A Fluid Liquid‐Crystal Material with Highly Polar Order

Hiroya Nishikawa(Kyushu University), Kazuya Shiroshita(Kyushu University), Hiroki Higuchi(Kyushu University), Yasushi Okumura(Kyushu University), Yasuhiro Haseba(JNC (Japan)), Shin‐ichi Yamamoto(JNC (Japan)), Koki Sago(JNC (Japan)), Hirotsugu Kikuchi(Kyushu University)
Advanced Materials
October 10, 2017
Cited by 364

Abstract

Abstract An anomalously large dielectric permittivity of ≈10 4 is found in the mesophase temperature range (MP phase) wherein high fluidity is observed for a liquid‐crystal compound having a 1,3‐dioxane unit in the mesogenic core (DIO). In this temperature range, no sharp X‐ray diffraction peak is observed at both small and wide Bragg angles, similar to that for a nematic phase; however, an inhomogeneous sandy texture or broken Schlieren one is observed via polarizing optical microscopy, unlike that for a conventional nematic phase. DIO exhibits polarization switching with a large polarization value, i.e., P = 4.4 µC cm −2 , and a parallelogram‐shaped polarization–electric field hysteresis loop in the MP phase. The inhomogeneously aligned DIO in the absence of an electric field adopts a uniform orientation along an applied electric field when field‐induced polarization switching occurs. Furthermore, sufficiently larger second‐harmonic generation is observed for DIO in the MP phase. Second‐harmonic‐generation interferometry clearly shows that the sense of polarization is inverted when the +/− sign of the applied electric field in MP is reversed. These results suggest that a unidirectional, ferroelectric‐like parallel polar arrangement of the molecules is generated along the director in the MP phase.


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