Physical properties of nematic phenylcyclohexanes, a new class of low melting liquid crystals with positive dielectric anisotropy

1977 ◽  
Vol 60 (5) ◽  
pp. 421-423 ◽  
Author(s):  
L. Pohl ◽  
R. Eidenschink ◽  
G. Krause ◽  
D. Erdmann
1985 ◽  
Vol 40 (9) ◽  
pp. 932-943 ◽  
Author(s):  
Hp. Schad ◽  
S. M. Kelly

Abstract We have measured the physical properties of three homologues of a new class of polar nematic liquid crystals having no molecular association. On the basis of mean field and continuum theories an analysis of the physical properties has been performed. The advantageous application of this class of compounds (substituted aromatic ketones) in liquid crystal displays - especially in the highly multiplexed twisted nematic display - is outlined and an example of a simple practical mixture is given.


Molecules ◽  
2021 ◽  
Vol 26 (10) ◽  
pp. 2873
Author(s):  
Ana Barrera ◽  
Corinne Binet ◽  
Frédéric Dubois ◽  
Pierre-Alexandre Hébert ◽  
Philippe Supiot ◽  
...  

In the present work, the dielectric properties of recycled liquid crystals (LCs) (non-purified, purified, and doped with diamond nanoparticles at 0.05, 0.1, and 0.2 wt%) were investigated. The studied LC mixtures were obtained from industrial recycling of end-of-life LC displays presenting mainly nematic phases. Dielectric measurements were carried out at room temperature on a frequency range from 0.1 to 106 Hz using an impedance analyzer. The amplitude of the oscillating voltage was fixed at 1 V using cells with homogeneous and homeotropic alignments. Results show that the dielectric anisotropy of all purified samples presents positive values and decreases after the addition of diamond nanoparticles to the LC mixtures. DC conductivity values were obtained by applying the universal law of dielectric response proposed by Jonscher. In addition, conductivity of the doped LC mixtures is lower than that of the undoped and non-purified LC.


Langmuir ◽  
2017 ◽  
Vol 33 (48) ◽  
pp. 13849-13860 ◽  
Author(s):  
Joydip De ◽  
Santosh Prasad Gupta ◽  
Indu Bala ◽  
Sandeep Kumar ◽  
Santanu Kumar Pal

2005 ◽  
Vol 82 (9) ◽  
pp. 1349 ◽  
Author(s):  
Gerald R. Van Hecke ◽  
Kerry K. Karukstis ◽  
Hanhan Li ◽  
Hansford C. Hendargo ◽  
Andrew J. Cosand ◽  
...  

1993 ◽  
Vol 148 (1) ◽  
pp. 213-222 ◽  
Author(s):  
Kayoko Ueda ◽  
Chizu Sekine ◽  
Takeshi Tani ◽  
Koichi Fujisawa ◽  
Takayuki Higashii ◽  
...  

2018 ◽  
Vol 157 ◽  
pp. 109-116 ◽  
Author(s):  
Elias Regis ◽  
Leonardo de O. Aguiar ◽  
Patricia Tuzimoto ◽  
Edivandro Girotto ◽  
Tiago E. Frizon ◽  
...  

2018 ◽  
Vol 9 ◽  
pp. 1544-1549 ◽  
Author(s):  
Margarita A Kurochkina ◽  
Elena A Konshina ◽  
Daria Khmelevskaia

We have experimentally investigated the effect of the reorientation of a nematic liquid crystal (LC) in an electric field on the photoluminescence (PL) of CdSe/ZnS semiconductor quantum dots (QDs). To the LC with positive dielectric anisotropy, 1 wt % QDs with a core diameter of 5 nm was added. We compared the change of PL intensity and decay times of QDs in LC cells with initially planar or vertically orientated molecules, i.e., in active or passive LC matrices. The PL intensity of the QDs increases four-fold in the active LC matrix and only 1.6-fold in the passive LC matrix without reorientation of the LC molecules. With increasing electric field strength, the quenching of QDs luminescence occurred in the active LC matrix, while the PL intensity did not change in the passive LC matrix. The change in the decay time with increasing electric field strength was similar to the behavior of the PL intensity. The observed buildup in the QDs luminescence can be associated with the transfer of energy from LC molecules to QDs. In a confocal microscope, we observed the increase of particle size and the redistribution of particles in the active LC matrix with the change of the electric field strength. At the same time, no significant changes occurred in the passive LC matrix. With the reorientation of LC molecules from the planar in vertical position in the LC active matrix, quenching of QD luminescence and an increase of the ion current took place simultaneously. The obtained results are interesting for controlling the PL intensity of semiconductor QDs in liquid crystals by the application of electric fields.


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