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A phenomenological model for the undulating twist grain boundary-C phase
We propose a simple phenomenological model which is able to account for the various twist grain boundary (TGB) phases, including the recently discovered undulating twist grain boundary-C* (UTGB C* ) phase. In the UTGB C* phase, the smectic C* (SmC*)-like blocks and the grain boundaries separating th...
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Published in: | Liquid crystals 2001-04, Vol.28 (4), p.525-533 |
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container_end_page | 533 |
container_issue | 4 |
container_start_page | 525 |
container_title | Liquid crystals |
container_volume | 28 |
creator | Pramod, P. A. Hatwalne, Yashodhan Madhusudana, N. V. |
description | We propose a simple phenomenological model which is able to account for the various twist grain boundary (TGB) phases, including the recently discovered undulating twist grain boundary-C* (UTGB
C*
) phase. In the UTGB
C*
phase, the smectic C* (SmC*)-like blocks and the grain boundaries separating them undulate to form a two-dimensional square lattice perpendicular to the TGB helix axis. We treat the grain boundaries separating adjacent smectic blocks as interfaces with an anisotropic interfacial tension. At moderate chiral strengths we find a TGB
A
-TGB
C
-SmC* sequence. As the chiral strength is increased this goes to the sequence TGB
A
-UTGB
C*
-SmC*. Such sequences have been observed experimentally. |
doi_str_mv | 10.1080/02678290010018033 |
format | article |
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C*
) phase. In the UTGB
C*
phase, the smectic C* (SmC*)-like blocks and the grain boundaries separating them undulate to form a two-dimensional square lattice perpendicular to the TGB helix axis. We treat the grain boundaries separating adjacent smectic blocks as interfaces with an anisotropic interfacial tension. At moderate chiral strengths we find a TGB
A
-TGB
C
-SmC* sequence. As the chiral strength is increased this goes to the sequence TGB
A
-UTGB
C*
-SmC*. Such sequences have been observed experimentally.</description><identifier>ISSN: 0267-8292</identifier><identifier>EISSN: 1366-5855</identifier><identifier>DOI: 10.1080/02678290010018033</identifier><language>eng</language><publisher>Taylor & Francis Group</publisher><ispartof>Liquid crystals, 2001-04, Vol.28 (4), p.525-533</ispartof><rights>Copyright Taylor & Francis Group, LLC 2001</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c344t-e1c6bff7e06fa5f8268f509143223e5f91396729c4791e85c11b22b348aff4c83</citedby><cites>FETCH-LOGICAL-c344t-e1c6bff7e06fa5f8268f509143223e5f91396729c4791e85c11b22b348aff4c83</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,27905,27906</link.rule.ids></links><search><creatorcontrib>Pramod, P. A.</creatorcontrib><creatorcontrib>Hatwalne, Yashodhan</creatorcontrib><creatorcontrib>Madhusudana, N. V.</creatorcontrib><title>A phenomenological model for the undulating twist grain boundary-C phase</title><title>Liquid crystals</title><description>We propose a simple phenomenological model which is able to account for the various twist grain boundary (TGB) phases, including the recently discovered undulating twist grain boundary-C* (UTGB
C*
) phase. In the UTGB
C*
phase, the smectic C* (SmC*)-like blocks and the grain boundaries separating them undulate to form a two-dimensional square lattice perpendicular to the TGB helix axis. We treat the grain boundaries separating adjacent smectic blocks as interfaces with an anisotropic interfacial tension. At moderate chiral strengths we find a TGB
A
-TGB
C
-SmC* sequence. As the chiral strength is increased this goes to the sequence TGB
A
-UTGB
C*
-SmC*. Such sequences have been observed experimentally.</description><issn>0267-8292</issn><issn>1366-5855</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2001</creationdate><recordtype>article</recordtype><recordid>eNqFkM1KQzEQhYMoWKsP4C4vcDU_Nz8X3JSiVii40XXITZM2kntTkpTatzel7goKM8zizHeYOQDcY_SAkUSPiHAhSYcQriURpRdgginnDZOMXYLJUW_qArkGNzl_IYSElGICFjO43dgxDrVDXHujAxziygboYoJlY-FuXO2CLn5cw7L3ucB10n6EfayCTodmXg10trfgyumQ7d3vnILPl-eP-aJZvr--zWfLxtC2LY3FhvfOCYu408xJwqVjqMMtJYRa5jpMOy5IZ1rRYSuZwbgnpKet1M61RtIpwCdfk2LOyTq1TX6ohyiM1DEKdRZFZZ5OjB_rV4PexxRWquhDiMklPRqfFf0LF__iZ5Qq34X-AEybdfs</recordid><startdate>20010401</startdate><enddate>20010401</enddate><creator>Pramod, P. A.</creator><creator>Hatwalne, Yashodhan</creator><creator>Madhusudana, N. V.</creator><general>Taylor & Francis Group</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20010401</creationdate><title>A phenomenological model for the undulating twist grain boundary-C phase</title><author>Pramod, P. A. ; Hatwalne, Yashodhan ; Madhusudana, N. V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c344t-e1c6bff7e06fa5f8268f509143223e5f91396729c4791e85c11b22b348aff4c83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2001</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Pramod, P. A.</creatorcontrib><creatorcontrib>Hatwalne, Yashodhan</creatorcontrib><creatorcontrib>Madhusudana, N. V.</creatorcontrib><collection>CrossRef</collection><jtitle>Liquid crystals</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Pramod, P. A.</au><au>Hatwalne, Yashodhan</au><au>Madhusudana, N. V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A phenomenological model for the undulating twist grain boundary-C phase</atitle><jtitle>Liquid crystals</jtitle><date>2001-04-01</date><risdate>2001</risdate><volume>28</volume><issue>4</issue><spage>525</spage><epage>533</epage><pages>525-533</pages><issn>0267-8292</issn><eissn>1366-5855</eissn><abstract>We propose a simple phenomenological model which is able to account for the various twist grain boundary (TGB) phases, including the recently discovered undulating twist grain boundary-C* (UTGB
C*
) phase. In the UTGB
C*
phase, the smectic C* (SmC*)-like blocks and the grain boundaries separating them undulate to form a two-dimensional square lattice perpendicular to the TGB helix axis. We treat the grain boundaries separating adjacent smectic blocks as interfaces with an anisotropic interfacial tension. At moderate chiral strengths we find a TGB
A
-TGB
C
-SmC* sequence. As the chiral strength is increased this goes to the sequence TGB
A
-UTGB
C*
-SmC*. Such sequences have been observed experimentally.</abstract><pub>Taylor & Francis Group</pub><doi>10.1080/02678290010018033</doi><tpages>9</tpages></addata></record> |
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title | A phenomenological model for the undulating twist grain boundary-C phase |
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