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The optimal reflection angle was determined by means of optical simulation.
Furthermore, via adjusting the thickness to only 1.65 mm, the optimal reflection loss can obtain −51.2 dB at 13.92 GHz with a broad bandwidth of 4.4 GHz.
The nanocomposites obtained from 4.3 wt% PVP exhibited excellent EM performance, their optimal reflection loss (RL, in dB unit) value reached as high as −57.8 dB at a coating thickness of 1.9 mm.
The optimal reflection loss (RL) value reaches −57.9 dB when the matching thickness is 2.9 mm at 6.9 GHz and the effective absorption bandwidth (RL < −10 dB) is 2.7 GHz (6.1 8.9 GHz).
An optimal reflection loss of −41.1 dB is reached at 8.2 GHz with a matching thickness of 2.2 mm, the bandwidth with a reflection loss less than −10 dB is obtained in the 5.5 11.3 GHz range for absorber thicknesses of 1.5 2.5 mm.
The optimal reflection loss (RL) of Fe@C@BaTiO3-parrafin composites are −40.2 dB at 8.14 GHz with a thickness of 2.24 mm and the absorption bandwidth of those below −10 dB is 8.4 GHz with only absorbent thicknesses of 1.7 2.0 mm.
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Optimal low reflection of the microwave radiation was achieved using the three-stub tuner.
The sample prepared in optimal conditions indicated reflection loss of −15 dB corresponding to 97% absorption, at the range of 9.2 10.8 GHz.
The sample prepared in optimal conditions had reflection loss of less than −10 dB (absorption >90%) and covering a frequency range of 8.4 11.6 GHz.
Considering rotations as well as reflection, the optimal rotation matrix can then be expressed as R= VS{U}^T.
However, the Delphi method is optimal because the reasoned reflection process improves the options for reaching some sort of consensus on the value system.
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