A novel method for encapsulation of a liquid crystal in monodisperse micron-sized polymer particles

2001 ◽  
Vol 279 (11) ◽  
pp. 1082-1089 ◽  
Author(s):  
N.-H. Park ◽  
S.-Il Park ◽  
K.-D. Suh

2015 ◽  
Vol 42 (6Part38) ◽  
pp. 3670-3670
Author(s):  
S Tokurei ◽  
J Morishita ◽  
K Shiotsuki ◽  
Y Bamba ◽  
M Ogaki ◽  
...  


1989 ◽  
Vol 28 (S2) ◽  
pp. 123 ◽  
Author(s):  
Guo-Ping Chen ◽  
Toyokazu Nakamura


2004 ◽  
Vol 409 (1) ◽  
pp. 293-299 ◽  
Author(s):  
J. F. Strömer ◽  
C. V. Brown ◽  
E. P. Raynes


2013 ◽  
Vol 9 (3) ◽  
pp. 162-169 ◽  
Author(s):  
Jong-Man Kim ◽  
Jongbin Kim ◽  
Youngmin Cho ◽  
Kwangjoon Kim ◽  
Seung-Woo Lee




1993 ◽  
Vol 50 (7) ◽  
pp. 551-555
Author(s):  
Katsuhiko RINDO ◽  
Akira YOSHIMATSU


2011 ◽  
Vol 181-182 ◽  
pp. 26-32
Author(s):  
Benjamin I. Outram ◽  
Steve J. Elston

The difference between e1 and e3 parameters for flexoelectric polarization, as originally defined byMeyer, is measured for nematic liquid crystal materials E7 and BL087 in Twisted Nematic (TN) cells with In-Plane Switching (IPS) electric fields using the crystal rotation method, which measures transmission as a function of angle of incidence. Values of e1 − e3 for E7 and BL087 are found to be 7.2±1.0 pCm−1 and 9.4±1.0 pCm−1 respectively.



1978 ◽  
Vol 14 (14) ◽  
pp. 430 ◽  
Author(s):  
C. Hilsum ◽  
R.J. Holden ◽  
E.P. Raynes


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