2004
DOI: 10.1039/b400135b
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Advanced liquid crystals for television

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Cited by 239 publications
(187 citation statements)
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“…Difluorinated alkoxy compounds are suitable for preparation of VA mixtures because of their large negative dielectric anisotropy and low optical birefringence. Moreover, the recently synthesized terphenyl derivatives with lateral fluorine substitution have the additional advantage of low rotational viscosity, while keeping the birefringence moderately low as required for VA mode applications [14].…”
Section: Introductionmentioning
confidence: 99%
“…Difluorinated alkoxy compounds are suitable for preparation of VA mixtures because of their large negative dielectric anisotropy and low optical birefringence. Moreover, the recently synthesized terphenyl derivatives with lateral fluorine substitution have the additional advantage of low rotational viscosity, while keeping the birefringence moderately low as required for VA mode applications [14].…”
Section: Introductionmentioning
confidence: 99%
“…All these factors create additional sources of ions of organic origin [82]. However, recent advances in the chemical synthesis of novel liquid crystal materials exhibiting improved chemical stability reduced the probability of such events significantly [83][84][85][86]. Liquid crystals can get contaminated with ionic impurities during the process of chemical synthesis.…”
Section: Classical Methods Of Liquid Crystal Purificationmentioning
confidence: 99%
“…By applying the proper chemical design along with the methods of chemical synthesis and post-synthetic techniques, many improved liquid crystal materials were successfully produced and tested in numerous applications [2,28,[83][84][85][86]. The high resistivity liquid crystals are characterized by extremely low levels of ionic impurities.…”
Section: Practical Example: Electro-optics Of Highly Purified Liquid mentioning
confidence: 99%
“…the short axis of a GB monomer. As for the choice of the exponents, we recall that by integrating the dispersion interaction between a LJ particle and an infinite slab formed by LJ centres, an overall particle-surface potential governed by a (9,3) law is obtained. In the literature, the particle-surface energy is usually modelled with a variety of repulsive and attractive exponents, like the (10, 4) exponents implemented by Steuer et al, 26 and the (9, 3) used by Caprion et al 27 Considering that most common materials mentioned in the Introduction are far from being completely smooth 9,20,21 and also the existence of electrostatic interactions [13][14][15][16][17][18][19] between surfaces and molecules, we have arbitrarily set the repulsive coefficient n to a softer value of 6 to allow for some surface penetration, while keeping m = 3.…”
Section: Surface-monomer Interactionmentioning
confidence: 99%