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Ferrielectricity in Chiral Smectic Cβ of an Antiferroelectric Liquid Crystal
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The switching current behavior and the complex dielectric constant under DC electric bias field and domain structures of
an antiferroelectric liquid crystal, 4-(1-methylheptyloxycarbonyl) phenyl 4'-octyloxybiphenyl-4-carboxylate (MHPOBC), were
investigated as a function of optical purity and cell thickness, and the ferrielectricity of the chiral smectic C
β
phase (SmC
β
*) was discussed. Optically pure samples show two-step decrease in the real part of complex dielectric constant with increasing DC bias field. The first decrease corresponds to the suppression of the ferroelectric Goldstone mode, which is also suppressed by decreasing cell thickness. The second step, which is observed even in the chiral smectic C
α
phase (SmC
α
*), corresponds to the suppression of a new relaxation mode induced by DC electric bias field. Three peaks of the switching current were observed in SmC
β
* and also in the lower-temperature region of SmC
α
*. Temperature dependence curves of the peak positions
are continuously connected together at the phase transition temperature between SmC
β
* and SmC
α
*. It can be said that the antiferroelectricity of SmC
α
* is conserved in SmC
β
*, and that the ferrielectricity of SmC
β
* may consist of the ferroelectricity
of SmC* and the antiferroelectricity of SmC
α
*. Striped domains observed in SmC
β
* after removing the DC electric bias field can be considered to be the SmC
α
* phase.
Title: Ferrielectricity in Chiral Smectic Cβ of an Antiferroelectric Liquid Crystal
Description:
The switching current behavior and the complex dielectric constant under DC electric bias field and domain structures of
an antiferroelectric liquid crystal, 4-(1-methylheptyloxycarbonyl) phenyl 4'-octyloxybiphenyl-4-carboxylate (MHPOBC), were
investigated as a function of optical purity and cell thickness, and the ferrielectricity of the chiral smectic C
β
phase (SmC
β
*) was discussed.
Optically pure samples show two-step decrease in the real part of complex dielectric constant with increasing DC bias field.
The first decrease corresponds to the suppression of the ferroelectric Goldstone mode, which is also suppressed by decreasing cell thickness.
The second step, which is observed even in the chiral smectic C
α
phase (SmC
α
*), corresponds to the suppression of a new relaxation mode induced by DC electric bias field.
Three peaks of the switching current were observed in SmC
β
* and also in the lower-temperature region of SmC
α
*.
Temperature dependence curves of the peak positions
are continuously connected together at the phase transition temperature between SmC
β
* and SmC
α
*.
It can be said that the antiferroelectricity of SmC
α
* is conserved in SmC
β
*, and that the ferrielectricity of SmC
β
* may consist of the ferroelectricity
of SmC* and the antiferroelectricity of SmC
α
*.
Striped domains observed in SmC
β
* after removing the DC electric bias field can be considered to be the SmC
α
* phase.
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