrib><title>Domain reorientation due to smectic layer instability in high tilt angle-based surface stabilized ferroelectric liquid crystal cell</title><title>Journal of applied physics</title><description>High tilt angle (45
°) ferroelectric liquid crystal (
F
L
C) in surface stabilized geometry, having no chiral smectic A (
S
m
A
∗) phase, has been studied for the reorientation of the smectic layers near the transition temperature (
T
c). The electro-optical studies have shown the stripe domain formation in which the liquid crystal molecules are aligned along the rubbing direction, but the smectic layers are tilted away from the rubbing direction at room temperature. In such high tilt angle
F
L
C
s, the molecular alignment and smectic layer formation start from bottom and top rubbed grooves at
T
c. The domain formation of the FLC takes place in the middle of the top and bottom surfaces due to the frustration of the dipolar interaction. The smectic layer switching is observed by optical microscopy and confirmed by the dielectric spectroscopy method near
T
c of
S
m
C
∗ and chiral nematic phases. Domain switching has shown a larger switching angle than the molecular tilt angle within the smectic layer. These studies are expected to be significant for understanding the smectic layer structure and the domain switching process, which may pave the way for large optical switching devices.</description><subject>Ferroelectric materials</subject><subject>Ferroelectricity</subject><subject>Grooves</subject><subject>Liquid crystals</subject><subject>Optical microscopy</subject><subject>Optical switching</subject><subject>Room temperature</subject><subject>Rubbing</subject><subject>Surface stability</subject><subject>Transition temperature</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp90E1LAzEQBuAgCtbqwX8Q8KSwNR_dTfYo9RMKXvS8JNlJm5Ju2iR7qFf_uFu2Z08zDA_vwIvQLSUzSir-WM4IreWcz8_QhBJZF6IsyTmaEMJoIWtRX6KrlDaEUCp5PUG_z2GrXIcjhOigyyq70OG2B5wDTlsw2Rns1QEidl3KSjvv8mHY8dqt1jg7n7HqVh4KrRK0OPXRKgP4RH-Gk4UYA_ghKh6z3L53LTbxMBCPDXh_jS6s8gluTnOKvl9fvhbvxfLz7WPxtCwMkyIXwIQywnBoDWXUmFbWsgRdgaWMtYIyri3AXCjGQCvNKtUyYFoppgSz2vIpuhtzdzHse0i52YQ-dsPLhhMua8ZLUQ3qflQmhpQi2GYX3VbFQ0NJc-y4KZtTx4N9GG0ybqzuH_wHtsJ_5g</recordid><startdate>20240421</startdate><enddate>20240421</enddate><creator>Yadav, Neha</creator><creator>Kumar, Suraj</creator><creator>Choudhary, Amit</creator><creator>Thakur, Anil K.</creator><creator>Rajesh</creator><creator>Singh, Surinder P.</creator><creator>Biradar, Ashok M.</creator><general>American Institute of Physics</general><scope>AJDQP</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-6670-6207</orcidid><orcidid>https://orcid.org/0000-0002-5713-8217</orcidid><orcidid>https://orcid.org/0000-0002-5913-0657</orcidid></search><sort><creationdate>20240421</creationdate><title>Domain reorientation due to smectic layer instability in high tilt angle-based surface stabilized ferroelectric liquid crystal cell</title><author>Yadav, Neha ; Kumar, Suraj ; Choudhary, Amit ; Thakur, Anil K. ; Rajesh ; Singh, Surinder P. ; Biradar, Ashok M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c287t-e27ac7c3edc121ccd8985eb6ef122d7123bfee47a22ebab26ad2e2baa2a72fbf3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Ferroelectric materials</topic><topic>Ferroelectricity</topic><topic>Grooves</topic><topic>Liquid crystals</topic><topic>Optical microscopy</topic><topic>Optical switching</topic><topic>Room temperature</topic><topic>Rubbing</topic><topic>Surface stability</topic><topic>Transition temperature</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yadav, Neha</creatorcontrib><creatorcontrib>Kumar, Suraj</creatorcontrib><creatorcontrib>Choudhary, Amit</creatorcontrib><creatorcontrib>Thakur, Anil K.</creatorcontrib><creatorcontrib>Rajesh</creatorcontrib><creatorcontrib>Singh, Surinder P.</creatorcontrib><creatorcontrib>Biradar, Ashok M.</creatorcontrib><collection>AIP Open Access Journals</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yadav, Neha</au><au>Kumar, Suraj</au><au>Choudhary, Amit</au><au>Thakur, Anil K.</au><au>Rajesh</au><au>Singh, Surinder P.</au><au>Biradar, Ashok M.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Domain reorientation due to smectic layer instability in high tilt angle-based surface stabilized ferroelectric liquid crystal cell</atitle><jtitle>Journal of applied physics</jtitle><date>2024-04-21</date><risdate>2024</risdate><volume>135</volume><issue>15</issue><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>High tilt angle (45
°) ferroelectric liquid crystal (
F
L
C) in surface stabilized geometry, having no chiral smectic A (
S
m
A
∗) phase, has been studied for the reorientation of the smectic layers near the transition temperature (
T
c). The electro-optical studies have shown the stripe domain formation in which the liquid crystal molecules are aligned along the rubbing direction, but the smectic layers are tilted away from the rubbing direction at room temperature. In such high tilt angle
F
L
C
s, the molecular alignment and smectic layer formation start from bottom and top rubbed grooves at
T
c. The domain formation of the FLC takes place in the middle of the top and bottom surfaces due to the frustration of the dipolar interaction. The smectic layer switching is observed by optical microscopy and confirmed by the dielectric spectroscopy method near
T
c of
S
m
C
∗ and chiral nematic phases. Domain switching has shown a larger switching angle than the molecular tilt angle within the smectic layer. These studies are expected to be significant for understanding the smectic layer structure and the domain switching process, which may pave the way for large optical switching devices.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0198434</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0001-6670-6207</orcidid><orcidid>https://orcid.org/0000-0002-5713-8217</orcidid><orcidid>https://orcid.org/0000-0002-5913-0657</orcidid><oa>free_for_read</oa></addata></record> |
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source | Alma/SFX Local Collection |
subjects | Ferroelectric materials Ferroelectricity Grooves Liquid crystals Optical microscopy Optical switching Room temperature Rubbing Surface stability Transition temperature |
title | Domain reorientation due to smectic layer instability in high tilt angle-based surface stabilized ferroelectric liquid crystal cell |
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