Full metadata record
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Cady, A | en_US |
dc.contributor.author | Liu, ZQ | en_US |
dc.contributor.author | Han, XF | en_US |
dc.contributor.author | Wang, ST | en_US |
dc.contributor.author | Veum, M | en_US |
dc.contributor.author | Janarthanan, N | en_US |
dc.contributor.author | Hsu, CS | en_US |
dc.contributor.author | Olson, DA | en_US |
dc.contributor.author | Huang, CC | en_US |
dc.date.accessioned | 2019-04-03T06:38:05Z | - |
dc.date.available | 2019-04-03T06:38:05Z | - |
dc.date.issued | 2002-12-01 | en_US |
dc.identifier.issn | 1539-3755 | en_US |
dc.identifier.uri | http://dx.doi.org/10.1103/PhysRevE.66.061704 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/28328 | - |
dc.description.abstract | We present differential optical reflectivity and null transmission ellipsometry data from several mixtures of MHPBC enantiomers. From this data, we have determined the chiral smectic phase sequence as a function of enantiomeric excess. The data suggest a change in the structure of the smectic-C(alpha)* phase and the surface tilt state as the enantiomeric excess is reduced. The results also show that the intermediate phases, smectic C(FI2)*, smectic C(FI1)*, and smectic C(alpha)*, disappear sequentially on reducing the net chirality. | en_US |
dc.language.iso | en_US | en_US |
dc.title | Effect of enantiomeric excess on surface structures and phase sequences in free-standing liquid-crystal films | en_US |
dc.type | Article | en_US |
dc.identifier.doi | 10.1103/PhysRevE.66.061704 | en_US |
dc.identifier.journal | PHYSICAL REVIEW E | en_US |
dc.citation.volume | 66 | en_US |
dc.citation.issue | 6 | en_US |
dc.citation.spage | 0 | en_US |
dc.citation.epage | 0 | en_US |
dc.contributor.department | 應用化學系 | zh_TW |
dc.contributor.department | Department of Applied Chemistry | en_US |
dc.identifier.wosnumber | WOS:000180427000046 | en_US |
dc.citation.woscount | 15 | en_US |
Appears in Collections: | Articles |
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