2014
DOI: 10.3390/ma7031502
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Dispersion of γ-Alumina Nano-Sized Spherical Particles in a Calamitic Liquid Crystal. Study and Optimization of the Confinement Effects

Abstract: We report an experimental study on confined systems formed by butyloxybenzylidene octylaniline liquid crystal (4O.8) + γ-alumina nanoparticles. The effects of the confinement in the thermal and dielectric properties of the liquid crystal under different densities of nanoparticles is analyzed by means of high resolution Modulated Differential Scanning Calorimetry (MDSC) and broadband dielectric spectroscopy. First, a drastic depression of the N-I and SmA-N transition temperatures is observed with confinement, t… Show more

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Cited by 8 publications
(8 citation statements)
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“…Figure 2 shows the specific heat vs. temperature around the N-I phase transition for bulk CBO11O.Py and some of the confined samples. As expected, the dispersion of nanoparticles induces a downward shift in the N-I phase transition temperature together with a suppressed and rounded specific heat peak similar to what is found for other liquid crystals under confinement [ 26 , 28 , 29 , 30 , 31 ]. This effect can be translated to the other phase transitions (N g -N spc , Cr-N and Cr-I), but the depression in temperature is lesser.…”
Section: Resultssupporting
confidence: 81%
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“…Figure 2 shows the specific heat vs. temperature around the N-I phase transition for bulk CBO11O.Py and some of the confined samples. As expected, the dispersion of nanoparticles induces a downward shift in the N-I phase transition temperature together with a suppressed and rounded specific heat peak similar to what is found for other liquid crystals under confinement [ 26 , 28 , 29 , 30 , 31 ]. This effect can be translated to the other phase transitions (N g -N spc , Cr-N and Cr-I), but the depression in temperature is lesser.…”
Section: Resultssupporting
confidence: 81%
“…Such a linear dependence is fitted to the relationship 1TρsTbulk=Aρs where A = 0.078 cm 3 ·g −1 . This behavior differs substantially from that of the 4O.8 monomer confined via the dispersion of the same γ-alumina nanoparticles [26], in which the dependence was not linear. Such a difference could be explained by arguing that, since the CBO11O.Py molecule is larger and more flexible than the 4O.8 one, more dispersive material is needed to induce similar changes in the transition temperatures in the former with respect to the latter.…”
Section: Resultsmentioning
confidence: 83%
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“…These inorganic materials can tolerate high temperatures and provide high reliability. Doping different types of nanoparticles (NPs), such as polyhedral oligomeric silsesquioxane (POSS) [ 19 , 20 ], alumina NPs [ 21 ], metallic NPs [ 22 , 23 , 24 ], and ionic surfactant [ 25 ] into an LC film can induce the microscopic alignment of LC molecules. Achieving LC alignment by dispersing NPs into LCs is an easier method than using conventional polymer layers.…”
Section: Introductionmentioning
confidence: 99%