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Updated: Jul 23, 2025

Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals
Published on: August 15, 2018
Three Distinct Polar Phases, Isotropic, Nematic, and Smectic-A Phases, Formed from a Fluoro-Substituted Dimeric
Shigemasa Nakasugi1,2, Sungmin Kang1,2, Tso-Fu Mark Chang2
1Advanced Technology Research Department, LG Japan Lab Inc., 1-2-13, Takashima, Nishi-ku, Yokohama, Kanagawa 220-0011, Japan.
Abstract:
A dimeric molecule, di-5(3FM-C4T), with fluoro-substituted mesogenic cores composed of three-aromatic rings and linked by a pentamethylene spacer is prepared. Di-5(3FM-C4T) forms the ferroelectric nematic (NF), ferroelectric smectic-A (SmAPF), and polar isotropic (IsoP) phases. The NF phase is composed of molecules in U-shaped conformation that behave like polar rod-like molecules. The reversal spontaneous polarization (Ps) is approximately 8 μC cm-2, which is extremely large and reflects the huge dipole moment (11.2 D) of the one-side mesogenic core. On the other hand, the SmAPF phase is formed by bent-shaped molecules. The NF-SmAPF phase transition thus follows the conformational change of molecules. The reversal Ps of the SmAPF phase is around 4 μC cm-2, which is half of that in the NF phase, and this is an expected value from the bent shape of the molecules. It is interesting that the highest temperature IsoP phase still exhibits the polar structure and possibly retains some polar aggregation of molecules in small domains. The three polar phases exhibit the dielectric mode due to the collective polarization fluctuation at around 100 Hz, giving the high dielectric constant over 8000.
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