Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/2322
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dc.contributor.authorKrishna Prasad, S.-
dc.contributor.authorNair, Geetha G.-
dc.contributor.authorChandrasekhar, S.-
dc.contributor.authorGoodby, J.W.-
dc.date.accessioned2007-05-17T09:54:04Z-
dc.date.available2007-05-17T09:54:04Z-
dc.date.issued1995-02-
dc.identifier.citationMolecular Crystals and Liquid Crystals, 1995, Vol.260, p387-394en
dc.identifier.issn1058-725X-
dc.identifier.urihttp://hdl.handle.net/2289/2322-
dc.descriptionRestricted Access.en
dc.description.abstractWe report high pressure studies on a binary system of 4-(2'-methyl butyl)phenyl 4'-n-octyl biphenyl-4-carboxylate (CE8 from BDH) and 4-n- dodecyloxy biphenyl-4'-(2'-methyl butyl)benzoate (C12). For the concentration range 0.32<X<0.62, where X is the weight fraction of C12, the system shows the following sequence of transitions at room pressure: Isotropic- Cholesteric (Ch)-Twist Grain Boundary (TGB)-Smectic A (A)Smectic C- (C*). For X=0.25, the Ch phase transforms directly to the A phase at 1 bar, but there is an induced TGB phase between the Ch and A phases at elevated pressures. Analysis of the topology of the pressure-temperature diagram in the vicinity of the Ch-TGB-A meeting point indicates that is a critical end point rather than a bicritical point as expected from the mean field theory. At X=0.64 there is a direct TGB-C* transition at 1 bar, but there appears a pressure induced A phase between the TGB and C* phases. The topology of the phase diagram suggests that the TGB-A-C* meeting point is a bicritical point.en
dc.format.extent295470 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherGordon and Breach Science Publishers.en
dc.relation.urihttp://dx.doi.org/10.1080/10587259508038712en
dc.rights1995 OPA (Overseas Publishers Association) N.V.en
dc.titlePressure induced twist grain boundary phaseen
dc.typeArticleen
Appears in Collections:Research Papers (SCM)

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