Ueda Hiroki, Akita Takuya, Uchida Yoshiaki, Kimura Tsuyoshi
Division of Materials Physics, Graduate School of Engineering Science, Osaka University;
Division of Chemical Engineering, Graduate School of Engineering Science, Osaka University.
J Vis Exp. 2018 Aug 15(138):58018. doi: 10.3791/58018.
Materials showing coupling phenomena between magnetism and (ferro)electricity, i.e., magnetoelectric effects, have attracted a great deal of attention due to their potential applications for future device technologies such as sensors and storage. However, conventional approaches, which usually utilize materials containing magnetic metal ions (or radicals), have a major problem: only a few materials have been found to show the coupling phenomena at room temperature. Recently, we proposed a new approach to achieve room-temperature magnetoelectrics. In contrast to conventional approaches, our alternative proposal focuses on a completely different material, a "liquid crystal", free from magnetic metal ions. In such liquid crystals, a magnetic field can be utilized to control the orientational state of constituent molecules and the corresponding electric polarization through magnetic anisotropy of the molecules; it is an unprecedented mechanism of the magnetoelectric effect. In this context, this paper provides a protocol to measure ferroelectric properties induced by a magnetic field, that is, the direct magnetoelectric effect, in a liquid crystal. With the method detailed here, we successfully detected magnetically-tuned electric polarization in the chiral smectic C phase of a liquid crystal at room temperature. Taken together with the flexibility of constituent molecules, which directly affects the magnetoelectric responses, the introduced method will serve to allow liquid crystal cells to acquire more functions as room-temperature magnetoelectrics and associated optical materials.
表现出磁与(铁)电之间耦合现象,即磁电效应的材料,因其在诸如传感器和存储等未来器件技术中的潜在应用而备受关注。然而,传统方法通常使用含有磁性金属离子(或自由基)的材料,存在一个主要问题:只有少数材料在室温下表现出耦合现象。最近,我们提出了一种实现室温磁电材料的新方法。与传统方法不同,我们的替代方案聚焦于一种完全不同的材料——不含磁性金属离子的“液晶”。在这种液晶中,磁场可通过分子的磁各向异性来控制组成分子的取向状态以及相应的电极化;这是一种前所未有的磁电效应机制。在此背景下,本文提供了一种测量液晶中由磁场诱导的铁电性质,即直接磁电效应的方法。利用此处详述的方法,我们成功在室温下检测到了液晶手性近晶C相中的磁调谐电极化。结合直接影响磁电响应的组成分子的灵活性,所引入的方法将有助于使液晶单元作为室温磁电材料及相关光学材料获得更多功能。