Structure and properties of organic liquid crystals

Author(s):  
I.G. Voigt-Martin

Organic liquid crystals (LCs), both in the monomeric and polymeric state, are capable of self organisation because of the anisotropic shape of their molecules. By suitable molecular engineering it is thus possible to induce interesting physical properties like ferroelectricity, second harmonic generation (SHG) and photoconductivity. For a deeper understanding it is necessary to gain insight into the relationship between molecular characteristics (electronic charge distribution, dipole moments, hyperpolarisabilities, molecular conformation), structural relations (symmetry relations, space groups, defects) and the above physical propertiesFor structure analysis electron diffraction patterns from different crystallographic zones with many higher orders of diffraction are required. Unfortunately a characteristic feature of LCs is their loss of all higher order reflections and a change in symmetry. Furthermore, LCs give rise to specific defects, which give important information about the elastic energy density of the system. These can only be characterised by a phase contrast imaging method in which the small angle spatial frequencies are transferred by the electron microscope phase transfer function.

2017 ◽  
Vol 129 (32) ◽  
pp. 9674-9678
Author(s):  
Stijn van Cleuvenbergen ◽  
Przemysław Kędziora ◽  
Jean-Luc Fillaut ◽  
Thierry Verbiest ◽  
Koen Clays ◽  
...  

2017 ◽  
Vol 56 (32) ◽  
pp. 9546-9550 ◽  
Author(s):  
Stijn van Cleuvenbergen ◽  
Przemysław Kędziora ◽  
Jean-Luc Fillaut ◽  
Thierry Verbiest ◽  
Koen Clays ◽  
...  

1989 ◽  
Vol 175 ◽  
Author(s):  
Gregory J. Exarhos ◽  
William D. Samuels

AbstractPhysical properties intrinsic to linear inorganic polymer systems can be modified through replacement of chemical groups external to the chain backbone. This substitution also perturbs chemical bonding along the chain which can further influence polymer properties. Several phosphazene polymers deposited as thin dielectric films exhibit extended ultraviolet transmission. Second harmonic generation (SHG) has been observed in these polymers as well as in cyclic polymer precursors. The relative magnitude of SHG is found to correlate both with the nature of the substitutional group and molecular conformation. Influence of these parameters on substrate-film adhesion and measured optical properties is discussed in terms of substitutional group electronegativity, and electronic charge localization in the polymer chain which is probed using molecular spectroscopic techniques.


2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Jie Yin ◽  
Hongxiang Zong ◽  
Hong Tao ◽  
Xuefei Tao ◽  
Haijun Wu ◽  
...  

AbstractMultitudinous topological configurations spawn oases of many physical properties and phenomena in condensed-matter physics. Nano-sized ferroelectric bubble domains with various polar topologies (e.g., vortices, skyrmions) achieved in ferroelectric films present great potential for valuable physical properties. However, experimentally manipulating bubble domains has remained elusive especially in the bulk form. Here, in any bulk material, we achieve self-confined bubble domains with multiple polar topologies in bulk Bi0.5Na0.5TiO3 ferroelectrics, especially skyrmions, as validated by direct Z-contrast imaging. This phenomenon is driven by the interplay of bulk, elastic and electrostatic energies of coexisting modulated phases with strong and weak spontaneous polarizations. We demonstrate reversable and tip-voltage magnitude/time-dependent donut-like domain morphology evolution towards continuously and reversibly modulated high-density nonvolatile ferroelectric memories.


2004 ◽  
Vol 116 (28) ◽  
pp. 3763-3768 ◽  
Author(s):  
Naohiko Ikuma ◽  
Rui Tamura ◽  
Satoshi Shimono ◽  
Naoyuki Kawame ◽  
Osamu Tamada ◽  
...  

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 ◽  
...  

2017 ◽  
Vol 21 (07n08) ◽  
pp. 476-492 ◽  
Author(s):  
Toshiyuki Akabane ◽  
Kazuchika Ohta ◽  
Tokihiro Takizawa ◽  
Takehiro Matsuse ◽  
Mutsumi Kimura

The most difficult problem on syntheses of the phthalocyanine-based liquid crystals is the long reaction time. In order to shorten the reaction time, we have developed novel Methods A, B and D, for the syntheses of phthalocyanine-based liquid crystals by using microwave heating and/or adding a phase transfer catalysis of Aliquat 336. A series of phthalocyanine derivatives C[Formula: see text]PcZn(1) ([Formula: see text] 10, 12, 14, 16 and 18: a, b, c and e) could be successfully synthesized in a dramatically short reaction time of 30–60 min using Methods A and B by microwave heating. On the other hand, anothor series of the derivatives C[Formula: see text](OH)PcZn (2a–2e) could not be synthesized by microwave heating. Therefore, all these derivatives were synthesized using conventional Method C by oil bath heating, but the reaction took a very long time (22.5–88 h). To shorten the reaction time, we have developed Method D by oil bath heating with adding a phase transfer catalyst of Aliquat 336. In this method, we successfully shortened the reaction time from 88 h to 3 h for the synthesis of the derivative 2a. Thus, the reaction time for oil bath heating can be also greatly shortened by adding the phase transfer catalyst of Aliquat 336. Furthermore, we have established from POM, DSC and temperature-dependent X-ray diffraction measurements that the derivative C[Formula: see text]PcZn (1a) shows a very rare pseudohexagonal columnar (Col[Formula: see text] phase, and that the derivatives C[Formula: see text]PcZn (1b–1e) and C[Formula: see text](OH)PcZn (2b–2e) exhibit spontaneous perfect homeotropic alignment in a large area between two glass plates in their Col[Formula: see text] phases.


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