2015
DOI: 10.1080/15421406.2015.1066554
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Blue Phase Range Widening Induced by Laponite Nanoplatelets in the Chiral Liquid Crystal CE8

Abstract: We report on the widening of blue phase range induced by surface-functionalised laponite nanoplatelets dispersed in a chiral liquid crystal. The results are obtained by means of high-resolution ac calorimetry and optical microscopy and they are reproducible upon heating and cooling, identifying thermodynamically stable blue phases. It is shown that nanoplatelets target mostly the cubic structure of blue phase I and increase its temperature stability range by a factor of two. The present results are in agreemen… Show more

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Cited by 14 publications
(7 citation statements)
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“…The small spherical QDs of the present and previous studies [44,45] exhibit a minor shift of the BPIII-I transition temperature to slightly higher or lower values (depending on the QDs size, surface functionalization, and the LC host). On the contrary, large anisotropic NPs, such as graphene, laponite, and MoS 2 nanosheets, systematically upshift the BPIII-I transition temperature even at minute concentrations [55][56][57]67]. This trend confirmed by other studies [68,69] is attributed to the ordering of LC molecules induced within the I phase by the large surfaces of nanosheets.…”
Section: Discussionsupporting
confidence: 77%
See 1 more Smart Citation
“…The small spherical QDs of the present and previous studies [44,45] exhibit a minor shift of the BPIII-I transition temperature to slightly higher or lower values (depending on the QDs size, surface functionalization, and the LC host). On the contrary, large anisotropic NPs, such as graphene, laponite, and MoS 2 nanosheets, systematically upshift the BPIII-I transition temperature even at minute concentrations [55][56][57]67]. This trend confirmed by other studies [68,69] is attributed to the ordering of LC molecules induced within the I phase by the large surfaces of nanosheets.…”
Section: Discussionsupporting
confidence: 77%
“…This trend confirmed by other studies [68,69] is attributed to the ordering of LC molecules induced within the I phase by the large surfaces of nanosheets. It also explains why large anisotropic NPs with similar surface functionalization promote the stabilization of the more ordered BPI structure over the less ordered, macroscopically amorphous BPIII [55][56][57]67].…”
Section: Discussionmentioning
confidence: 95%
“…This upshift is much stronger for large anisotropic NPs with respect to their spherical counterparts dispersed in CE8. Substantial upshift of the isotropic to the liquid-crystalline phase transition has also been reported in other studies of anisotropic NPs (e.g., laponite clay nanoplatelets, graphene oxide nanosheets, carbon nanotubes) dispersed in chiral and non-chiral LCs [77][78][79][80][81][82]. A mean-field-based interpretation has been proposed by Gorkunov and Osipov [83].…”
Section: Blue Phase and Twist-grain Boundary Phase Stabilization In Liquid Crystal Ce8 Induced By Anisotropic Nanoparticlessupporting
confidence: 56%
“…Conflict between chirality and positional order of smectic phase is compromised when layers clubs together in form of twist grain boundary and each boundary displays rotation in helix form which also resembles screw dislocation. These can further be grouped to TGBP-A, C and C-chiral based on smectic phase present for transition [7,[23][24][25][26]. Ferroelectric LC owing to pre-occupied polarization (groups with dipole moment e.g.…”
Section: Introductionmentioning
confidence: 99%
“…However, increasing dimensions can lead to stabilization of blue phase as demonstrated by Lavrič mons mass% with potential applicability in electro-optical devices. Formulated LCs enhance stability to 6 K and 7.5 K respectively for clay and graphene (when compared to neat CE8) with both promoting formation of blue phase-I over others owing to considerable surface areas of both reinforcements [23,24]. 3).…”
Section: Introductionmentioning
confidence: 99%