Nacke Pierre, Manabe Atsutaka, Klasen-Memmer Melanie, Chen Xi, Martinez Vikina, Freychet Guillaume, Zhernenkov Mikhail, Maclennan Joseph E, Clark Noel A, Bremer Matthias, Giesselmann Frank
Institute of Physical Chemistry, University of Stuttgart, Pfaffenwaldring 55, 70569, Stuttgart, Germany.
Display Solutions, Merck Electronics KGaA, 64293, Darmstadt, Germany.
Sci Rep. 2024 Feb 23;14(1):4473. doi: 10.1038/s41598-024-54832-0.
We present a new ferroelectric nematic material, 4-((4'-((trans)-5-ethyloxan-2-yl)-2',3,5,6'-tetrafluoro-[1,1'-biphenyl]-4-yl)difluoromethoxy)-2,6-difluorobenzonitrile (AUUQU-2-N) and its higher homologues, the molecular structures of which include fluorinated building blocks, an oxane ring, and a terminal cyano group, all contributing to a large molecular dipole moment of about 12.5 D. We observed that AUUQU-2-N has three distinct liquid crystal phases, two of which were found to be polar phases with a spontaneous electric polarization P of up to 6 µC cm. The highest temperature phase is a common enantiotropic nematic (N) exhibiting only field-induced polarization. The lowest-temperature, monotropic phase proved to be a new example of the ferroelectric nematic phase (N), evidenced by a single-peak polarization reversal current response, a giant imaginary dielectric permittivity on the order of 10, and the absence of any smectic layer X-ray diffraction peaks. The ordinary nematic phase N and the ferroelectric nematic phase N are separated by an antiferroelectric liquid crystal phase which has low permittivity and a polarization reversal current exhibiting a characteristic double-peak response. In the polarizing light microscope, this antiferroelectric phase shows characteristic zig-zag defects, evidence of a layered structure. These observations suggest that this is another example of the recently discovered smectic Z (SmZ) phase, having smectic layers with the molecular director parallel to the layer planes. The diffraction peaks from the smectic layering have not been observed to date but detailed 2D X-ray studies indicate the presence of additional short-range structures including smectic C-type correlations in all three phases-N, SmZ and N-which may shed new light on the understanding of polar and antipolar order in these phases.
我们展示了一种新型铁电向列相材料,4-((4'-((反式)-5-乙基氧杂环庚烷-2-基)-2',3,5,6'-四氟-[1,1'-联苯]-4-基)二氟甲氧基)-2,6-二氟苯腈(AUUQU-2-N)及其高级同系物,其分子结构包括氟化结构单元、一个氧杂环和一个末端氰基,所有这些都有助于产生约12.5 D的大的分子偶极矩。我们观察到AUUQU-2-N有三个不同的液晶相,其中两个被发现是极性相,自发极化P高达6 μC/cm。最高温度相是一个常见的互变向列相(N),仅表现出场致极化。最低温度的单向性相被证明是铁电向列相(N)的一个新例子,这由单峰极化反转电流响应、约10量级的巨大虚部介电常数以及不存在任何近晶层X射线衍射峰所证明。普通向列相N和铁电向列相N被一个反铁电液晶相分隔开,该反铁电液晶相具有低介电常数和呈现特征双峰响应的极化反转电流。在偏光显微镜下,这个反铁电相显示出特征性的之字形缺陷,这是层状结构的证据。这些观察结果表明,这是最近发现的近晶Z(SmZ)相的另一个例子,具有分子指向矢平行于层平面的近晶层。迄今为止尚未观察到近晶层的衍射峰,但详细的二维X射线研究表明,在所有三个相——N、SmZ和N中都存在包括近晶C型关联在内的额外短程结构,这可能为理解这些相中的极性和反极性有序提供新的线索。