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dc.contributor.authorLiu, Z. Q.en_US
dc.contributor.authorMcCoy, B. K.en_US
dc.contributor.authorWang, S. T.en_US
dc.contributor.authorPindak, R.en_US
dc.contributor.authorCaliebe, W.en_US
dc.contributor.authorBarois, P.en_US
dc.contributor.authorFernandes, P.en_US
dc.contributor.authorNguyen, H. T.en_US
dc.contributor.authorHsu, C. S.en_US
dc.contributor.authorWang, Shunen_US
dc.contributor.authorHuang, C. C.en_US
dc.date.accessioned2019-04-03T06:40:51Z-
dc.date.available2019-04-03T06:40:51Z-
dc.date.issued2007-08-17en_US
dc.identifier.issn0031-9007en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevLett.99.077802en_US
dc.identifier.urihttp://hdl.handle.net/11536/10437-
dc.description.abstractEmploying resonant x-ray diffraction, we observed unique pitch evolutions in the smectic-C-alpha* phase in mixtures of two antiferroelectric liquid crystals. Our results show that the pitch in this phase continuously evolves across 4 layers, contradicting a theoretical model that predicts that the smectic-C-FI2* phase intervenes in the smectic-C-alpha* phase. The phase sequences we found can be explained by another model that includes one type of long-range interaction among smectic layers.en_US
dc.language.isoen_USen_US
dc.titleUnique pitch evolution in the Smectic-C-alpha(*) phaseen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevLett.99.077802en_US
dc.identifier.journalPHYSICAL REVIEW LETTERSen_US
dc.citation.volume99en_US
dc.citation.issue7en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department應用化學系zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.identifier.wosnumberWOS:000248866900052en_US
dc.citation.woscount27en_US
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