Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/2895
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dc.contributor.authorPullarkat, Pramod A.-
dc.contributor.authorHatwalne, Yashodhan-
dc.contributor.authorMadhusudana, N.V.-
dc.date.accessioned2007-06-15T09:01:59Z-
dc.date.available2007-06-15T09:01:59Z-
dc.date.issued2001-01-
dc.identifier.citationLiquid Crystals, 2001, Vol.28, p525 - 533en
dc.identifier.issn0267-8292-
dc.identifier.issn1366-5855 (online)-
dc.identifier.urihttp://hdl.handle.net/2289/2895-
dc.descriptionRestricted Access.en
dc.description.abstractWe 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* (UTGBC*) phase. In the UTGBC* 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 TGBA-TGBC-SmC* sequence. As the chiral strength is increased this goes to the sequence TGBA-UTGBC*-SmC*. Such sequences have been observed experimentally.en
dc.format.extent324759 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherTaylor & Francisen
dc.relation.urihttp://dx.doi.org/10.1080/02678290010018033en
dc.rights2001 Taylor & Francisen
dc.titleA phenomenological model for the undulating twist grain boundary-C* phaseen
dc.typeArticleen
Appears in Collections:Research Papers (SCM)

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