微波应用液晶材料介电特性的测量

Juan R. Sánchez, V. Nova, C. Bachiller, B. Villacampa, Alberto de la Rua, R. Kronberger, Felipe L. Peñaranda, V. Boria
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引用次数: 1

摘要

液晶(LC)是一种各向异性的液体材料,它像液体一样流动,但同时它的分子又像固体一样具有取向秩序[1]。因此,LC是一种很有前途的介质材料,可用于设计微波频率下的可重构器件。为了优化可重构微波器件的设计,需要精确测量lc的介电常数和损耗正切值。然而,由于其最近用于微波应用,新的lc在这些频率上没有很好地表征。因此,在微波元件和器件的实际应用中,需要在该频率范围内进行表征[2]。在这项工作中,劈裂圆柱谐振器方法已被用于表征两个频率点,即5和11 GHz的lc。该方法是通过测量LC分子两种状态的共振频率和品质因子来提取复介电常数[3]。为了达到这两种状态,不需要电场或磁场,只是电池必须在腔内旋转90º。测定了默克公司的GT3-23002和青岛QYPD193、QYPD142、QYPD036四种不同LC样品的介电性能(介电常数和损耗正切)。QYPD036和QYPD193样品的介电各向异性最高,相应的损耗正切参数也最高。此外,我们还观察到,在较高的频率下,所有lc的损耗正切减小,介质各向异性增加,这在可重构微波器件的开发中必须考虑到。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
MEASUREMENT OF THE DIELECTRIC PROPERTIES OF LIQUID CRYSTAL MATERIAL FOR MICROWAVE APPLICATIONS
Liquid Crystal (LC) is an anisotropic liquid material which flows like a liquid, but at the same time its molecules have an orientational order like in the solid state [1]. Thus, LC is a promising dielectric material for designing reconfigurable devices at microwave frequencies. In order to optimize the design of reconfigurable microwave devices, accurate values of the dielectric permittivity and the loss tangent of LCs are needed. However, new LCs are not well characterized at these frequencies because of its recent use for microwave applications. Therefore, the characterization in this frequency range is required for its practical use within microwave components and devices [2].   In this work, the split-cylinder resonator method has been used for the characterization of LCs at two frequency points, i.e. 5 and 11 GHz. The method is based on the measurement of the resonance frequency and quality factor of the two states of the LC molecules for extracting the complex dielectric permittivity [3].   For achieving these two states, no electric or magnetic fields are needed, just the cell must be turned 90º inside the cavity. The dielectric properties (permittivity and loss tangent) of four different LC samples, GT3-23002 from Merck and QYPD193, QYPD142, and QYPD036 from Qingdao QY Liquid Crystal Co, have been obtained. The highest values of the dielectric anisotropy are presented for the samples QYPD036 and QYPD193, together with the highest values of the corresponding loss tangent parameters. Furthermore, it is observed for all the LCs that the loss tangent decreases and the dielectric anisotropy increases at higher frequencies, which must be taken into account in the development of reconfigurable microwave devices.
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