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Observation of a uniaxial ferroelectric smectic A phase
We report the observation of the smectic A(F), a liquid crystal phase of the ferroelectric nematic realm. The smectic A(F) is a phase of small polar, rod-shaped molecules that form two-dimensional fluid layers spaced by approximately the mean molecular length. The phase is uniaxial, with the molecul...
Autores principales: | , , , , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
National Academy of Sciences
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9704750/ https://www.ncbi.nlm.nih.gov/pubmed/36375062 http://dx.doi.org/10.1073/pnas.2210062119 |
Sumario: | We report the observation of the smectic A(F), a liquid crystal phase of the ferroelectric nematic realm. The smectic A(F) is a phase of small polar, rod-shaped molecules that form two-dimensional fluid layers spaced by approximately the mean molecular length. The phase is uniaxial, with the molecular director, the local average long-axis orientation, normal to the layer planes, and ferroelectric, with a spontaneous electric polarization parallel to the director. Polarization measurements indicate almost complete polar ordering of the ∼10 Debye longitudinal molecular dipoles, and hysteretic polarization reversal with a coercive field ∼2 × 10(5) V/m is observed. The SmA(F) phase appears upon cooling in two binary mixtures of partially fluorinated mesogens: 2N/DIO, exhibiting a nematic (N)–smectic Z(A) (SmZ(A))–ferroelectric nematic (N(F))–SmA(F) phase sequence, and 7N/DIO, exhibiting an N–SmZ(A)–SmA(F) phase sequence. The latter presents an opportunity to study a transition between two smectic phases having orthogonal systems of layers. |
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