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Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals
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Molecular model for nematic, smectic-A, and smectic-C liquid crystals.
Mário J de Oliveira1, Dora Izzo2
1Instituto de Física, Universidade de São Paulo, Rua do Matão, 1371, 05508-090 São Paulo, São Paulo, Brazil.
Physical Review. E
|December 17, 2020
Summary
This study introduces a molecular model for liquid crystal phase transitions, detailing isotropic, nematic, smectic-A, and smectic-C phases. It reveals continuous transitions between smectic-C and nematic phases, with a non-zero tilt angle.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Physical Chemistry
Background:
- Liquid crystals exhibit diverse mesophases, including isotropic, nematic, smectic-A, and smectic-C.
- Understanding the molecular interactions governing phase transitions is crucial for materials design.
- Existing models like the McMillan model provide a basis for analyzing these transitions.
Purpose of the Study:
- To develop and analyze a molecular model for liquid crystal phase transitions.
- To describe the isotropic, nematic, smectic-A, and smectic-C phases and their interconversions.
- To investigate the role of molecular shape and interactions in determining phase behavior.
Main Methods:
- Analysis of a molecular model incorporating a pair potential with cylindrical symmetry.
- Inclusion of a biquadratic pair potential to favor molecular tilt within smectic layers.
- Comparison of the model's phase diagram with the McMillan molecular model.
Main Results:
- The model successfully describes phase transitions between isotropic, nematic, smectic-A, and smectic-C phases.
- The phase diagram for the first three phases resembles that of the McMillan model.
- A continuous phase transition line separates the smectic-C and nematic phases, characterized by a non-zero tilt angle.
Conclusions:
- The proposed molecular model accurately captures key liquid crystal phase behaviors.
- The biquadratic potential effectively models the molecular tilt in smectic phases.
- The tilt angle continuously vanishes at the smectic-C to smectic-A phase transition line.
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