2012
DOI: 10.1049/el.2012.1061
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Electrical characterisation of liquid crystals at millimetre wavelengths using frequency selective surfaces

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Cited by 43 publications
(38 citation statements)
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“…2 shows the solution of (5) for the structure in Fig.1 at different RMS voltages (at room temperature and 1 kHz AC-signal), assuming a separation of z = 75 µm, pretilt angles of 4º on both surfaces, and LC material type GT3-23001, which is manufactured by Merck for microwave applications. The LC characteristic data given by Merck is shown in the figure caption, and the RF parameters ( ⊥ ) and ( // ) have been measured by the authors in the band from 140 to 165 GHz [15]. As can be seen, the molecular tilt angle takes the value = 4º at the extremes, increasing its value with the separation until it reaches the maximum at the center of the LC layer.…”
Section: Static Modeling Of Liquid Crystals In the Nematic Phasementioning
confidence: 99%
See 1 more Smart Citation
“…2 shows the solution of (5) for the structure in Fig.1 at different RMS voltages (at room temperature and 1 kHz AC-signal), assuming a separation of z = 75 µm, pretilt angles of 4º on both surfaces, and LC material type GT3-23001, which is manufactured by Merck for microwave applications. The LC characteristic data given by Merck is shown in the figure caption, and the RF parameters ( ⊥ ) and ( // ) have been measured by the authors in the band from 140 to 165 GHz [15]. As can be seen, the molecular tilt angle takes the value = 4º at the extremes, increasing its value with the separation until it reaches the maximum at the center of the LC layer.…”
Section: Static Modeling Of Liquid Crystals In the Nematic Phasementioning
confidence: 99%
“…most important parameter at antenna level) would be around 20º, which can be used in most applications. However, if a very small phase error is required and the cell structure provides a relatively large effect due to the transversal inhomogeneity, this latter can be suppressed by depositing a thin conductive layer (ITO, PDOT) across the surface of the entire cell [15], similar as in LC Displays.…”
Section: Extraction Of Voltage Dependence Of Reflectarray Cellsmentioning
confidence: 99%
“…1, can be made identical over the entire surface. The LC used is the mixture GT3-23001, which is manufactured by Merck and whose parameters are: e r// (100 GHz)=3.25, e r ±(100 GHz)=2.47, tan5//(100 GHz)= 0.015, tan5±(100 GHz)= 0.02 (measured in [10]), and 8^/(1 KHz)=8.1, Ae (1 KHz)=4.6 (givenby Merck).…”
Section: A Design Of the Lc-based Reflectarray Structurementioning
confidence: 99%
“…The dielectric anisotropy at RF also has an influence on the accuracy of the method used. However, an FSS has previously been used to extract this parameter above 100 GHz [10], and since the LC does not present transversal inhomogeneity, the values obtained for Ae r (100 GHz) are considered to be sufficiently accurate. The uncertainty associated with the value of Ae r (0.33 Hz) can produce average phase errors after voltage synthesis, of around ±10°.…”
Section: Biasing and Voltage Synthesis For The Cellsmentioning
confidence: 99%
“…In order to reduce the possibility of breakage during processing, the thickness of the quartz substrate is chosen to be 250 μm and a metalized silicon wafer is used to form the ground plane. A thin (100 nm) resistive boron diffused polycrystaline silicon film [19] was deposited by a low pressure Chemical Vapour Deposition process at 620 o C on the un-patterned side of the quartz wafer to give an almost mmwave transparent but low frequency conductive layer. This layer is used for the establishment of a low frequency quasistatic electric field in the cavity to bias the liquid crystals; it has been experimentally determined that a low frequency field is best suitable for the biasing of the LC [13].…”
Section: A Design and Realizationmentioning
confidence: 99%