Pixel-isolated liquid-crystal mode by using a patterned anisotropic phase separation for flexible LCDs

2007 ◽  
Vol 15 (2) ◽  
pp. 119 ◽  
Author(s):  
Se-Jin Jang ◽  
Jong-Wook Jung ◽  
Hak-Rin Kim ◽  
Min Young Jin ◽  
You-Jin Lee ◽  
...  
Keyword(s):  
Liquid Crystal ◽  
Phase Separation ◽  
Anisotropic Phase

Surface effects on photopolymerization induced anisotropic phase separation in liquid crystal and polymer composites

2007 ◽  
Vol 90 (19) ◽  
pp. 193510 ◽  
Author(s):  
Min Young Jin ◽  
Tae-Hee Lee ◽  
Jong-Wook Jung ◽  
Jae-Hoon Kim
Keyword(s):  
Liquid Crystal ◽  
Phase Separation ◽  
Polymer Composites ◽  
Surface Effects ◽  
Anisotropic Phase

Application to Mechanically Stable Flexible Liquid Crystal Displays Using Surface Induced Anisotropic Phase Separation

2008 ◽  
Vol 480 (1) ◽  
pp. 278-283 ◽  
Author(s):  
You-Jin Lee ◽  
Min Young Jin ◽  
Jong-Wook Jung ◽  
Hak-Rin Kim ◽  
Yoonseuk Choi ◽  
...  
Keyword(s):  
Liquid Crystal ◽  
Phase Separation ◽  
Liquid Crystal Displays ◽  
Anisotropic Phase

Dependence of Cell Gap on Anisotropic Phase Separation of Liquid Crystal and Polymer Composites

2007 ◽  
Vol 46 (4A) ◽  
pp. 1585-1589 ◽  
Author(s):  
Min Young Jin ◽  
Tae-Hee Lee ◽  
Se-Jin Jang ◽  
Ji-Hong Bae ◽  
Jae-Hoon Kim
Keyword(s):  
Liquid Crystal ◽  
Phase Separation ◽  
Polymer Composites ◽  
Anisotropic Phase

Formation of binary phase gratings in photopolymer-liquid crystal composites by a surface-controlled anisotropic phase separation

2005 ◽  
Vol 86 (2) ◽  
pp. 021906 ◽  
Author(s):  
Jae-Hong Park ◽  
Iam Choon Khoo ◽  
Chang-Jae Yu ◽  
Min-Sik Jung ◽  
Sin-Doo Lee
Keyword(s):  
Liquid Crystal ◽  
Phase Separation ◽  
Binary Phase ◽  
Anisotropic Phase

Phase equilibria in solutions of rod-like particles

1956 ◽  
Vol 234 (1196) ◽  
pp. 73-89 ◽  
Keyword(s):  
Free Energy ◽  
Phase Separation ◽  
Partition Function ◽  
Colloidal Particles ◽  
Double Layers ◽  
Positive Energy ◽  
Isotropic Phase ◽  
Electric Double Layers ◽  
Rigid Rod ◽  
Anisotropic Phase

A partition function for a system of rigid rod-like particles with partial orientation about an axis is derived through the use of a modified lattice model. In the limit of perfect orientation the partition function reduces to the ideal mixing law ; for complete disorientation it corresponds to the polymer mixing law for rigid chains. A general expression is given for the free energy of mixing as a function of the mole numbers, the axis ratio of the solute particles, and a disorientation parameter. This function passes through a minimum followed by a maximum with increase in the disorientation parameter, provided the latter exceeds a critical value which is 2e for the pure solute and which increases with dilution. Assigning this parameter the value which minimizes the free energy, the chemical potentials display discontinuities a t the concentration a t which the minimum first appears. Separation into an isotropic phase and a some what more concentrated anisotropic phase arises because of the discontinuity, in confirmation of the theories of Onsager and Isihara, which treat only the second virial coefficient. Phase separation thus arises as a consequence of particle asymmetry, unassisted by an energy term . Whereas for a large-particle asymmetry both phases in equilibrium are predicted to be fairly dilute when mixing is athermal, a comparatively small positive energy of interaction causes the concentration in the anisotropic phase to increase sharply, while the concentration in the isotropic phase becomes vanishingly small. The theory offers a statistical mechanical basis for interpreting precipitation of rod-like colloidal particles with the formation of fibrillar structures such as are prominent in the fibrous proteins. The asymmetry of tobacco mosaic virus particles (with or without inclusion of their electric double layers) is insufficient alone to explain the well-known phase separation which occurs from their dilute solutions at very low ionic strengths. Higher-order interaction between electric double layers appears to be a major factor in bringing about dilute phase separation for these and other asymmetric colloidal particles bearing large charges, as was pointed out previously by Oster.

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