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dc.contributor.authorVIJ, JAGDISHen
dc.contributor.authorSONG, JANG-KUNen
dc.contributor.authorPANARIN, YURIen
dc.date.accessioned2009-05-12T12:55:28Z
dc.date.available2009-05-12T12:55:28Z
dc.date.issued2008en
dc.date.submitted2008en
dc.identifier.citationSandhya, K.L., Song, J.K., Panarin, Yu.P., Vij, J.K., Kumar, S., Experimental study of high-temperature smectic- C FI2 phase in chiral smectic liquid crystals that exhibit phase-sequence reversal , Physical Review E - Statistical, Nonlinear, and Soft Matter Physics, 77, 5, 2008, 051707 -en
dc.identifier.otherYen
dc.identifier.urihttp://hdl.handle.net/2262/29915
dc.descriptionPUBLISHEDen
dc.description.abstractWe report the results of an experimental study of a recently observed phase sequence reversal of smectic-C<sub>FI2</sub><sup>*</sup> [SmC*(qT=1/2); a four layer antiferroelectric] phase appearing in the temperature range above the smectic-C* (SmC*) phase from the results of optical birefringence, spontaneous polarization, selective reflection, conoscopy, and dielectric spectroscopy. The SmC<sub>FI2</sub><sup>*</sup> phase is observed in an antiferroelectric liquid crystalline compound, 10OHF, in a temperature range above that of SmC* phase and is found to be thermodynamically monotropic, i.e., it appears only upon cooling from SmC<sub>alpha</sub><sup>*</sup> phase. This is also unstable as if it is once transformed to SmC* by the application of the bias, it does not return to its original state unless the sample is heated and cooled again in the absence of the bias. Nevertheless this phase is stabilized by the addition of a chiral smectic compound 9OTBBB1M7 (abbreviated as C9), having a wide temperature range of the SmC<sub>FI2</sub><sup>*</sup> phase. The temperature range of the low temperature SmC* decreases with increase in the concentration of C9 and for a concentration of 55 wt. %, SmC* disappears and the transition takes place directly from SmC<sub>FI2</sub><sup>*</sup> to the crystalline phase on cooling. The existence of such a high-temperature SmC<sub>FI2</sub><sup>*</sup> phase is also supported by a phenomenological model.en
dc.description.sponsorshipThe authors thank H. T. Srinivasa, Raman Research Institute, Bangalore, India, for assisting in the synthesis of these compounds. K.L.S. thanks IRCSET for support. J.K.S. thanks Samsung Electronics Co., Ltd., for granting a leave of absence from Seoul and SFI is thanked for Grant No. 02/ IN.1/I031. We also thank Nissan chemicals, Tokyo for supplying polyimide aligning agent RN1175. We thank Atsuo Fukuda for fruitful discussions.en
dc.format.extent051707en
dc.format.mimetypeapplication/pdf
dc.language.isoenen
dc.relation.ispartofseriesPhysical Review E - Statistical, Nonlinear, and Soft Matter Physicsen
dc.relation.ispartofseries77en
dc.relation.ispartofseries5en
dc.rightsYen
dc.subjectElectronic & Electrical Engineeringen
dc.titleExperimental study of high-temperature smectic- C FI2 phase in chiral smectic liquid crystals that exhibit phase-sequence reversalen
dc.typeJournal Articleen
dc.type.supercollectionscholarly_publicationsen
dc.type.supercollectionrefereed_publicationsen
dc.identifier.peoplefinderurlhttp://people.tcd.ie/jvijen
dc.identifier.peoplefinderurlhttp://people.tcd.ie/ypanarinen
dc.identifier.rssinternalid58098en
dc.identifier.doihttp://dx.doi.org/10.1103/PhysRevE.77.051707en
dc.identifier.rssurihttp://dx.doi.org/10.1103/PhysRevE.77.051707
dc.contributor.sponsorScience Foundation Ireland (SFI)en


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