Parton-Barr Charles, Gleeson Helen F, Mandle Richard J
School of Physics and Astronomy, University of Leeds, Leeds, LS2 9JT, UK.
School of Chemistry, University of Leeds, Leeds, LS2 9JT, UK.
Soft Matter. 2024 Jan 17;20(3):672-680. doi: 10.1039/d3sm01282d.
The ferroelectric nematic phase (N) is a recently discovered phase of matter in which the orientational order of the conventional nematic liquid crystal state is augmented with polar order. Atomistic simulations suggest that the polar N phase would be denser than conventional nematics owing to contributions from polar order. Using an oscillating U-tube densitometer, we obtain detailed temperature-dependent density values for a selection of conventional liquid crystals with excellent agreement with earlier reports. Having demonstrated the validity of our method, we then record density as a function of temperature for M5, a novel room-temperature ferroelectric nematic material. We present the first experimental density data for a N material as well as density data for a nematic that has not previously been reported. We find that the room-temperature N material shows a large (>1.3 g cm) density at all temperatures studied, notably including phases without polar order. An increase in density at phase transitions is observed. The magnitude of the increase for the intermediate-to-ferroelectric nematic (N-N) transition is an order of magnitude smaller than the isotropic-nematic (I-N) transition. We then probe potential consequences that may result from an elevated density through measurement of the refractive indices ( and ). The of M5 is compared with 5CB and polar smectic liquid crystals. We observe how the highly polar nature of the system counteracts the effects of an increase in density. With knowledge of experimental density, we are able to derive an approximation that yields the polar order parameter, 〈1〉, from polarisation measurements. Present results may be typical of ferroelectric nematic materials, potentially guiding material development, and is especially relevant for informing ongoing studies into this emerging class of materials.
铁电向列相(N)是最近发现的一种物质相,其中传统向列液晶态的取向有序性因极性有序而增强。原子模拟表明,由于极性有序的贡献,极性N相比传统向列相密度更大。使用振荡U型管密度计,我们获得了一系列传统液晶随温度变化的详细密度值,与早期报告结果高度吻合。在证明了我们方法的有效性之后,我们接着记录了新型室温铁电向列材料M5的密度随温度的变化情况。我们给出了第一种N相材料的实验密度数据以及一种此前未报道过的向列相的密度数据。我们发现,室温下的N相材料在所有研究温度下都表现出较大的密度(>1.3 g/cm³),特别是在没有极性有序的相态中。在相变处观察到密度增加。中间相向铁电向列相(N-N)转变时密度增加的幅度比各向同性向列相(I-N)转变时小一个数量级。然后,我们通过测量折射率( 和 )来探究密度升高可能产生的潜在影响。将M5的 与5CB和极性近晶液晶进行了比较。我们观察到该系统的高极性如何抵消密度增加的影响。基于实验密度,我们能够推导出一个近似值,通过极化测量得出极性序参量〈1〉。目前的结果可能是铁电向列材料的典型特征,有望指导材料开发,尤其有助于为正在进行的这类新兴材料的研究提供参考。