Twist Grain Boundary Liquid-Crystalline Phases under the Effect of the Magnetic Field: A Complete2H and13C NMR Study

ChemPhysChem ◽  
2008 ◽  
Vol 9 (4) ◽  
pp. 556-566 ◽  
Author(s):  
Valentina Domenici ◽  
Carlo Alberto Veracini ◽  
Vladimira Novotná ◽  
Ronald Y. Dong
2001 ◽  
Vol 279 (11) ◽  
pp. 1144-1148
Author(s):  
A. Yoshino ◽  
M. Ishida ◽  
H. Yuki ◽  
H. Okabayashi ◽  
H. Masuda ◽  
...  

2019 ◽  
Vol 7 (34) ◽  
pp. 10530-10543 ◽  
Author(s):  
Susanta Chakraborty ◽  
Malay Kumar Das ◽  
Alexej Bubnov ◽  
Wolfgang Weissflog ◽  
Dorota Węgłowska ◽  
...  

Induction of TGB phases in binary mixtures of hockey stick-shaped and chiral ferroelectric liquid crystal compounds.


2021 ◽  
Vol 9 (6) ◽  
pp. 1895-1910
Author(s):  
Hale Ocak ◽  
Belkız Bilgin Eran ◽  
Sevgi Nuray ◽  
Aykun Özkonstanyan ◽  
Silvio Poppe ◽  
...  

A huge effect of a magnetic field on the layer spacing of smectic and polar smectic liquid crystalline phases of a diamagnetic bent-core mesogen is reported, which is opposite for the uniformly chiral compound and its racemic mixture.


2015 ◽  
Vol 51 (35) ◽  
pp. 7512-7515 ◽  
Author(s):  
Hale Ocak ◽  
Belkız Bilgin-Eran ◽  
Dilek Güzeller ◽  
Marko Prehm ◽  
Carsten Tschierske

Chiral 4-cyanoresorcinol derived bent-core molecules form liquid crystalline phases with helically deformed layers representing TGBA and TGBC-like structures.


2000 ◽  
Vol 55 (1-2) ◽  
pp. 298-300
Author(s):  
R. Blinc ◽  
A. Gregorovič ◽  
B. Zalar

The deuteron NMR lineshapes in the tilted antiferroeelectric smectic liquid crystalline phases are evaluated for: i) the case of a discrete short pitch modulation P1 = N • d where N = 2,3,4, ii) for a superposition of two modulations p1 and p0 where p0 ≫p1 as well as iii) for the case where in addition rapid molecular exchange between adjacent layers takes place due to translational diffusion. The results are compared with the experimental deuteron NMR spectra of α-CD2 deuterated MHPOBC in the Sm C*A phase measured at different angles between the magnetic field direction and the normals to the smectic layers. The alternating tilt structure of the Sm C*A phase is confirmed


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