Nakasugi Shigemasa, Kang Sungmin, Chang Tso-Fu Mark, Ishizaki Hiroki, Sone Masato, Watanabe Junji
Advanced Technology Research Department, LG Japan Lab Inc., 1-2-13, Takashima, Nishi-ku, Yokohama, Kanagawa 220-0011, Japan.
Institute of Innovative Research, Tokyo Institute of Technology, 4259, Nagatsuta-cho, Midori-ku, Yokohama, Kanagawa 226-8503, Japan.
J Phys Chem B. 2022 Jul 7;126(26):4967-4976. doi: 10.1021/acs.jpcb.2c01938. Epub 2022 Jun 24.
This study reports the electric switching behaviors and dielectric properties of the ferroelectric smectic-A (SmAP), anti-ferroelectric smectic-A (SmAP), anti-ferroelectric SmCP, and smectic-A (SmA) phases formed by mixing the bent-shaped dimeric molecules, α,ω-bis(4-alkoxyanilinebenzylidene-4'-carbonyloxy)pentanes. These four phases each show characteristic features. The SmAP shows a low threshold electric field for ferroelectric switching and a large dielectric strength due to the collective fluctuation mode of dipoles at around 500 Hz. Both the threshold electric field and dielectric strength are strongly dependent on the cell thickness. The threshold field decreases to 0.1 V μm, and the dielectric strength increases up to a huge value of 10,000 as the cell thickness increases up to 80 μm. The SmAP also shows a similar collective mode at around 2 kHz with a relatively small dielectric strength (around 200), which may be induced by the anti-phase rotation of dipoles in adjacent layers. In these collective modes, the dielectric strength is found to be inversely proportional to the switching threshold field. On the other hand, another anti-ferroelectric SmCP as well as the paraelectric SmA show only the non-collective mode (i.e., rotational relaxation of individual molecules around their short axes) at a high frequency of around 100 kHz.
本研究报告了通过混合弯曲形二聚体分子α,ω-双(4-烷氧基苯胺亚苄基-4'-羰基氧基)戊烷形成的铁电近晶-A(SmAP)、反铁电近晶-A(SmAP)、反铁电SmCP和近晶-A(SmA)相的电开关行为和介电性能。这四个相各自呈现出特征特性。SmAP由于在500 Hz左右偶极子的集体涨落模式,表现出低的铁电开关阈值电场和大的介电强度。阈值电场和介电强度都强烈依赖于盒厚。随着盒厚增加到80μm,阈值场降至0.1 V/μm,介电强度增加到高达10000的巨大值。SmAP在2 kHz左右也呈现出类似的集体模式,介电强度相对较小(约200),这可能是由相邻层中偶极子的反相旋转引起的。在这些集体模式中,发现介电强度与开关阈值场成反比。另一方面,另一种反铁电SmCP以及顺电SmA在约100 kHz的高频下仅呈现非集体模式(即单个分子围绕其短轴的旋转弛豫)。